Archive... · TheissueoftheInformationcontainedinthispublicationdoesnotimplyanyauthority...
Transcript of Archive... · TheissueoftheInformationcontainedinthispublicationdoesnotimplyanyauthority...
00oo
00
Milliard technical handbook
32
o gBook one
E
1
Semiconductor devices2<D CD
S3o3Q.
| Part eightMicrowave semiconductors andcomponents
£
c3
CO
CO
<3June 1979 Qf
MOI7CCVII
MICROWAVE SEMICONDUCTORSAND COMPONENTS
CONTENTS
MIXER AND DETECTOR DIODES
SELECTION GUIDE (see coloured pages) fc
GENERAL SECTION A =
GUNN, IMPATT AND NOISE DIODES B
BACKWARD DIODES D =
VARACTOR DIODES (Multiplier, specialpurpose and tuning types) E |
GUNN OSCILLATORS F |
DOPPLER AND TRAFFIC RADARS G |
MISCELLANEOUS H =
ISOLATORS AND CIRCULATORS J |
INDEX >
The issue of the Information contained in this publication does not imply any authority
or licence for the utilisation of any patented feature.
'Milliard' is the trademark of Mullard Limited and is registered in most of the principal
countries of the world,
Mullard Limited 1979
Book 1 comprises the following parts-
Part 1 A Small-signal transistors
Part 1
B
Low -frequency power transistors
Part 2 R,F. power devices
Part 3 Diodes
Part 4 Power diodes
Part 5 Thyristors, trlacs
Part 6 LOCMOS digital integrated circuits
Part 7A Consumer integrated circuits
Part 7B Professional analogue integrated circuits
Part 8 Microwave semiconductors and components
Part 9 Opto -electronic devices {to be issued later)
PLUS—
Signetics Technical Handbooks
Memories
Microprocessors
Analogue
Logic
Printed by Unwin Brothers Limited
The Gresham Press, Old WoHing, Surrey
A member of the Staples Printing Group
r? BOOK 1 (Part 8)
SEMICONDUCTOR DEVICESMicrowave semiconductorsMicrowave components
Milliard manufacture and market electronic componentsunder the Mullard, Philips and Signetics brands.
MULLARD LTD,, MULLARD HOUSE, TORRINGTON PLACE,LONDON, WC1E 7HD
Telephone 01-580 6633 Telex: 264341
DATA HANDBOOK SYSTEM
The Mullard data handbook system is made up of three sets of books, each comprising
several parts, plus the Signetics technical handbooks.
The three sets of books, easily identifiable by the colours on their covers, are as follows:
Book t (blue) Semiconductor devices and
integrated circuits
Book 2 (orange) Valves and tubes
Book 3 (green) Passive components, materials, and
assemblies.
Each part is completely reviewed annually ; revised and reprinted where necessary. Revisions
to previous data sheets are indicated by an arrow in the margin.
The data sheets contained in these books are as accurate and up to date as it is reasonably
possible to make them at the time of going to press. It must, however, be understood that no
guarantee can be given here regarding the availability of the various devices or that their
specifications may not be changed before the next edition is published.
The devices for which full data is given in these books are those around which we would
recommend equipment to be designed. Where appropriate, other types no longer recom-
mended for new equipment designs, but generally available for equipment production are
listed separately with abridged data. Data sheets for these types may be obtained on
request. Older devices for which data may still be obtained on request are also included in
the index of the appropriate part of each book.
Requests for information regarding the data handbook system (including Signetics data)
and for individual data sheets should be made to the
Technical Publications Department
Mullard Limited
New Road
Mitcham
Surrey CR4 4XY
Telex: 22194
Information regarding price and availability of devices must be obtained from our
authorized agents or from our representatives.
SELECTION GUIDE
SECTION B - GUNN, IMPATT AND NOISE DIODES
Gunn Effect Devices
poutmin.
(mW)
Type No. Description Operating
Voltage
(V)
rtot
max.
<W)
5
10
15
100
200
300
50
CXY11ACXY11BCXY11C
CXY19CXY19ACXY19BCXY21
Gallium arsenide bulk effect
devices employing the Gunneffect to produce c.w. oscilla-
tions in X-band
7.0
7.0
7.0
8 to 1
5
8 to 15
8 to 15
8,0
1.0
1.0
1.0
6.0
6.0
7.5
25
5
10
15
CXY14ACXY14BCXY14C
Gallium arsenide bulk effect
devices employing the Gunneffect to produce c,w, oscilla-
tions in J-band
7.0
7.0
7.0
1.0
1.0
1.0
25
50
CXY24ACXY24B
Gallium arsenide bulk effect
devices employing the Gunneffect to produce c.w. oscilla-
tions inQ-band (Ka-band)
3.5
3.5
4.0
4,0
Impatt Diodes
p"out Type No. Description Operating Frequency
mm. Vol tage Range(mW) (V) (GHz)
500 BXY50 High efficiency silicon Impatt 91 8 to 10
400 BXY51 diodes for the generation of 80 10 to 12
300 BXY52 microwave c.w. power 70 12 to 14650 BXY60 120 6 to 8
Noise Diode
Frequency
Range
Type No. Description Typ. Excess
Noise
Ratio
(dB)
Typ,
Avalanche
Voltage
IV)
10 Hz to
18 GHzBAT31 Broadband noise generator 34 20
SECTION C - MIXER AND DETECTOR DIODES
Schottky Barrier Mixer Diodes
Max.
Operating
Frequency
(GHz!
Type No. Description
I.F.
Impedance
(n)
Max.
Noise
Figure
(dB)
12 BAT 10 Plastic package 250-500 7.5
12 BAT 11 Li.O. 280-3 SO 7.0
12BAT50BAT50R*
Rimmed coaxial 300-500 6.8
12BAV22BAV22R*
Rimmed coaxial 300—550 7.5
12
BAV9GABAV96BBAV9GCBAV96D
M.Q.M, 250-450
7.5
7.0
6.5
ao
12
BAW95DBAW95EBAW95FBAW95G
Reversible cartridge 250-500
8.2
7.5
7.0
6.5
18BAT39BAT39A Mixer pW 250-450
6.5
7.5
18BAT 51
BAT51R*Rimless coaxial 220-320 7.5
18BAT52BAT52R*
Rimless coaxial 220-320 8.5
40 BAT38 Mixer pill 700-1100 10
40 BAT59 Mixer pill 700-1400 10
40 BAV72 M.Q.M. 850-1300 10
'Reverse polarity version.
SECTION C (cant.)
Schottky Barrier Detector Diodes
Frequency
Range(GHz)
Type No. Description Typ.
1 /f noise
(dB)
Typ.
Tangential
Sensitivity
(dBm)
8 to 12 BAV46 Reversible cartridge 10 -55
8 to 1 2 BAV75 Pill 10 -50
8 to 12 BAV97 M.Q.M. 10 -54
Schottky Barrier Diode for Intruder Alarm Applications
Frequency
Range(GHz)
Type No. Description Typ.
1/f noise
(jiV)
Typ.
Voltage output
for -90 dBminput
8 to 12 BAV46 Reversible cartridge 1.0* 40
*1 Hz to 1 kHz from carrier
SECTION D - BACKWARD DIODES
Backward Detector Diodes
Frequency
Range
(GHz)
Type No. Description Figure
of merit
(Ml
Typ.
Tangential
Sensitivity
(dBm)
1 to 18 AEY17 Mixer Mil >120 -53
12 to 18AEY29AEY29R*» Rimless coaxial >50 -53
! to 18 AEY31 M.Q.M. >120 -53
1 to 18 AEY31A M.Q.M. >50 -50
18 to 40 AEY3Z M.Q.M. >50 2.0 ^A/fiWt
** Reverse polarity version
tZero bias current sensitivity (typ
J
SECTION E - VARACTOR DIODES
Multiplier Varactor Diodes
Ca;
min,
^acitance
max.atVR
(V)
Type No. Description vRmax.
IV)
Typ.
Cut-off
Frequency
(GH?)
0,25
0.4
0.5
0.9
6
6
BXY41
BXY40
Silicon planar step recovery 25*
25*
200*
180*
0,5 1.0 6 BXY32 Silicon planar epitaxial step
recovery. For high order
frequency multiplier outputs
in X-band
20 150
0.6
0.8
1.0
1.5
6
6
1N5157
BXV29
Silicon planar epitaxial step
recovery. For frequency
multiplier outputs in X-band
20
25
200
120
o.a 1.2 6 BXY39 Silicon planar step recovery 40* 150*
1.0
1.0
2.5
3.0
6
6
BXY28
1N5155
Silicon planar epitaxial step
recovery. For frequency
multiplier outputs in C-band
45
35
120
120_—„
1.2 2.0 6 BXY38 Silicon planar step recovery 50* 120*
1.5
2.5
2.5
3.5
6
6
BXY56
BXV57
High efficiency silicon types
for multipliers with output
frequencies in C and X-bands
60
60
160*
140*
2.0 4.0 6 BXY37 Silicon planar step recovery 70* 100*
3.0 6.0 6 BXY27 Silicon planar epitaxial step
recovery. For frequency
multiplier outputs in S-band
55 100
4.0 6.0 6 BXY35 Silicon planar step recovery 70* 75*
5.0 7.5 6
1N5152
1N5153
Silicon planar epitaxial step
recovery. For frequency
multiplier outputs in S-band75 100
6.0 12 6 BXY35 Silicon planar step recovery 100* 25*
28 39 6 BAY96 Silicon planar epitaxial. For
high efficiency frequency
multipliers
120 25
SECTION E (cant.)
Special Purpose Varador Diodes
Capacitance
min. max.
(pF)
atVR
(V)
Type No. Description VRmax.
(V)
Typ.
Cut-off
Frequency
(GHz)
0.2 typ- CXY10 Gallium arsenide. For parametric
amplifiers, frequency multipliers
and switches
6 350
0,25 typ. 6 CXY12 Gallium arsenide. For frequency
multiplier circuits up to G-band
output frequency
10 500
03 0.5 CAY ID Gallium arsenide diffused mesa
type, For parametric amplifiers,
frequency multipliers and switches
G 240
—
Frequency
Range
(GHz)
Type No. Description Typ.
An.
(dB)
Typ.
Insertion
Loss
<dB)
2 to 7
7 to 12
CXY22ACXY22B Gallium arsenide limiter diodes
20
16
0.2
0.3
Tuning Varactor Diodes
Capacitance atV R Type No, Description V Rmin. max. max.
(pF> (V) {V)
0.8 1.2 4 BXY53 60
3.7 5.7 4 BXY54 Silicon planar epitaxial tuning devices 60
12 18 4 BXYB5 60
0.8 1.2 CXY23A 12
1.2 1.8 CXY23B Gallium arsenide Schottky barrier tuning 12
1.6 2.5 CXY23C devices 12
25 3.5 CXY23D 12
SECTION F - GUNN OSCILLATORS
This selection represents only a part of the Mullard range of solid state sources. Custombuilt
sources, including some with higher output powers, are available on request. Muliard offers a
comprehensive capability in the area of general solid state oscillators, with complex phase
locked and frequency agile sources for military applications.
Type No.
Nominal
Centre
Frequency
(GHz)
prout
(mWl
MinimumMechanical
Tuning
Range
[MHz}
MinimumElectronic
Tuning
Range
(MHz)
Output
Coupling
CLS310 9.4 5 ±50 200 WG16/WR90
CL8G30CLS630S
10.687 3 - - WG16/WR90
CL8631
CL8631S9.35 8 - - WG16/WR90
CLB632
CL8632S9.47 8 - - WG16/WR90
CL8633CLS633S
10.525 8 - - WG16/WR90
CLB640R*CL8640Tt
10.49
10.56
6
6
±60±60
30
8
WG16/WR90WG16/WR90
CLseao** 9.375 5 ±75 50 WG16/WR90
* Receiver local oscillator
T Transmitter** Klystron replacement for marine radars. Complies with B.O.T. specification
BOTSBN 115 10057/1,
S following type number signifies a self-oscillating mixer (auto-detector).
SECTION G - DOPPLER AND TRAFFIC RADARS
Traffic radars
Type No. Description Detection
Range
(metres)
A.C. Suppiv
Vol tage
(V)
CL888QBNX-band traffic radar sensor.
Cable entry through case,100 110
CL8880BNCX-band traffic radar sensor.
Cable entry through
mounting foot
100 110
Dapple r modules
Power Output Voltage Output*Type No. Description Centre frequency typ. typ.
(GH*) (mW) (fiV)
CL8960 10.687 10 40
CL8961 9.350 10 40
CL8962Doppler modules for
volumetric presence9.470 10 40
CL8963detection, industrial
process control,10.525 10 40
CL8964proximity switching,
intruder alarms and9.900 10 40
CLS965similar applications.
10,565 10 40
CL8967 10.365 10 40
Output voltage for input power 100 d8 down on power output at IS dB min.Sl 9nal + noise
SECTION H - MISCELLANEOUS
Horn antenna
Type No. Description Frequency Range
(GHz)
Gam(dB)
ACX-01A Horn antenna for miniature radars 9.0 to 1
1
16
M ix b rs/detecto rs
Type No. Description Centre Frequency
(GHz)
Connections
CL7500
CL7520Waveguide single ended mixers/detectors
10.637
9.35
WG16/WR90
WG16/WR90
parametric amplifier
Type No. Description
Gain
(dB)
Noise
Figure
max.
(dB)
Bandwidth
(MHz)
Frequency
Range
(GHz)
CL9022Packaged parametric amplifier in
temperature stabilized enclosure20 2.3 15 2.7 to 3,1
SECTION J - ISOLATORS AND CIRCULATORS
See selection guide in section J
GENERAL SECTION
GENERAL
MICROWAVE SEMICONDUCTORSGENERAL EXPLANATORY NOTES
TYPE NOMENCLATUREMullard microwave semiconductor devices are registered with Pro-Electron.The type nomenclature of a discrete device or, in certain cases, of a range of devices, consists of threeletters followed by a serial number. The serial number normally consists of two figures, but a suffixletter is added where variants or a series occur.
The first letter indicates the semiconductor material used:
A - germanium
B - silicon
C - compound materials, such as gallium arsenide
The second letter indicates the general function of the device:
A - detection diode, mixer diode
E • backward diode
X - multiplier diode such as varactor or step recovery diode
The third letter is T, V, W, X or Y which indicates that the device is designed or developed for industrial,professional or transmitting applications.
Subscripts for quantity symbols
A, a anode terminal
BR breakdown
F, f forward
I, i input
J, j junction
K, k cathode
O, o open-circuit, output
R, r resistive, reverse, repetitive
S, s series, source
Z,z impedance
O Mullard YJuly 1978
GENERAL
ELECTRICAL PARAMETERS
Resistance
Reactance
Impedance
Admittance
Conductance
Susceptance
Mutual inductance
Inductance
Capacitance
Frequency limits
Bandwidth
Noise factor
Symbols for microwave semiconductor devices
n efficiency
B bandwidth
cd diode capacitance
Ci
junction capacitance
Cmin diode capacitance at breakdown voltage
Co diode capacitance at zero bias
Cp parasitic (parallel) capacitance
Cs stray capacitance
Ctot total capacitance
f operating frequency
fco varactor diode cut-off frequency
1 current
•dc bias current
i.f. intermediate frequency
if d.c. forward current
Ifm peak forward current
IR continuous (d.c.) reverse leakage current
Lc conversion loss
Ls series inductance
M figure of merit
Nf flicker noise
N if noise figure at intermediate frequency
Device Associated
circuit
r R
X X
z Z
Y Y
9 G
b B
m M
1 L
c C
f max.
f min.
Af B
N
July 1978Y Milliard r?
Microwave semiconductors General Explanatory Notes GENERAL
No overall noise figure
N r noise temperature ratio
Pin input r.f . power
pout output r.f. power
ptot total power dissipated within the device
R|_ r.f. load resistance
Rs
spreading resistance
Rth thermal resistance
Si current sensitivity
sts tangential sensitivity
Tamb ambient temperature
Tease case temperature
Ths heatsink temperature at device interface with device
Ti
junction temperature
Tstg storage temperature
tp pulse duration
ts storage time
ttr transition time
V voltage
VBR breakdown voltage
V(BR)R reverse breakdown voltage
vf d.c. forward voltage
Vr d.c. reverse voltage
v.s.w.r. voltage standing wave ratio
Zjf intermediate frequency impedance
Zrf radio frequency impedance
Zv video impedance
vfflicker noise
Jk
PRODUCT SAFETY
The most modern high technology materials have been used in these components to ensure the highest
performance for the user. Some of them are toxic to man but the quantity used in a single device is so
small that the risk of toxic effects are negligible even in extreme circumstances.
U Milliard rJuly 1978
SEMICONDUCTOR GENERAL EXPLANATORYDEVICES NOTES
EXPLANATION OF HANDBOOK DATA
1. FORM OF ISSUEThe semiconductor data published in the Handbook follows the samepattern, as much as possible, concerning, (a) the forms of issue, (b) theratings system and (c) the ratings presentation.
1.1 Types of Data
The Handbook data is published either as tentative or final data.
Tentative Data
Tentative data aims at providing information on new devices as early as
possible to allow the customer to proceed with circuit design. The tentativedata may not include all the characteristics or ratings which will beincorporated later in. the final data and some of the numerical values
quoted may be slightly adjusted later on.
Final Data
The transfer from tentative data to final data involves the addition of thosenumerical values and curves which were not available at tentative datastage and small adjustments to those values already quoted in tentative data.
Reissue of final data may be made from time to time to incorporateadditional information resulting from prolonged production experienceor to meet new applications.
1.2 Presentation of Data
The information on the published data sheets is presented in the followingform
:
—description of basic application and physical characteristics of thedevice,
—quick reference data giving the most important ratings andcharacteristics.
—outline and dimensions. Reference to standard outline nomenclatureif applicable and lead connections.
—Ratings. Voltage, current, power and thermal ratings.
—Characteristics.
—Application information or operating conditions.
—Mechanical and environmental data if applicable.
—Charts showing ratings and characteristics.
2. RATINGSA rating is a limiting condition of usage specified for a device by themanufacturer, beyond which the serviceability may be impaired.
A rating system is a set of principles upon which ratings are established
and which determines their interpretation. There are three systems whichhave been internationally accepted and which allocate responsibility
between the device manufacturer and the circuit designer differently.
Milliard
2.1 Rating Systems
Unless otherwise stated the ratings given in semiconductor data sheets
follow the absolute maximum rating system.
The definitions of the three systems accepted by the International Electro-
technical Commission are as follows:
ABSOLUTE MAXIMUM RATING SYSTEM
Absolute maximum ratings are limiting values of operating and environ-
mental conditions applicable to any device of a specified type as defined
by the published data, and should not be exceeded under the worst
probable conditions.
These values are chosen by the device manufacturer to provide acceptable
serviceability of {he device, taking no responsibility for variations in equip-
ment or environment, and the effects of changes in operating conditions
due to variations in the characteristics of the device under consideration
and of all other devices in the equipment.
The equipment manufacturer should design so that initially and throughout
life no absolute maximum value for the intended service is exceeded with
any device under the worst probable operating conditions with respect
to variations i" supply voltage, environment, equipment components,
equipmen .omrol adjustment, load, signal or characteristics of the device
under consideration and of all other devices in the equipment.
DESIGN-CENTRE RATING SYSTEM
Design-centre ratings are limiting values of operating and environmental
conditions applicable to a bogey device of a specified type as defined by
its published data, and should not be exceeded under normal conditions.
These values are chosen by the device manufacturer to provide acceptable
serviceability cf the device in average applications, taking responsibility
for normal changes in operating conditions due to variations in supply
voltage, environment, equipment components, equipment control adjust-
ment, load, signal or characteristics of all other devices in the equipment.
The equipment manufacturer should design so that initially no design-
centre value for the intended service is exceeded with a bogey device in
equipment operating at the stated normal supply voltage.
DESIGN-MAXIMUM RATING SYSTEM
Design-maximum ratings are limiting values of operating and environ-
mental conditions applicable to a bogey device of a specified type as
defined by its published data, and should not be exceeded under the
worst probable conditions.
These values are chosen by the device manufacturer to provide acceptable
serviceability of the device, taking responsibility for the effects of changes
in operating conditions due to variations in the characteristics of the
device under consideration.
The equipment manufacturer should design so that initially and throughout
life no design-maximum value for the intended service is exceeded with a
bogey device under the worst piobable operating cbnditions with respect
to variations in supply voltage, environment, equipment components,equipment control adjustment, load, signal or characteristics of the device
under consideration and of all other devices in the equipment.
Milliard
GUNN, IMPATTAND NOISE DIODES
B
SILICON AVALANCHENOISE DIODE
BAT31
Epitaxial , silicon planar , broadband noise generator. This is a current controlled device
operated at avalanche breakdown and is effective from less than 10 Hz to above J-band.
Applications include built-in test equipment (BITE) for surveillance , tracking and weather
radars, microwave links , direction finding, p. cm. systems and noise modulators for
electronic countermeasures.
It conforms to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range <10 Hz to >18 GHz
Avalanche voltage min. 17
max. 22
VV
Recommended operating current range 0. 5 to 40 mA
Broadband excess noise ratio (fig. 3) typ. 34 dB
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Dimensions in mm
A: concentricity tolerance ;+ 0.13
01.60w1.52
5770
Normal operation with reverse bias, i.e. heatsink end positive.
MilliardSEPTEMBER 1977 BAT31 Page 1
max. 40 mA
max. 1.0 Wmax. 80 OC
-55 to +150 °C
mln. 17 V
min. 0.4 pF
max. 0.8 pF
max. 0.1 MA
max. 60 a
LIMITING VALUES (Absolute max. rating system)
IR
Ptot
TmbT8tg range
CHARACTERISTICS (T^ = 25 °C)
VBR(R) at IR = 5 mA
Cjat VR = 6V, f = 1MHz
IR at VR = 6 V
Rglope at IR = 40 mA, f = 1 kHZ 1)
^1 at IR = 1 mA and 40 mA, f = 1 kHz l) max. 2.
5
R40
C8
typ. 0.2 pF
Ls typ. 650 pH
Rl1) Rgiope is the reverse slope resistance and =- is the ratio of reverse slope resistance
at 1 mA and 40 mA, measured at 1 kHz. This ratio is included in the characteristics
to eliminate spurious effects in the noise output/current characteristic.
The reverse slope resistance consists of the space charge resistance Rsc , the
spreading resistance R—, and the ' thermal resistance' R^, i. e.
Rslope
= Rsc +Rsp + Rth
where: Rsc is approximately 10 Q at 10 to 40 mA and 19 Q at 1 mA
RSp is approximately 1 Q
VUu is the effective resistance due to isothermal heating in the device when
operated with an infinite heatsink. Above 10 MHz, Rth may be neglected.
2) The location of the top cap should be a hole of diameter 1. 8 to 2. 2 mm, bearing on
flange with a force not exceeding 10 N.
3) Other encapsulations may be made available on request.
MilliardBAT31 Page 2
SILICON AVALANCHENOISE DIODE
BAT31
APPLICATION INFORMATION
The device, as characterized, is operated in a SO Q characteristic impedance measure-ment system. When used as a noise source in an on-off mode, the device, when off,
should appear to be 50 $2. Since it has a large reflection coefficient when zero biased orbiased just below avalanche breakdown, sufficient attenuation is required to provide areasonable match to 50 Q. For the broadest operating frequency range, an attenuator ofapproximately 14 dB with a v. s. w. r. of <1. 2 : 1 is recommended. This will reduce theavailable excess noise by 14 dB. Higher excess noise may be obtained, but over areduced operating frequency range , in a balanced configuration with low noise directionalcouplers (e. g. a 3 dB quadrature coupler) , or fed into a broadband ferrite isolator (or ter-minated circulator) which would reduce the available excess noise by approximately ldB.
Temperature and excess noise relationship
Excess noise Noise temperature 1 Hz bandwidth 1 MHz bandwidth
dB OK dBm dBm
+100 2. 9 x 1012 - 74 - 14
+ 90 2. 9 x 1011 - 84 - 24
+ 80 2. 9 x 1010 - 94 - 34
+ 70 2. 9 x 109 -104 - 44
+ 60 2. 9 x 108 -114 - 54
+ 50 2. 9 x 107 -124 - 64
+ 40 2. 9 x 106 -134 - 74
+ 30 2. 9 x 105 -144 - 84
+ 20 2.9 xl()4 -154 - 94
+ 10 2. 9 x 103 -164 -104
2. 9 x 102 -174 -114
The device may be pulse operated with a rise time of «0. 5 ps
The device should be operated from a constant current source, however, good results
may be achieved using a 28 V supply and typically a metal film or wirewound 1. 6 kQ
resistor in series with the noise diode , with suitable power supply decoupling.
m some applications, current profiling with time may be useful, i.e. linear excess noise
ratio as a function of log bias current as shown in fig. 1. This may be used for receiver
sensitivity measurement on a P. P. I. display.
MilliardBAT31 Page 3
Recommended bias
range for broadbandoperation up to 12.4GHz
45i-
"D
40oc
W.
o 35(-
<D10
bc
<° 30<DuXW
2k0.1
5 6 7 8/ / / /.
i i i i i i I
/9 10 12.4
Y i i i i 1
1
j i
1.0 10 40
Noise diode bias current (mA) D7762
Fig. 1
Typical excess noise ratio as a function of avalanche current
with frequency as a parameter.
Device mounted in a 50 fl 7 mm coaxial line as shown in Fig. 2
MilliardBAT31 Page 4
SILICON AVALANCHENOISE DIODE
BAT31
/
07mm-
/////
//////
S77T77\ PV/V'/\ > y Noise diode
077*3 / / ' /Fig. 2
Device mounted in a 50 $2 7 mm coaxial line
CD
Z
O-t->
o
40
38
36
^ 34
</>
<DuXLU
32
15mA noise diode bias
t Absolute error for 50H1 system impedance
j—i i ' i i
1.0 2.0 5.0 10Frequency (GHz)
Fig. 3 D7764
Typical broadband noise performance for an avalanche current of 15 mAwith device mounted as shown in Fig. 2
MilliardBAT31 Page 5
<M' N *>?
I -»
—-^ tn
>C
c
> <U•*-> U)
<n ac +>
<u o"D >
<b-H
<n Dutr u
a cL. a>a<D .O.
1000
a
100
10
a£a
St(0c
.ID
0000 Measured values
Vb = 19.43 volts
Theoretical fit fori T
j 1' 1 1 1 M
0.1 1.0 10 100
Avalanche current (mA) D7765
Fig. 4
Typical broadband noise density measured over a 1 kHz to 10 kHz bandwidth.
MilliardBAT31 Page 6
SILICON IMPATTDIODE BXY50
A high efficiency silicon Impatt diode for the generation of c.w. power at micro-wave frequencies. It conforms to the environmental requirements of BS9300 whereapplicable.
QUICK REFERENCE DATA
Operating frequency 8.0 to 10 GHz
Pout
(typ.)Crha = 35°C) 600 mWOperating current (typ.
)
135 mA
Operating voltage (typ.
)
91 V
OUTLINE AND DIMENSIONS
02.1max
A-
1 1 621.53
+ ve
3.122.98 li
0.66036
1.801 50
1.621.53
Heatsink
end25 max _x 45'chamfer A = concentricity tolerance =±013
- ve
All dimensions in mm
JUNE 1977Milliard
BXY50 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
P max. (see note 1)
R (j-hs) max.
T .- T, max.
] hs
T rangestg
ELECTRICAL CHARACTERISTICS (Thg
= 25°C)
Min.
V Reverse breakdown voltage(BR)R
(atl = 1.0mA) 65R
I Reverse current (at VD = 50V)R kc Total capacitance (at V.n_.=5V)
TYPICAL OSCILLATOR PERFORMANCE
Operating current (see note 2)
Operating voltage
Frequency (see note 3) 8.
Output power (see notes 2,4,5 and 6) 500
Efficiency" 5.0 - %
OPERATING NOTES
1. The maximum junction temperature is 200 C, therefore care must be taken to
200 -T.hs ,„
ensure that P^ max. sR (J
. hs)W.
200 - Ths W
Rth<*"
hs)
15 °c/w
165 °c
-55 to +175 °c
Typ. Max.
75 85 V
- 10 HA
0.9 - pF
135 mA
91 V
firm
10 GHz
mW
vth'
where P^ = P. - P ...
tot in out
T = temperature of heatsink at interface with device
R (j- hs) = thermal resistance from junction to heatsink in which device
is clamped.
2. The bias supply should be current regulated to within l%and care should betaken
to avoid transient current surges which could cause burnout. The bias circuit
should be arranged to present a high impedance at d. c. tov.h.f. frequencies.
This will help to prevent oscillation in the bias circuit and noisy operation. The
maximum power supply requirements are 115V and 160mA.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The polarity of the device must be strictly observed when applying bias,(see
outline drawing).
5. The output power is normally measured in a coaxial cavity near to centre band
frequency.
Milliard—IVIMMUi %mBXY50 Page 2
SILICON IMPATTDIODE BXY50
OPERATING NOTES (contd.
)
6. The heatsink end of the device should be held in a collet or equivalent clampingsystem to ensure minimum thermal resistance in the path to the mounting base.This in turn must be coupled to an adequate heatsink. Alternatively, directsoldering, using a low melting point solder, or an electrically conductive singleloaded epoxy, such as Epotek H40, may be used.
7. This device may be used as a negative resistance amplifier.
Devices may be selected to suit customers' specific requirements
Split copper heatsink
«. To bias Tee
and r.f. load
(50O)
Movable slug
insulation
Diode
COAXIAL TEST OSCILLATOR CAVITY
MilliardBXY50Page 3
-
op11
j
1
| | 1
*£
,35
-1
—
1
1
—
1
1 _
1—1—
!
—
h
-N-r
sII
...
- h- — —
O
--
--.h+-—t-
— T 1
1
|
-
i
...
J-1
1 -4-!
1 I _
L
<- E
;cr op
Mullard BXY50 Page 4
SILICON IMPATTDIODE BXY51
A high efficiency silicon Impatt diode for the generation of c. w. power at micro -
wave frequencies. It conforms to the environmental requirements of BS 9300 whereapplicable.
QUICK REFERENCE DATA
Operating frequency 10 to 12 GHz
Pout
(typ.)(Th8 =35°C) 450 mW
Operating current (typ.
)
120 mA
Operating voltage (typ.
)
80 V
OUTLINE AND DIMENSIONS
02.1max
A-
il 621 53
+ ve
. 3.12Jp 2 98
1
—
05*77
3-U066 *036
r, 801.50
1.621.53
17
Heatsink
end25max _x 45°chamfer A _ concentricity tolerance =±013
- ve
All dimensions in mm
JUNE 1977Mullard
BXY51 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
P max. (see note 1)tot
Rth ^ " hs) maX *
T - T, max.j hs
T rangestg
ELECTRICAL CHARACTERISTICS (Thg
= 25°C)
V Reverse breakdown voltage(BR)R
(atID = 1.0mA)R
I Reverse current (at VD = 45V)R kCT Total capacitance (at V. >
R- 5V)
TYPICAL OSCILLATOR PERFORMANCE
Operating current (see note 2)
Operating voltage
Frequency (see note 3)
Output power (see notes 2,4,5 and 6)
Efficiency
OPERATING NOTES
1. The maximum junction temperature is 200 C, therefore care must be taken to
200 - Tuhs ,„ensure that P^ max. ^ R^ (j
. hs)W,
where P = P. - P,.
tot in out
T = temperature of heatsink at interface with devicehs
R (j- hs) =thermal resistance from junction to heatsink in which device
is clamped.
2. The bias supply should be current regulated to within l%and care should betaken
to avoid transient current surges which could cause burnout. The bias circuit
should be arranged to present a high impedance at d.c. to v.h.f. frequencies.
This will help to prevent oscillation in the bias circuit and noisy operation.
Particular care should be taken to minimise stray capacitances across the diode.
The maximum power supply requirements are 105V and 170mA.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The polarity of the device must be strictly observed when applying bias, (see
outline drawing).
5. The output power is normally measured in a coaxial cavity near to centre band
frequency.
200 -Tis W
Rth
(^ hs)
19 °c/w
165 °c
-55 to +175 °c
Min. Typ. Max.
55 65 75 V
- - 10 /iA
- 0.85 - PF
120 mA
80 V
10 - 12 GHz
400 450 - mW_ 5.0 - %
Milliard —iwiuiiui v«Bxy51 page 2
SILICON IMPATTDIODE BXY51
OPERATING NOTES (contd.
)
6. The heatsink end of the device should be held in a collet or equivalent clampingsystem to ensure minimum thermal resistance in the path to the mounting base.This in turn must be coupled to an adequate heatsink. Alternatively, directsoldering, using a low melting point solder, or an electrically conductive singleloaded epoxy, such as Epotek H40, may be used.
7. This device may be used as a negative resistance amplifier.
Devices may be selected to suit customers' specific requirements
|
Split copper heatsink
Diode
.RE.
insulation
Movable slug
COAXIAL TEST OSCILLATOR CAVITY
MilliardBXY51 Page 3
NIo
II
o
-
| | | 1 ..
» £
NI©
II
o
|
\n <E
Milliard BXY51 Page 4
SILICON IMPATTDIODE BXY52
A high efficiency silicon Impatt diode for the generation of c.w. power at micro-wave frequencies. It conforms to the environmental requirements of BS 9300 whereapplicable.
QUICK REFERENCE DATA
Operating frequency 12 to 14 GHz
Pout^-XThs^50^ 370 mWOperating current (typ.
)
120 mA
Operating voltage (typ.
)
70 V
OUTLINE AND DIMENSIONS
02.1max
A-
1 1.621 53
+ ve
3.12v 2 98 1L
066036
1 1.801.50
1.621.53
Heatsinkend25max. _
x 45°chamfer A = concentricity tolerance =±013
- ve
All dimensions in mm
JUNE 1977Milliard
BXY52 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
P max. (see note 1)tot
R (j-hs) max.
T - T. max.j hs
T rangestg
ELECTRICAL CHARACTERISTICS (Thg
= 25°C)
V Reverse breakdown voltage
hs W
(BR)R(at ID = 1.0mA)
R
Rth<j
i-hs)
24 °C/W
165 °c
-55 to +175 °c
Min. Typ. Max.
50 55 60 V
- - 10 fiA
- 0.75 - PF
120 mA
70 V
12 14 GHz
300 370 - mW- 4.5 - %
I Reverse current (at V„ = 40V)R KC Total capacitance (at V. R. R
-5V)
TYPICAL OSCILLATOR PERFORMANCE
Operating current (see note 2)
Operating voltage
Frequency (see note 3)
Output power (see notes 2,4,5 and 6)
Efficiency
OPERATING NOTES
1. The maximum junction temperature is 200°C, therefore care must be taken to
200 - Tuhs ,.,
ensure than P^ max. ^ - W
,
tn
where P, ^ = P. - P ,tot in out
T = temperature of heatsink at interface with devicehs
R (j- hs) = thermal resistance from junction to heatsink in which device
is clamped.
2. The bias supply should be current regulated to within l%and care should betaken
to avoid transient current surges which could cause burnout. The bias circuit
should be arranged to present a high impedance at d. c. to v. h. f .frequencies.
This will help to prevent oscillation in the bias circuit and noisy operation.
Particular care should be taken to minimise stray capacitance across the diode.
The maximum power supply requirements are 90V and 150mA.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The polarity of the device must be strictly observed when applying bias,(see
outline drawing).
5. The output power is normally measured in a coaxial cavity near to centre band
frequency.
Milliard —
—
BXY52 Page 2
SILICON IMPATTDIODE BXY52
OPERATING NOTES (contd.
)
6. The heatsink end of the device should be held in a collet or equivalent clamping
system to ensure minimum thermal resistance in the path to the mounting base.
This in turn must be coupled to an adequate heatsink. Alternatively, direct
soldering, using a low melting point solder, or an electrically conductive single
loaded epoxy, such as Epotek H40, may be used.
7. This device may be used as a negative resistance amplifier.
Devices may be selected to suit customers' specific requirements
Split copper heatsink
/ ^Spacer
Diode
« To bias Tee
and r.f. load
(50O)
Movable slug
COAXIAL TEST OSCILLATOR CAVITY
MilliardBXY52 Page 3
~~*
NXom
II
o
J 2
NX<>
II
<- E
._ - w>
MullardBXY52 Page 4
SILICON IMPATTDIODE BXY60
A high efficiency silicon Impatt diode for the generation of c.w. power at micro-wave frequencies. It conforms to the environmental requirements of BS 9300 whereapplicable.
QUICK REFERENCE DATA
Operating frequency 6. to 8. GHz
Pout(typ.)(Ths = 35°C) 750 mWOperating current (typ.
)
125 mA
Operating voltage (typ.
)
120 V
OUTLINE AND DIMENSIONS
r
+ ve
3.122.98
02.1max
A-
it
1162M 53
066 u036
1.801.50
1.621.53
Heatsink
end0.2 5 max. _x LS'chamfer A _ concent.ricity tolerance -t
ve
All dimensions in mm
013
JUNE 1977Milliard
BXY60 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Ptot
max. (see note 1)
Rth (j - hs) max.
T. - T. max.j hs
T. max.
Tstg
ran&e
200 - Tuhs
Rth (J " hs >
W
14 °c/w
165 °c
200 °c
-55 to +175 °c
Mln. Typ. Max.
85 100 115 V
- - 10 M- 0.97 - pF
125 mA
120 V
6.0 - 8.0 GHz
650 750 - mW- 5.0 - %
ELECTRICAL CHARACTERISTICS (Ths = 25°C)
V/dd\d Reverse breakdown voltage(BR)R
(atIR = 5.0mA)
IR Reverse current (at Vr = 70V)
CT Total capacitance (at V/gR*R = 75V)
Operating current (see note 2)
Operating voltage
Frequency (see note 3)
Output power (see notes 2,4,5 and 6)
Efficiency
OPERATING NOTES
1. The maximum junction temperature is 200°C, therefore care must be taken to
200 - Tuhsensure that P
tQtmax. <
R (j. hs)
W,th
rout
T. = temperature of heatsink at interface with device
Rth (J" ns ) = thermal resistance from junction to heatsink in which device
is clamped.
2. The bias supply should be current regulated to within 1% and care should betaken
to avoid transient current surges which could cause burnout. The bias circuit
should be arranged to present a high impedance at d. c. toV.h. f. frequencies.
This will help to prevent oscillation in the bias circuit and noisy operation.
Particular care should be taken to minimise stray capacitances across the diode.
The maximum power supply requirements are 140V and 180mA.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The polarity of the device must be strictly observed when applying bias (see out-
line drawing).
5. The output power is normally measured in a coaxial cavity near to centre band
frequency.
MilliardBXY60 Page 2
SILICON IMPATTDIODE BXY60
OPERATING NOTES (contd.
)
6. The heatsink end of the device should be held in a collet or equivalent clamping
system to ensure minimum thermal resistance in the path to the mounting base.
This in turn must be coupled to an adequate heatsink. Alternatively, direct sold-
ering, using a low melting point solder, or an electrically conductive single
loaded epoxy, such as Epotek H40, may be used.
7. This device may be used as a negative resistance amplifier.
Devices may be selected to suit
customers' specific requirements
Split copper heatsink
/ /Spacer
Movable slug
Diode
COAXIAL TEST OSCILLATOR CAVITY
MilliardBXY60 Page 3
0.8
pout(W)
0.6
0.4
0.2
14 16
D.C. input power (W)
TYPICAL OUTPUT POWER AS A FUNCTION OF D.C. INPUT POWER
06219
0.8
Pout(W)
0.6
0.4
0.2
20 40 60 80 100 120 140
I dc bias(mA)
TYPICAL OUTPUT POWER AS A FUNCTION OF BIAS CURRENT
MullardBXY60 Page 4
GUNN EFFECTDEVICES
CXY11ACXY11BCXY11C
Gallium arsenide bulk effect devices employing the Gunn effect to produce c.w.
oscillations at microwave frequencies. Each device is encapsulated in a standard
microwave package and conforms to the environmental requirements of BS9300where applicable.
QUICK REFERENCE DATA
Operating voltage (typ.
)
7.0 V
Ptot
max. (Tmb = 70oC) 1.0 WOperating frequency 8.0 to 12 GHz
Pout
mln* CXY11A 5.0 mWCXY11B 10 mWCXY11C 15 mW
Unless otherwise stated , data is applicable to all types
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Heatsink/ end
/ 1.6O
/v1.52
-J2.08
1 n
2.21 .j2.03 *
*\\ *
+ve
^
>
_.,_ .>
t-ve 01;|O
1.63
"1.52
Ta.
OS769
1
0.61^a*8"*i
.-2.362.03
M3.10
A: concentricity tolerance = +0.13
All dimensions in mm
MAY 1977Mullard
CXY11A Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Vmax. x)
V max (for less than 1 ms)
Ptot
max. CTmb = 70 °Q
Temperature
Tmt, range
T .. rangestg 6
ELECTRICAL CHARACTERISTICS (Tamb = 25 °Q
]dc (atV = 7.0V) 1)
Frequency *)
Pout
(atV = 7.0V) 3) CXY11ACXY11BCXY11C
7.5 V
9.0 V
1.0 w
-40 to +70 OC
-55 to +150 °C
Min. Typ. Max.
120 150 mA
8. 9.
5
12 GHz
5.0 8.0 - mW10 12 - mW15 20 - mW
A.M. noise to output power ratio *) -90 -100 dB
OPERATING NOTES
*) Bias must be applied in such a way that the mounting base (heatsink end) of the device
is always positive. Reversing the polarity may cause permanent damage. Care
should be taken to protect the device from transients. An 8. 2 V voltage regulator
diode to shunt the power supply is recommended for this purpose.
2) The frequency is governed by the choice of cavity to which the device is coupled.
3) The output power is normally measured in a coaxial cavity at a frequency of 9. 5 GHz.
Other centre frequencies may be supplied at 8. 5, 10. 5 and 11. 5 GHz by suffixing the
type number e.g. CXY11B/10. 5 specifies a diode giving 10 mW min. at 10. 5 GHz.
See the table below.
Diodes with these other centre frequencies will not necessarily oscillate over the
whole 8 to 12 GHz range.
The bias may be optimized to give maximum output power within the V max. and Ptot
max. ratings.
4) A.,M. noise is measured in a 1 Hz to 1 kHz bandwidth with the diode mounted in a
CL8630 oscillator.
5) It is important to ensure good thermal contact between the device and the mounting
base , which in turn should be coupled to an adequate heatsink.
6) The power supply should be low impedance voltage regulated and capable of supplying
approximately 1. 5 times the normal current , to initiate oscillation.
Minimum output
power (mW)
Test Frequency (GHz)
8.5 9.5 10.5 11.5
5 CXY11A/8.
5
CXY11A CXY11A/10.5 CXY11A/11. 5
10 CXY11B/8.5 CXY11B CXY11B/10.5 CXY11B/11.5
15 CXY11C/8.5 CXY11C CXY11C/10.5 CXY11C/11.5
I Complete oscilla
1Devices may be
tors using these devices are obtainable from Mullard Ltd. ,
selected to suit customers' specific requirements.
MullardCXYllAPage 2
GUNN EFFECTDEVICES
CXY14ACXY14BCXY14C
Gallium arsenide bulk effect device employing the Gunn effect to produce c.w. -
oscillations at microwave frequencies. Each device is encapsulated in a standard
microwave package and conforms to the environmental requirements of BS9300
where applicable.
QUICK REFERENCE DATA
Operating voltage 7.0 V
Ptot max. CTmb = 70 °Q 1.0 WOperating frequency 12 to 18 GHz
Pout min. CXY14A 5.0 mWCXY14B 10.0 mWCXY14C 15.0 mW
Unless otherwise stated , data is applicable to all types
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Heatsinkend
+ve -ve fl1 -60
A= concentricity tolerance = +0.13
All dimensions in mm
MAY 1977Milliard
CXY14A Page 1
7.5 V
9.0 V
1.0 W
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
V max. (d. c.
)
V max. (for less than 1 ms)
Ptot
max. (Tmb = 70 °C)
Temperature
Tmb range _4° to +7° °c
Tstg range -55 to +150 oq
ELECTRICAL CHARACTERISTICS (Tamb = 25 °C)
Min. Typ. Max.
Idc
(at V = 7. V) 1) - 120 145 mA
Frequency 2) 12 14 18 GHz
Pout
(at V= 7.0 V) 3) CXY14A 5.0 8.0 - mW
CXY14B 10 12 - mWCXY14C 15 20 - mW
OPERATING NOTES
1) Bias must be applied in such a way that the mounting base (heatsink end) of the device
is always positive. Reversing the polarity may cause permanent damage. Careshould be taken to protect the device from transients. An 8. 2 V voltage regulator
diode to shunt the power supply is recommended for this purpose.
2) The frequency is governed by the choice of cavity to which the device is coupled.
3) The output power is normally measured in a coaxial cavity at approximately centre
-
band frequency. The bias may be optimized to give maximum output power within the
V max. and Ptot:
max. ratings.
4) ft is important to ensure good thermal contact between the device and the mounting
base , which in turn should be coupled to an adequate heatsink.
5) The power supply should be low impedance voltage regulated and capable of supplying
approximately 1. 5 times the normal current , to initiate oscillation.
Devices may be selected to suit customers'
specific requirements
MilliardCXY14APage2
GUNN EFFECTDEVICE
CXY19
Gallium arsenide bulk effect device employing the Gunn effect to produce c.w. .
oscillations at microwave frequencies. Each device is encapsulated in a standard
microwave package and conforms to the environmental requirements of BS9300
where applicable.
QUICK REFERENCE DATA
Operating voltage (note 2) 8 to 15 V
Ptot
max. (Tmb =70°C) 6.0 W
Operating frequency 8 to 12 GHz
Pout
min. (f = 9.5GHz) 100 mW
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
A= concentricity tolerance = +0.13
All dimensions in mm
MAY 1977Milliard
CXY19 Page 1
15 V
6.0 W
-40 to +70 °C
-55 to +150 °C
Min. Typ. Max.
- 450 mA
8.0 9.5 12 GHz
100 150 mW
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
V max. (see note 1)
P„ _ max. (T = 70°C)tot mb '
Temperature
TmbranSe
T . rangestg 6
ELECTRICAL CHARACTERISTICS (Tamb= 25°C)
I (at V = 12V) (see notes 1 and 2)
Frequency (see note 3)
P ^ (see note 2)out
OPERATING NOTES
1. Bias must be applied in such a way that the mounting base (heatsink end) of the
device is always negative. Reversingthe polarity may cause permanent damage.
Care should be taken to protect the device from transients.
2. Each device is measured for maximum output power at 9. 5GHz in a coaxial test
cavity. The bias is optimized for this maximum within the V max. and P max.
ratings. The operating voltage and corresponding current are quoted for this
condition on a test record supplied with each device.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The heatsink end of the device should be held in a collet or equivalent clamping
system to ensure minimum thermal resistance in the path to the mounting base.
This in turn must be coupled to an adequate heatsink. Alternatively, direct sold-
ering, using a low melting point solder, or an electrically conductive single
loaded epoxy, such as Epotek H40, may be used.
5. The power supply should be low impedance voltage regulated and capable of
supplying approximately 1.5 times the normal current, to initiate oscillation.
Devices may be selected to suit
customers' specific requirements
MilliardCXY19 Page 2
GUNN EFFECTDEVICE
CXY19A
Gallium arsenide bulk effect device employing the Gunn effect to produce c.w.
oscillations at microwave frequencies. Each device is encapsulated in a standard
microwave package and conforms to the environmental requirements of BS9300
where applicable.
QUICK REFERENCE DATA
Operating voltage (note 2) 8 to 15 V
Ptot max. (Tmb = 70OQ 6.0 WOperating frequency 8 to 12 GHz
Pout min. (f = 9.5GHz) 200 mW
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Ar concentricity tolerance = +0.13
All dimensions in mm
5772
JUNE 1977Mullard
CXY19A Page 1
Typ. Max.
450 - mA
9.5 12 GHz
250 . mW
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
V max. (see note 1) 15 V
P, max. (T =70°C) 6.0 Wtot
v mb
Temperature
T ,_ range -40 to +70 °Cmb
T range -55 to +150 °Cstg *
ELECTRICAL CHARACTERISTICS (Tamb = 25°C)
Min.
Idc(at V = 12V) (see notes 1 and 2)
Frequency (see note 3) 8.
Pout <see note 2) 20°
OPERATING NOTES
1. Bias must be applied in such a way that the mounting base (heatsink end) of the
device is always negative. Reversing the polarity may cause permanent damage.
Care should be taken to protect the device from transients.
2. Each device is measured for maximum output power at 9. 5GHz in a coaxial test
cavity. The bias is optimized for this maximum within the V max. and Ptot max.
ratings. The operating voltage and corresponding current are quoted for this
condition on a test record supplied with each device.
3. The frequency is governed by the choice of cavity to which the device is coupled.
4. The heatsink end of the device should be held in a collet or equivalent clamping
system to ensure minimum thermal resistance in the path to the mounting base.
This in turn must be coupled to an adequate heatsink. Alternatively, direct sold-
ering, using a low melting point solder, or an electrically conductive single
loaded epoxy, such as Epotek H40, may be used.
5. The power supply should be low impedance voltage regulated and capable of
supplying approximately 1.5 times the normal current, to initiate oscillation.
Devices may be selected to suit
customers' specific requirements
MilliardCXY19A Page 2
GUNN EFFECTDEVICE
CXY19B
Gallium arsenide bulk effect n+ sandwich device employing the Gunn effect to produce
c. w. oscillations at microwave frequencies. Each device is encapsulated in a standard
microwave package and conforms to the environmental requirements of BS9300 whereapplicable.
QUICK REFERENCE DATA
Operating voltage ^) 8 to 15 V
Ptot max. (Tmb = 70 °C) 7.5 WOperating frequency- 8 to 12 GHz
Pout min ' <f=9.5GHz) 300 mW
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Dimensions in mm
+ve 0J;|O
A: concentricity tolerance = +0.13
All dimensions in mm
JUNE 1977Milliard
CXY19B Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Vmax. !) 2)
15 V
Ptot
max. CTmb = 70°C)°™ 7.5 W
Temperature
Tmb ranSe
Tgtg range
ELECTRICAL CHARACTERISTICS (Tamb = 25 °C)
Idc*>
Frequency )
Pout
2)
-40 to +70 °C
-55 to +150 °c
Min. Typ. Max.
650 900 mA
8. 9.
5
12 GHz
300 325 - mW
Devices may be selected to suit
customers' specific requirements
1) Bias must be applied in such a way that the mounting base (heatsink end) of the device
is always negative. Reversing the polarity may cause permanent damage. Care should
be taken to protect the device from transients.
2) Each device is measured for maximum output power at 9. 5 GHz in a coaxial test
cavity. The bias is optimized for this maximum within the V max. and Ptot max.
ratings. The operating voltage and corresponding current are quoted for this condition
on a test record supplied with each device.
3) The frequency is governed by the choice of cavity to which the device is coupled.
4) The heatsink end of the device should be held in a collet or equivalent clamping system
to ensure minimum thermal resistance in the path to the mounting base. This in turn
must be coupled to an adequate heatsink. Alternatively, direct soldering, using a low
melting point solder, or an electrically conductive single loaded epoxy, such as
Epotek H40, may be used.
5) The power supply should be low impedance voltage regulated and capable of supplying
approximately 1.5 times the normal current, to initiate oscillation.
MilliardCXY19B Page 2
GUNN EFFECTDEVICE
CXY21
Gallium arsenide bulk effect device employing the Gunn effect to produce c.w.
oscillations at microwave frequencies. It is encapsulated in a standard microwave
package and conforms to the environmental requirements of BS9300 where appli-
cable.
QUICK REFERENCE DATA
Operating voltage 8.0 V
Ptot max. (Tmb = 70°C) 2.5 W
Operating frequency range 8.0 to 12 GHz
Pout typ. (at fQ= 9. 5 GHz) 50 mW
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Heatsinkend
+ve -ve •];|0
A: concentricity tolerance = +0.13
All dimensions in mm
MARCH 1978Milliard
CXY21 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
V max. 1) 10 V
V max. (for less than 1 ms.
)
12 V
Ptot
maX*(Tmb
= 70 ° C) 2 - 5 WTmb range -40 to +70 oq
Tstg range -55 to +150 <>C
ELECTRICAL CHARACTERISTICS (Tamb = 25 °C)
Min. Typ. Max.
Frequency range 2) 8. - 12 GHz
D.C. operating current (at V = 9.5 V) - 210 265 mA
Power output 3) 40 50 - mW
OPERATING NOTES
1) The heatsink end is positive. Bias must be applied in such a way that the mountingbase end of the device is always positive. Reversal of the bias will cause permanentdamage. Care should be taken to prevent the device from transients. An 11 V voltage
regulator diode to shunt the power supply is recommended for this purpose.
2) The frequency is governed by the choice of cavity to which the device is coupled.
3) The power output is normally measured in a coaxial cavity at approximately mid-bandfrequency. The bias may be optimized to give maximum power output within the limits
of V max. and Ptot
max.
4) The heatsink end of the device should be held in a collet or similar clamping systemto ensure minimum thermal resistance in the path to the mounting base. This in turn
must be coupled to an adequate heatsink. Alternatively, direct soldering, using a lowmelting point solder, or an electrically conductive single loaded epoxy such as EpotekH40, may be used.
5) The power supply should below impedance voltage regulated and be capable of supply-
ing 1. 5 times the normal current, to initiate oscillation.
Devices may be selected to suit customers'
specific requirements.
MullardCXY21 Page 2
Data based on pre-production devices
CXY24A(Dev.No.
823CXY/B)
CXY24B(Dev.No.
823CXY/C)
GUNN EFFECT DEVICES
Gallium arsenide bulk effect devices employing the Gunn effect to produce c.w. oscillations at micro-
wave frequencies. They are encapsulated in metal-ceramic packages suitable for mounting in various
types of cavity. The devices will oscillate in Q-band (Ka-band), the actual frequency being determined
by the type of cavity.
QUICK REFERENCE DATA
Operating frequency range
Operating voltage
Operating current
Power output at 34 GHz CXY24ACXY24B
30 to 38 GHz
typ. 3.5 V
typ. 0.8 A
min. 25 mWmin. 50 mW
Dimensions in mmMECHANICAL DATA
Avoid pressure
in this area
Preferred areaof contact
O.i.
Top cap positive
Heatsink endnegative
-3.00.P 2.85
U MilliardMay 1978
CXY24A(Dev.No.
823CXY/B
CXY24B(Dev.No.
823CXY/C)
max. 6.0 V
max. note 2
max. 4.0 W-55 to +150 °C
max. +70 °C
RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC134)
Transient supply voltage (note 1
)
Continuous supply voltage
Power input (note 2)
Storage temperature range
Operational stud temperature (note 3)
CHARACTERISTICS
Tamb=25°C
Frequency (notes 4,5)
Operating voltage (notes 1,2)
Operating current (note 6)
Threshold current
Power output (note 4) CXY24ACXY24B
OPERATING NOTES
1. Bias must be applied in such a way that the heatsink end of the device is always negative. Reversing
the polarity may cause permanent damage. Care should be taken to protect the device against
transient voltages.
2. Each device is supplied with a maximum supply voltage recommendation for continuous operation,
within the limits of operating voltage and power input specified above.
3. Good thermal conductivity is essential between the heatsink end of the device and the cavity.
4. Power output is normally measured in a waveguide cavity at a frequency of 34 GHz, at a voltage not
exceeding the maximum recommended supply voltage (see note 2).
5. The frequency is governed by the choice of cavity to which the device is coupled.
6. The power supply should be low impedance, voltage regulated and capable of supplying current in
excess of the threshold current.
mm. typ. max.
30 34 38 GHz
- 3.5 5.0 V- 0.8 1.1 A- - 1.6 A
25 30 — mW50 60 - mW
Devices may be selected to suit
customers' specific requirements
May 1978
Milliard Zf
MIXER AND DETECTORDIODES
MICROWAVE MIXER/DETECTORDIODE
BAT10
Silicon Schottky barrier diode for use as a low level detector or as a low noise mixer at
microwave frequencies. The diode is plastic encapsulated with ribbon leads suitable for
mounting in stripline circuitry and conforms to the environmental requirements of BS9300
where applicable. Available as a matched pair 2/BAT10 M.
QUICK REFERENCE DATA
Frequency range 1. to 12 GHz
Mixer:Typical noise figure in X-band 7.0 dB
Detector
:
Typical tangential sensitivity in X-band with 100 nA bias -50 dBm
Typical current sensitivity in X-band with 50 /xA bias 5.0 nA/nW
OUTLINE AND DIMENSIONS
iD-fo.i
6.4
-02.5 »•
w 105
T
Reference plane for r I admittance
All dimensions in mm 03io«
JUNE 1977Milliard
BAT10 Page 1
LIMITING VALUES (Absolute max. rating system)
Electrical
Maximum peak pulsed r.f. input power at 9. 375 GHz,0.5 us pulse length
Maximum burn out (multiple r.f. spike, ANQ = 1 dB)
Temperature
Tstg range
Tamb Mn8e
ELECTRICAL CHARACTERISTICS (Tamb = 25 °C)
Mixer
Noise figure )
v . s. w. r. Voltage standing wave ratio )
Zif
Detector
Sts
si
V.s.w.r.
Zv1
f
Intermediate frequency impedance
Tangential sensitivity )
Current sensitivity )
Voltage standing wave ratio )
Video impedance )
Noise
1.0 W20 nj
0.2 erg
55 to +150 °C
55 to +150 °C
Typ. Max.
7.0 7.5 dB
- 2:1
- 500 n
-SO _ dBm
5.0 - MA/nW
- 5:1
600 - n
12 17 dB
NOTES
1. Measured in a 50 fi test mount at f = 9.375 GHz, rectified current = 2.0 mA, load
resistance = 20 0, i.f. = 45 MHz and i.f. noise figure = 1. 5 dB. BS9300.
2. Measured with respect to 50 fi at f = 9.375 GHz, rectified current = 2.0 mA, and
load resistance = 10 fi. BS9300.
3. Measured in a 50 £2 test mount at f =9.375 GHz, rectified current = 2.0 mA, load
resistance = 20 fiand i.f. = 45 MHz. BS9300.
4. Measured at f = 9. 375 GHz with 2. MHz bandwidth and 100 fiA bias.
5. Measured at f = 9. 375 GHz at an input power of 1. jiW and 50 fiA bias.
6. Measured with respect to 50 fiat f = 9.375 GHz, 100 nA bias and c.w. input less than
2.0 /xW. BS9300.
7. D.C. measurement with 1.0 mV max. and 50 /iA bias.
MilliardBAT10P&ge2
MICROWAVE MIXER/DETECTORDIODE
BAT10
No
Noise figure
(dB)
7.4
7.2
7.0
6.8
6.6
f= 9.375 GHz
i.f. = 45 MHzN
jf= 1.5 d B
1.5 2.0 2.5 3.0 3.5 4.0
Rectified current I ImA)
TYPICAL NOISE FIGURE AS A FUNCTION OF RECTIFIED CURRENT(MIXER APPLICATION)
450
I.Ff
impedance
(fl)
(00
350
300
MillI.R=45MHz
1.0 2.0 3.0 4.0
Rectified current I (mA)
TYPICAL I. F. IMPEDANCE AS A FUNCTION OF RECTIFIED CURRENT(MIXER APPLICATION)
MilliardBAT10 Page 3
Localoscillator
power(rrW)
5.0
4.0
3.0
2.0
1.0
f= 9.375 GHz
1.0 zo 3.0 4.0
Rectified current I (mA)
TYPICAL LOCAL OSCILLATOR POWER AS A FUNCTION OF RECTIFIED CURRENT(MIXER APPLICATION)
MullardRATIO Page 4
MICROWAVE MIXER/DETECTORDIODE
BAT10
Sts
Tangential
sensitivity
(dBm)-50
-C9
-48
-LI
-46
-45
f= 9.375 GHz
Video bandwidth = Oto 2 MHzi
JIJ
/
f
I
1
11
1
.
,
...
ZvVideo
impedance
(A)
50 100 150 200
D.C. forward bias (jiA)
TYPICAL TANGENTIAL SENSITIVITY AS A FUNCTION OFD.C. FORWARD BIAS CURRENT (DETECTOR APPLICATION)
MS73
1500
1000
500
50 no CO 200 250 300D.C. forward bias (>iA)
TYPICAL VIDEO IMPEDANCE AS A FUNCTION OFD.C. FORWARD BIAS CURRENT. (DETECTOR APPLICATION)
MilliardRATIO Page 5
zs****,
$o 3109
TYPICAL ADMITTANCE AS A FUNCTION OF FREQUENCY
MilliardBAT 10 Page 6
MICROWAVEMIXER DIODE
BAT11n
Silicon Schottky barrier low noise mixer diode mounted in a L.I.D. type envelope. •
Primarily intended for hybrid integrated circuit applications in X-band. It con-
forms to the environmental requirements of BS9300 where applicable. Available
as a matched pair 2/BATH M.
QUICK REFERENCE DATA
Typical noise figure in X-band 6.5 dB
Frequency range up to 12 GHz
MECHANICAL DATA Dimensions in mm
Contactfaces
Contact
D7511
Contact faces are gold plated ,- 5 /tin over 1. 27 ycm of nickel.
JUNE 1977Mullard
BATH Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
Max. burn-out (r.f. spike)
Max. burn-out (multiple d. c. spike)
Temperature
T8tg
range
amb
ELECTRICAL CHARACTERISTICS (Tamb= 25°C)
20 nj
0.2 erg
30 nj
0.3 erg
-55 to +150 °C
-55 to +150 °C
Min. Typ. Max.
Dynamic
NQ Noise figure (see note 1) - 6.5 7.0 dB
Z rf R.F. impedance spread referred
to 50ft bounded by co-ordinates
(see note 2).
Z.. Intermediate frequency
impedance (see note 3) 280
Operating frequency range
6 - jO. 3 0.4 - jO.3
6 + j0. 3 0.4 + J0.3
320 380 3
- 12 GHz
NOTES
1. Measured at 9. 375GHz ± 0. 1GHz, 1.5mA rectified current, R. = 1512. N inc-
ludes Nif= 1.5dB with 45MHz intermediate frequency. BS9321/1406.
2. Measured at 9.375GHz ± 0. 1GHz, 1.5mA rectified current, RL = 15fi. BS9321/
1409.
3. Measured at 9. 375GHz ± 0. 1GHz, 1.5mA rectified current, R. = 15J2, inter-
mediate frequency 45MHz, BS9321/1405.
4. Maximum out of balance condition for a matched pair:
a) 0. 1mA rectified current.
b) R. F. admittance 1. 15: 1 with other diode normalized to 50fi.
5. The diode maybe mounted on microstrip, using conventional thermocompression
or micro -gap bonding techniques. Alternatively, the application of a single loaded
epoxy, such as Epotek H40, may be used, followed by polymerisation at 150°C
for 15 minutes. The force applied to the-L.I.D. must not exceed 147mN (15gf).
6. Devices may be specially selected with the r.f. impedance measured at a cust-
omer' s specific frequency in the range 8. 4 to 12GHz.
Milliard' *^ BATH Page 2
MICROWAVEMIXER DIODE
BAT11
D5855
If10
ImA)
/
/*> /
s/
m
2 U 6 VF (V)
?n
?n3\J
*°Ir
2 1 VR(V)
TYPICAL D.C. CHARACTERISTIC
MilliardBATH Page 3
Milliard BATH Page 4
BAT 38
MICROWAVE MIXER DIODE
Subminiature silicon Schottky barrier mixer diode for use at Q-band (Ka-band) frequencies. Where
applicable, this device conforms to the environmental requirements of BS9300.
QUICK REFERENCE DATA
Frequency range
Noise figure typ.
26 to 40 GHz
8.5 dB
MECHANICAL DATA*2.56*2.S3 >
1
02.51max
1
Dimensions in mm
I
f TA
• 1.42 -
TA
„ U2 „w1.17
t
„ 1.32 „
1
. 1.8 „ * 1.32 .* 1.17 * * 1.22 *
)
" 1.7 •
< 7.16
H 1.22 *
"6.65
XX s reference plane
AA ss concentricity tolerance =+ 0.15
DMlTa
Fig.1
The cathode (positive) is marked red.
The cathode indicates the electrode which becomes positive in an a.c. rectifier circuit
Z! Mullard ¥June 1978
BAT 38
J\.RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC134)
Burn-out
R.F. spike max.
Peak pulse power (tp = 0.2 /us) max.
The devices are 100% burn-out screened to the above specifications at 34 GHz.
0.04
0.5
stg
Tamb
"R
'F
Zjf
-55 to +100 oc
-55 to +100 °C
typ. 2.0 MA
typ. 2.0 mA
typ. 8.5 dB< 10 dB
typ. 5.5 dB
Temperature
Storage temperature
Ambient temperature
CHARACTERISTICS Tamb = 25°C
Reverse current Vr = 0.5 V
Forward current Vp = 0.5 V
Overall noise figure
f = 34.86 GHz, rectified current = 0.5 mAN includes Njf of 1.5 dB (BS9321/1406)
Conversion loss
Noise temperature ratio
I.F. = 45 MHz
Voltage standing wave ratio*
f = 34.86 GHz, rectified current = 0.5 mAR L =15fi(BS9321/1409)
Intermediate frequency impedance
f = 34.86 GHz, rectified current = 0.5 mAR L = 15 SI, i.f. = 45 MHz (BS9321/1405)
Operating frequency range
MATCHED PAIRS
The diodes can be supplied in matched pairs under the type number 2/BAT38M. The diodes are
matched to ±10% on rectified current and within 150 £2 i.f. impedance.
1.6:1
erg
W
typ. 1.4:1
< 1.8:1
typ. 900 n700 to 1100 n
26 to 40 G
* Standard test holder.
June 1978
Mullard r?
BAT 38
3.0
2.0
1.0
R load -25fl
1
1.0 2.0 3.0 40 Local oscillator power ImWI
Fig.2 Typical rectified current as a function of local oscillator power at 34.86 GHz
m 15
o 13
1 1 1 1
i.f. = 45MHzN
j(= 1.5dB
1I
I
1I
\\1
L
\>V
200 400 600 800 1000 1200
Local oscillator power (gW)
Fig.3 Typical overall noise figure as a function of local oscillator power at 34.86 GHz
MilliardJune 1978
MICROWAVEMIXER DIODES
BAT39BAT39A
Subminiature silicon reversible Schottky barrier diodes primarily intended for low noise
mixer applications in X-band. They are intended as retrofits for AAY39 and AAY39A.
Available in a matched pair as 2/BAT39M.
QUICK REFERENCE DATA
Operating frequency 1.0 to 18 GHz
Noise figure at X-band BAT39 typ. 6.0 dB
BAT39A typ. 7.0 dB
Unless otherwise stated, data is applicable to both types.
MECHANICAL DATA Dimensions in mm
»!:S
rrA
1.A2"1.17
2.562.53
1.32
1.22
02.51max
1.81.7
7.16
6.65
1.321.22"
XX = reference plane All dimensions in mmAA = concentricity tolerance =+ 0.15
U2"1.17
02527a
Terminal identification
The positive end (cathode) is marked red.
The positive end indicates the electrode which becomes positive in an a.c. rectifier
circuit.
ACCESSORIES
WG16 holders to fit these diodes are available from Marconi Instruments Ltd.
,
(Sanders Division), Gunnels Wood Road, Stevenage, Herts.
MilliardJUNE 1977 BAT39 Page 1
RATINGS In accordance with the Absolute Maximum Ratings System (IEC134)
Burn-out f= 9. 375 GHz
Multiple d. c. spike
Multiple r. f. spike (spike width at
half peak power = 2 /xs)
Peak pulse power
f = 9. 375 GHz, tp= 1.0 /xs
Temperatures
Storage temperature
Ambient temperature
CHARACTERISTICS
Reverse current V^ = 0. 5 V
Forward current VF = 0. 5 V
Overall noise figure
f = 9. 375 GHz, RL = 15 8, BAT39rectified current = 1. mA BAT39AN includes Ntf = 1. 5 dB
(BS9300/1406 Method B)
'stg
Tamb
Min.
5.5
0. 1 erg
0.05
0.5
erg
W
-55 to +100 °C
-55 to +100 °C
T -amb 25 °C
fyp. Max.
2.0 MA
7.0 mA
6.0 6.5 dB
7.0 7.5 dB
Conversion loss BAT39BAT39A Lc
4.2
5.0
dB
dB
Noise temperature ratio
I.F. = 45 MHz (BS9300/1407) BAT39BAT39A
NrNr
- 1.1:1- 1.2:1
Voltage standing wave ratio
f = 9. 375 GHz, RL = 15 fi,
rectified current = 1. mA(BS300/1409)
Measured in standard test holder
v. s.w. r. 1.43:1
Intermediate frequency impedance
f = 9.375 GHz, RL = 15 £2
rectified current = 1.0 mA(BS9300/1405)
Operating frequency range
Zif 250
1.0
450 fi
18 GHz
MilliardBAT39 Page 2
MICROWAVE BAT39MIXER DIODES BAT39A
OPERATING NOTE
Optimum performance is obtained with BAT39 and BAT39A when the local oscillator
drive is" adjusted to give a diode rectified current of 1. mA and the load resistance is
restricted to 100 fi max.
APPLICATION INFORMATION
Mixer performance at other than Test Radio Frequency
Measured overall noise figure
f = 16.5 GHz, Nif= 1.5 dB, i.f. =45 MHz N<, typ. 7.0 dB
f= 3.0 GHz, Nif= 1.5 dB, i.f. =45 MHz N typ. 5.5 dBf= 9.5 GHz, i.f. = 3.0 kHz N typ. 29 dB
Signal/flicker noise at 9. 5 GHz
Measured at 2. kHz from carrier in
a 70 Hz bandwidth typ. 131 dB
Detector performance
Tangential sensitivity at 9. 375 GHz,
1 kHz to 1 MHz video bandwidth,
IF (bias) = 50 nA (BS9300/1411) Stg
typ. -52 dbm
A.C. video impedance
IF (bias) = 50 fiA (BS9300/1403) Zr typ. 800 fi
MullardBAT39 Page 3
D7396
^ 6.0
•
oa
| 5.0
o
4.0
3.0
-
2.0
1.0
1.0 2.0 3.0 4.0
Rectified current L(mA)
Typical rectified current as a
function of local oscillator power
MilliardBAT39 Page 4
MICROWAVEMIXER DIODES
BAT39BAT39A
«.b"
8 0-L
I
65 - I
\\
\
6.0 —
\
5.5 _1.0 2.0 3.0 4.0
Rectified current (mA)
Typical noise figure as a function
of rectified current
MullardBAT39 Page 5
MICROWAVEMIXER DIODES
BAT50BAT50R
Coaxial silicon Schottky barrier diodes for use in pre-tuned X-band low noise mixer <—circuits. They are intended for use as low noise retrofits at X-band frequencies for
coaxial mixer diodes types AAY50, AAY50R etc. The two types have identical dimensionsand characteristics but the polarity is reversed. The pair are intended for use in balanced
mixer circuits and conform to the environmental requirements of BS9300 where applic-
able.
QUICK REFERENCE DATA
Operating frequency max. 12 GHz
Noise figure typ. 6.2 dB
MECHANICAL DATA
Conforms to BS3934 SO-26
Dimensions In mm
02S01Q
Terminal identification
BAT50 Pin cathode
Body (red spot) anode
ACCESSORIES
BAT50R Pin anode
Body (green spot) cathode
Holders to fit these coaxial diodes are available in the U. K. from Marconi Instruments(Sanders Division) Gunnels Wood Rd. , Stevenage, Herts.
Note 1. The device is designed to make contact on this open face.
Note 2. Cone tapers to a radius of 0. 13 mm nominal.
MilliardJUNE 1977 BAT50 Page 1
RATINGS In accordance, with the Absolute Maximum Rating System (IEC134)
Burn-out
R. F. spike max. 0. 2 erg
Peak pulse power
tp= 0. 5 us
Temperatures
Storage temperature
Ambient temperature
CHARACTERISTICS
Reverse current Vo = 0. 5 V
Forward current Vp = 0. 5 V
Overall noise figure *)
f = 9. 375 GHz, rectified current = 1. mA,RL = 15 fi, N includes 1% = 1. 5 dB
Conversion loss
Noise temperature ratio
I. F. = 45 MHz
Voltage standing wave ratio *) 2)
f = 9375 ± 10% MHz, rectified current 1. mARL = 15 fi, NQ includes Nif = 1. 5 dB
Intermediate frequency impedance
Operating frequency range
max. 1.0 W
Tstg
-55 to +100 °C
^amb -55 to +100 °C
Tamb= 25 °c
fc 3. /iA
lF 7.0 mA
Notyp.
max.
6.2 dB
6.8 dB
v. s.w. r. max.
4.4 dB
1.1: 1
1. 43: 1
min. 300 n
max. 500 Q
max. 12 GHz
1) Measured in standard holder (K1007, Issue 3, Section 8B3. 3. 1/2.)
2) The nominal rectifier admittance at a plane 7.01 mm inside the body from the open
end is
—— + -J— mho.83.5 350
MilliardBAT50 Page 2
MICROWAVE BAT50MIXER DIODES BAT50R
OPERATING NOTE
These devices will exhibit their inherent improved noise figure performance over the
frequency range 1.0 to 12 GHz, but are not recommended for use as direct replacements
in pre-tuned mounts designed for the AAY50 type coaxial diode, at other than X-band
frequencies.
APPLICATION INFORMATION
Signal/Flicker noise ratio
f = 9. 5 GHz. Measured at 2 kHz from carrier
in 70 Hz bandwidth typ. 131 dB
Detector performance
Tangential sensitivity, f = 9. 375 GHz,video bandwidth = 1. MHz, Ip (bias) = 50 pA S^ typ. -52 dBmvideo impedance, IF (bias) = 50 /iA Zy typ. 800 Q
MilliardBAT50 Page 3
MICROWAVEMIXER DIODES
BAT51BAT51R
The BAT51 and BAT51R form a reverse pair of mixer diodes for use in balanced mixer
circuits at J -band (Ku band). The diodes are of silicon Schottky barrier construction and
are intended as retrofits for AAY51 and AAY51R. They are packaged in the standard
coaxial outline for this band , similar to 1N78 types. The encapsulation is hermetically
sealed and the diodes conform to the environmental requirements of BS9300 where
applicable. Available as a matched pair as 2/BAT51 MR.
QUICK REFERENCE DATA
Frequency range 12 to 18 GHz
Noise figure typ. 7.0 dB
Unless otherwise stated, data is applicable to both types.
MECHANICAL DATA Dimensions in mm-
DO- 37
5.59,5.49
1
19.4318.67
-m 07405
A = concentricity tolerance = ± 0. 35
*These limits apply only over 10. 32 dimension
Terminal identification
BATS1 Pin cathode
Body (red) anode
BAT51R Pin anode
Body (green) cathode
JUNB 1978Milliard
BAT51 Page 1
RATINGS la accordance with the Absolute Maximum System (IEC134)
Burn-out
f = 9. 375 GHz, multiple r.f. spike,
spike width at half peak power = 2 ns
Peak pulse power
f = 9. 375 GHz, tp= 1.0 *is
Temperatures
Storage temperature
Ambient temperature
CHARACTERISTICS
Reverse current V^ = 0. 5 V
Forward current Vp = 0. 5 V
Overall noise figure
f = 13.5 GHz,N includes N
tf= 1. 5 dB
Measured in JAN 201 holder (BS9300/1406 Method A)
Conversion loss
Noise temperature ratio
I.F. = 45 MHz (BS9300/1407)
Voltage standing wave ratio
f = 13.5 GHz
Intermediate frequency impedance
*stg
*amb
Zif
max. 0. 05 erg
0.5 W
-55 to +100
•55 to +100
oc
°C
Tamb = 25 °C
max.
typ.
typ.
max.
0.2
7.0
7.0
7.5
uA
mA
dB
dB
5.2 dB
1.1: 1
1.5: 1
min. 250 Q
typ. 350 Q
max. 450 Q
12 to 18 GHzOperating frequency range f
FINISH
The bodies are cadmium plated in order to be compatible with an aluminium holder
MATCHED PAIR
Maximum unbalance conditions, Z^ = 25 fi, rectified current 0. 1 mA.
MilliardBAT51 Page 2
MICROWAVEMIXER DIODES
BAT51BAT51R
D7S12
4.0
power(mW)
3.0
2.0
1.0
1.0 2.0 3.0 4.0 Rectified current I (mA)
Typical rectified current as a function of local oscillator power
D7SI3
10.0
Noise figure
No _1_
MB) 1
9.0 I
\1
8.0
7.0
6.0
1.0 2.0 3j0 4j0 Rectified current l (mA)
Typical noise figure as a function of rectified current
MullardBAT51 Page 3
MICROWAVEMIXER DIODES
BAT52BAT52R
The BAT52 and BAT52R form a reverse pair of mixer diodes for use in balanced mixercircuits at J-band (Ku band). The diodes are of silicon Schottky barrier construction andare intended as retrofits for AAY52 and AAY52R. They are packaged in the standardcoaxial outline for this band, similar to IN78 types. The encapsulation is hermeticallysealed and the devices conform to the environmental requirements of BS9300 whereapplicable. Available as a matched pair as 2/BAT52MR.
Frequency range
Noise figure
QUICK REFERENCE DATA
typ.
12 to 18
8.0
GHz
dB
Unless otherwise stated , data is applicable to both types.
MECHANICAL DATA Dimensions in mm •
DO- 37
I I
,4.80 t f'4.72
19.4318.67
- D7405
A = concentricity tolerance = ±0. 35
*These limits apply only over 10. 32 dimension
Terminal identification
BAT52 Pin cathode
Body (red) anodeBAT52R Pin anode
Body (green) cathode
JUNE 1978Milliard
BAT52 Page 1
RATINGS In accordance with the Absolute Maximum System (IECI 34)
Burn-out
f = 9. 375 GHz, multiple r.f. spike,
spike width at half peak power = 2 ns
Peak pulse power
f = 9. 375 GHz, tp= 1.0 ns
Temperatures
Storage temperature
Ambient temperature
CHARACTERISTICS
Reverse current Vr = 0. 5 V
Forward current Vp = 0. 5 V
Overall noise figure
f = 13.5 GHz,N includes Nif
= 1. 5 dB
Measured in JAN 201 holder (BS9300/1406 Method A)
Conversion loss
Noise temperature ratio
I.F. = 45 MHz (BS9300/1407)
Voltage standing wave ratio
f = 13. 5 GHz , rectified current = 0. 9 mA
Intermediate frequency impedance
stg
amb
Zif
max. 0. 05 erg
max. 0.
5
W
-55 to +100 °C
-55 to +100 °C
Tamb = 25 °C
max. 0.
2
nA
typ. 7. mA
typ.
max.
min.
typ.
max.
8.0 dB8.5 dB
5.2 dB
1.1: 1
1.5:1
250 G
350 Q
450 a
12 to 18 GHzOperating frequency range f
FINISH
The bodies are cadmium plated in order to be compatible with an aluminium holder
MATCHED PAIR
Maximum unbalance conditions, Z^ = 25 fl, rectified current 0. 1 mA.
MilliardBAT52 Page 2
MICROWAVEMIXER DIODE
BAT59
Subminiature silicon Schottky barrier mixer diode for use at Q-band (Ka-band). Whereapplicable, this device conforms to the environmental requirements of BS9300.
QUICK REFERENCE DATA
Frequency range 26 to 40 GHz
Noise figure typ. 8.5 dB
MECHANICAL DATA Dimensions in mm
•!:B
TT
U2"1.17'
,2.562.53
1.321.22'
XX s reference plane
AA = concentricity tolerance =+ 0.15
02.51max
1.81.7'
7.166.65"
1.321.22"
1.A2"1.17
"
D2S27Q
The cathode (positive) is marked red.
The cathode indicates the electrode which becomes positive in an a. c. rectifier circuit.
JUNE 1978Muttard
BAT59 Page 1
RATINGS Limiting values in accordance with the Absolute Maximum System (IEC134)
Burn-out (at 9. 375 GHz)
R.F. spike
Peak pulse power (tp= 0. 2 ps)
Temperature
Storage temperature
Ambient temperature
CHARACTERISTICS
Reverse current Vr = 0. 5 V
Forward current Vp = 0. 5 V
Overall noise figure
f = 34. 86 GHz , rectified current = 0. 5 mAN includes Nif of 1. 5 dB (BS9321/1406)
Conversion loss
Noise temperature ratio
I.F. =45 MHz Nr 1.6:1
Voltage standing wave ratio *)
f= 34. 86 GHz, rectified current = 0.5 mA V8Wr tJrP* 1,4: l
RL= 15 SI (BS9321/1409)
v.. . . < j g . j
' Intermediate frequency Impedance
f= 34.86 GHz, rectified current = 0.5 mA typ. 900
RL = 15 a, i. f. = 45 MHz (BS9321/1405)Mf 700 to 1100
Operating frequency range f 26 to 40 GHz
MATCHED PAIRS
The diodes can be supplied in matched pairs under the type number 2/BAT59M. The
diodes are matched to ±10% on rectified current and within 150 Q i. f. impedance.
max. 0.04 erg
max. 0.5 W
Tstg -55 to +100 oc
*amb -55 to +100 °C
Tamb~ 25 °C
iR typ. 2.0 MA
h typ. 2.0 mA
Notyp.
<8.5
10
dBdB
Lc typ. 5.5 dB
!) Standard test holder.
MilliardBAT59 Page 2
MICROWAVEMIXER DIODES
BAV22BAV22R
Coaxial Schottky barrier diodes for use in pre-tuned X- and S-band low noise mixer
circuits. The diodes are suitable as replacements for most British coaxial point contact
types in these bands, for example, GEM3, GEM4, CV7108, CV7109, CV2154 and
CV2155. They conform to the environmental requirements of BS9300 where applicable.
Available as a matched pair as 2/BAV22MR.
QUICK REFERENCE DATA
Operating frequency max. 12 GHz
Noise figure at X-band typ. 7.0 dB
at S-band typ. 6.0 dB
MECHANICAL DATA
Conforms to BS3934 SO-26
Unless otherwise stated, data is applicable to both types.
Dimensions in mm
02501a
Terminal identification
BAV22 Pin cathode
Body (red spot) anode
BAV22R Pin anodeBody (green spot) cathode
Note 1. The device is designed to make contact on this open face
Note 2. Cone tapers to a radius 0. 13 mm nominal
JUNE 1977Milliard
BAV22-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
Maximum peak pulse power
(9.375GHz, 0.5/iS pulse length) 1.0 WMaximum burn-out
multiple r. f. spikes, ANQ = ldB
5000 d.c. spikes,
Temperature
T rangestg
T , rangeamb °
ELECTRICAL CHARACTERISTICS (T&mb= 25°C)
N Noise figure (see note 1)
N Noise figure (at 3GHz)
v. s. w. r. Voltage standing wave
ratio (see note 2)- - 1.43:1
v. s. w. r. Voltage standing wave
ratio (at 3GHz) - 1.2:1
20 nj
0. 2 erg
35 nj
0. 35 erg
55 to +100 °C
55 to +100 °C
n. Typ. Max.
7.0 7. 5 dB
6.0 - dB
Z. f Intermediate frequency
impedance (see note 3) 300 - 550'if
NOTES
1. Measured at 9. 375GHz, 1mA rectified current, RL = 15fl. NQ includes Nif=1.5dB
with 45MHz intermediate frequency. BS9321/1406.
2. With respect to CV2154 holder at 9. 375GHz and 1mA rectified current, RL = 15fi.
BS9321/1409.
3. Measured at 9.375GHz, 1mA rectified current, RL = 15fi, i.f. = 45MHz. BS9321/
1405.
Milliard ^-^
MICROWAVEMIXER DIODES
BAV22BAV22R
— 20
iA)10jIfrlfT
/*>/
/s~ 2 4 6 8
VF (V)
IR (pA)
1
li 100-10 8 6 U 2
Vr(V)
TYPICAL D.C. CHARACTERISTIC
MilliardRAV22 - Page 3
OS86S
r*
c 500aai
E
U.*
~ 450
400
350
300 ,
D58S8
to•o
5 7.6O) I"•-
1in
1c 1
1 no
l
I
7.21
11
7.0
6.8
2.0 4.0
Rectified current I (mA)
2 4
Rectified current I (mA)
TYPICAL I.F. IMPEDANCEAGAINST RECTIFIED CURRENT
TYPICAL OVERALL NOISE FIGUREAGAINST RECTIFIED CURRENT
D5867
gE
- 4.0
o
l_
G 3.0in
_u_i
2.0
1.0
2X) 4.0
Rectified current I (mA)
TYPICAL LOCAL OSCILLATOR POWERAGAINST RECTIFIED CURRENT
35888
00o
z<3
+ 0.25
-0.25
-0.50
-0.75
-100 -50 50 100
Ambient temperature Tamb (*C)
TYPICAL CHANGE IN OVERALL NOISEFIGURE AGAINST TEMPERATURE
MilliardBAV22 - Page 4
BAV46
X-BAND MIXER/DETECTOR DIODE
Silicon Schottky barrier diode in DO-23 (1N23) outline specially designed for use in Doppler radar
systems and intruder alarms where low Vf noise and high sensitivity are required. May be used for
both mixer and detector applications.
QUICK REFERENCE DATA
Mixer mode
Voltage output for —90 dBm input power at X-band
1/, noise at a frequency 1 Hz to 1 kHz from carrier
Detector mode
Tangential sensitivity in bandwidth to 2 MHz
typ.
typ.
40 mV
1.0 mV
typ. —55 dBm
MECHANICAL DATACompatible with J.E.D.E.C. DO-23
Dimensions in mm
20.5
19.5
0l867o
A = concentricity tolerance = + 0.2
Terminal identification: diode symbol indicates polarity
Accessory: collet type 56321 (see page 4) converts BAV46 to DO-22 outline
c? Milliardr
February 1979
BAV46
RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC134)
Storage temperature range Tstg—20 to +100
Ambient temperature range for operation TamD —20 to +100
Reverse voltage Vr max. 2
Forward current lp wax. 10
CHARACTERISTICS (Tamb = 25 °C)
Forward voltage at lp =1 mA
Reverse current at Vr = 2 V
Mixer mode
Voltage output at X-band (notes 1 and 2)
1/fnoise (note 3)
Detector mode
Tangential sensitivity (note 4)
Video impedance (note 5)
VF
'R
vo
Nf
Nf
stssts
typ-
max.
mm.typ.
typ.
max.
mm.typ.
typ.
0.5
2
15
40
1.0
2.0
-52-55
850
OC
°C
V
mA
V
i"A
MVMV
J"V
MV
dBmdBm
Notes
1. Mixer operated with d.c. bias of 35 juA and r.f. bias of -18 dBm, giving a total bias of 42 juA.
2. Measurement made using Mullard CL8960 doppler radar module, output power 10 mW (typ.). The
input power to the mixer of -90 dBm is a signal 100 dB down on the output power from a typical
CL8960 with signal + noise at 18 dB (min.).
noise
A return signal, 100 dB down on radiated power, is equivalent to that achieved from a man target
of radar cross-section 1.0 m2 at a range of 15 m when operating the CL8960 with a 5 dB antenna.
February 1979
1r
Mullard V
X-band mixer/detector diode BAV46
Measurement circuit:
+7V
R1hookn
Y A.F. terminal
0BAV4.6 in
CL8960
Measurement amplifier
bandwidth 1 Hz to IkHz
Z iB >100kn
CI
~x
R2iokn
—o
MKJ
"\
N.B. a) The current lD should be approximately 35 nA with the Gunn device disconnected andapproximately 42 nA with the Gunn device operational and the antenna operating into
free space.
b) The coupling capacitor C1 should have a small impedance compared with Z;n.
3. Noise measured at a frequency 1 Hz to 1 kHz from carrier with a d.c. bias of 50 /iA.
4. Bandwidth to 2 MHz and a forward bias of 50 nA.
5. Measured with a forward bias of 50 ftA.
OPERATING NOTES
Care must be taken when making measurements that the precautions described in the operating notesare observed and that test equipment does not introduce transients.
1. The mixer diode has a low junction capacitance and may be damaged by transients of very shortduration. It is therefore recommended that soldering irons are isolated from the mains supplywhen soldering to the user's mixer a.f. terminals.
2. Precautions similar to those required for CMOS devices are necessary, namely:
(a) Earthed wrist straps should be worn.
(b) Table tops or other working surfaces should be conductive and earthed.
(c) Anti-static clothing should be worn.
(d) To prevent the development of damaging transient voltages, the device should not be inserted
or removed from the user's circuit with the d.c. power applied.
3. It is recommended that the user incorporates a mixer protection circuit. A suitable circuit consists
of two BA317 diodes connected in parallel but with one diode reversed, together with a parallel
10 nF capacitor. This circuit should be connected in close proximity to the mixer a.f. and earth
terminals and has been found to afford a suitable degree of protection.
4. A d.c. bias level of at least 30 pA must be maintained to ensure adequate mixer performance.It may be increased to 100 /xA without affecting sensitivity or noise level.
z> Milliard rFebruary 1979
BAV46
COLLET 56321 Dimensions in mm
6.35
6.25
7.42
f
6.35
6.25
All dimensions in mm5.05
"4.95D3H5
February 1979
Milliard Z!
X-Band mixer/detector diode BAV46
60Tangential
sensitivity
(-dBm)
55
50
45
40
35
30
isured at 10.68 GHzHz video bandwidth
n:10 20 30 40 50 60 70 80 90
D.C. forward bias(pA)
Videoimpedance
(fl)
10J
10J 10* 10
s
D.C. forward bias (jjA)
U MullardFebruary 1979 5
BAV72
MICROWAVE MIXER DIODE
Silicon Schottky barrier mixer diode for use in low noise mixer applications in Q-band. It conforms to
the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range
Noise figure
26 to 40
10
GHz
dB
MECHANICAL DATA Dimensions in mm
*2.2 1.63max
v1.5tf
0.38.0.25
2.001.80
A - concentricity
tolerance - ± 0.15
5.204.84
1.601.52
2\
J
1.631.68
0.380.25
OS23S
Terminal identification: red end indicates cathode
V MilliardJuly 1978
BAV72
max. 0.04 erg
max. 1.0 W-55 to +150 °C
-55 to +150 OC
RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC 134)
Burn-out (r.f. spike) (note 1
)
Burn-out, peak pulse power
Storage temperature range Tstg
Ambient temperature range Tamb
CHARACTERISTICS
Tamb = 25 C
Static
Reverse current (Vr = 0.5 V)
Forward current (Vp = 0.5 V
Dynamic
Noise figure (note 2)
Voltage standing wave ratio (note 3)
Intermediate frequency impedance (note 4)
Frequency range
Conversion loss (note 5)
Noise temperature ratio (note 6)
Notes
1. Local oscillator frequency = 9.375 GHz, number of pulses = 6 x 10^, pulse duration = 2 ns at half
peak energy, p.r.f. = 2000 p.p.s., load resistance = J2. Tamij= 25 °C.
2. Measured with a local oscillator frequency of 34.86 GHz, l = 0.5 mA, load resistance = 15 J2,
i.f. = 45 MHz, BS9300 No. 1406.
3. Measured with a local oscillator frequency of 34.86 GHz, l = 0.5 mA, load resistance = 15 SI,
BS9300 No. 1409.
4. Measured with a local oscillator frequency of 34.86 GHz, l = 0.5 mA, load resistance = 15 Si,
i.f. = 45 MHz, BS9300 No. 1405.
5. Measured at 34.86 GHz, 450 juW local oscillator power level and load resistance = 1 kft.
6. Measured at 34.86 GHz and i.f. = 45 MHz.
7. The diodes are measured in fixed tuned Q-band waveguide mounts. Details may be obtained from
Mullard Ltd.
'R max. 0.2 MAif min. 0.5 mA
No max. 10 dB
v.s.w.r. max. 1.8:1
Z|.f. min. 700 nmax. 1100 a
f min. 26 GHzmax. 40 GHz
Lc typ. 5.9 dB
N r typ. 1.4:1
July 1978
Mullard U
Microwave mixer diode BAV72
3.0
2.0
1.0
R,00d«2sn
10 2.0 3.0 40 Local oscillator power |mW)
Typical rectified current as a function of local oscillator power at 34.86 GHz
D«2Wa 16
1 1 1 1
« i.f.«45MHzN
jfr l.SdB
R|ooda 25a
31
1
1 U
g 1>o
I
12 1
1
1
I}
,
10 K>s.>^
8
200 400 600 800 1000 1200
Local oscillator power (jjW)
Typical overall noise figure as a function of local oscillator power at 34.86 GHz
Zf MilliardJuly 1978
MICROWAVEDETECTOR DIODE
BAV75
Silicon Schottky barrier diode in SO-86 outline, specially designed for use in
doppler radars where high detector sensitivity is required. It conforms to the
environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range 8. to 12 GHz
Tangential sensitivity (typ. ) with
100 jxA bias -50 dBm
OUTLINE AND DIMENSIONS
Conforms to B. S. 3934 SO-86
2.36m2.03
--
u
1 I
?
!
08 01.60 J
f'
01.60 03.1.52 3.
10
1.
1
98 1.52
1 |
1)0
-
1'
1.6 )
0.6
0.&
1__
2.21
^ 1.5 2 2.03
A : concentricity tolerance = +0 13
All dimensions in mm
H
JUNE 1978Milliard
BAV75 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
Peak pulse power (max. ) at 9. 375 GHz0.5 /is pulse length
Temperature
T rangestg
B
ambrange
0.75
-55 to +150
-55 to +150
W
ELECTRICAL CHARACTERISTICS (at T = 25 C)amb
Voltage standing wave ratio
(see notes 1,2, and 3)
Video impedance (see notes
4 and 5)
Tangential sensitivity (see
notes 1 and 2)
Flicker noise (see notes 4
and 6)
-49
typ.
211
310
-50
10 15
dBm
dB
NOTES
1. Measured at 10. 687 GHz with lOOuA forward bias.
2. Measured in a reduced height waveguide mount, (Sanders 6521, modified).
3. R. F. input power less than 5.0uW.4. Measured with 100 uA forward bias.
5. Maximum d.c. input voltage = l.OmV.
6. a) Measured at an i. f. of 1kHz with 50Hz bandwidth.
b) 1 /j noise remains constant with a forward bias not exceeding 250jiA.
D5406
£ 55
52
I |
1
1
1
1
1
1
1
to 2MHz video bandwidthForward bias = IOOjjA
Note : Device is tuned to a v. s.w.r.
of less than 2:1 at each frequencyf
4'
I
*L
Ns1
L
- \\
k
9 10 11 12
Frequency(GHz)
TANGENTIAL SENSITIVITY AS A FUNCTION OF FREQUENCY
MilliardBAV75 Page 2
MICROWAVEDETECTOR DIODE
BAV75
a 1800
o. 1600£
1400
1200
1000
800
600
400
200
ImV input (max)
-
50 100 150 200 250 300
D.C. forward bias (uA)
VIDEO IMPEDANCE AS A FUNCTION OF D. C. FORWARD BIAS
MilliardBAV75 Page 3
E 51
iH 49
5 47
45
43
41
39
37
35
33
i
1f
Ij
Measured at 10.687GHzin untuned holder.
to 2 MHz bandwidth
!
_t
!
11
I
7r|
/
//
r•
—
,
fi
50 100 150 200 250 300
D.C. forward bias (jjA)
TANGENTIAL SENSITIVITY AS A FUNCTION OF D.C. FORWARD BIAS
MilliardBAV75 Page 4
MICROWAVEMIXER DIODES
BAY96ABAY96BBAY96CBAY96D
A range of sub-miniature reversible low noise Schottky barrier mixer diodes. The
planar technology employed imparts a high degree of reliability and reproducability.
The metal -ceramic case is hermetically sealed and the devices conform to the
environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Maximum noise figure in X-band
BAV96A 7.5 dB
BAV96B 7.0 dB
BAV96C 6.5 dBBAV96D 6.0 dB
Unless otherwise stated , data is applicable to all types
OUTLINE AND DIMENSIONS
M.Q.M.
02.2max
.1.63
1.58
0.38.0.25
2.00
1.80
1.60
1.52
30*
i\
5.204.84
-1.63
1.58
0.380.25
All dimensions in mm A = concentricity tolerance = 10.15
Terminal identification: red end indicates cathode
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
Maximum burn out (see note 1) 15
0.15nj
erg
FEBRUARY 1978Mullard
BAV96A-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) (Contd.
)
Temperature
Tstg range -55 to +150 °C
Tamb range -55 to +150 °C
ELEC7TRICAL CHARACTERISTICS CTamb = 25°C)
NQ noise figure (see note 2) Mln. Typ. Max.
BAV96ABAV96BBAV96CBAV96D
v. s. w. r. (see note 3)
BAV96ABAV96BBAV96CBAV96D
Zif i. f. impedance (see note 4) 250
Sfg tangential sensitivity (see note 5)
Sts (see note 6)
7.0 7.5 dB6.5 7.0 dB6.0 6.5 dB5.5 6.0 dB
1.7: 1 2.0: 1
1.4: 1 1.6: 1
1.4: 1 1.6: 1
1.3: 1 1.5: 1
- 450 a
-52 - dBm
-54 - dBm
NOTES
1. Burn out is defined as the r. f. pulse energy necessary to cause ldB degradation
in noise figure when the diode is subjected to 2 x M)8 pulses of 2ns width.
2. Measured at 9. 375 ± 0. 1GHz. The noise figure includes i.f. amplifier contri-
bution of 1. 5dB, i.f. 45MHz, d. c. return for diode 15$2 max. , rectified current
1mA. BS9321/1406.
3. Measured in a reduced height waveguide mount under the same test conditions as
in note 2. BS9 321/1409.
4. I. F. = 45MHz, RL = 15S2, f = 9. 375 ± 0. 1GHz, IQ= 1mA. BS9321/1405.
5. Video bandwidth to 2MHz, 30^A bias. BS9322/1411.
6. Video bandwidth 1kHz to 1MHz, 30»iA bias. BS9322/1411.
7. A suitable holder for this diode is a modified version of Sanders type 6521.
Milliard£IAV96A-Page 2
MICROWAVEMIXER DIODES
s
s+aa
6-0.25
-as
0.75
psero
-100
BAY96ABAY96BBAY96CBAY96D
-50 50 100Tamb '*0
TYPICAL CHANGE IN OVERALL NOISE FIGUREAS A FUNCTION OF TEMPERATURE
05J71
1 *° ± / -* t£ ~]_
S _J
H J.8 £1 73 T
f_~1
£_
r
f~7
20 kO I (mA)
TYPICAL LOCAL OSCILLATOR POWERAS A FUNCTION OF RECTIFIED CURRENT
MullardBAV96A-Page 3
3 8.0
7.5
7.0
6.5
6.0
05872
11
1I
1
\
\<
I (mA)
TYPICAL OVERALL NOISE FIGURE AS A FUNCTION OFRECTIFIED CURRENT
<? 873
g 400
NI)
cO
| 350
It""
300
250
?nn
2.0 4.0 I (mA)
TYPICAL I. F. IMPEDANCE AS A FUNCTION OFRECTIFIED CURRENT
MilliardBAV96A-Page 4
MICROWAVEDETECTOR DIODE
BAV97
A reversible silicon Schottky barrier diode with excellent sensitivity and very low
1 noise. It conforms to the environmental requirements of BS9 300 where applicable.
J
The metal ceramic case is hermetically sealed.
QUICK REFERENCE DATA
Sj-g Tangential sensitivity (typ.
)
-54 dBm
- noise (typ.
)
10 dB
OUTLINE AND DIMENSIONS
M.Q.M.
02.2 -163.max 1.58
0.38.0.25
All dimensions in mm
2.001.80"
1.60
1.52
30*
i\
5.20
A s concentricity tolerance =20.15
J. 63
1.58
0.380.25
Terminal identification: red end indicates cathode
JUNE 1977Milliard
BAV97 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
Maximum burn out (see note 1)
Temperature
Tstg
range
T«mb
I* ,*e
ELECTRICAL CHARACTERISTICS (T = 25°C)amb '
S tangential sensitivity (see note- 2)
1_ noise (see note 3)
f
Z video impedance (see note 4) - 500
18
0.18 erg
-55 to +150 °C
-55 to +150 °C
Min. Typ. Max.
-52 -54 -58 dBm
- 10 15 dB
NOTES
1. Burn out is defined as the r.f. pulse energy necessary to cause ldB degradation
in noise figure when the diode is subjected to 2 x 10** pulses of 2ns width.
2. Video bandwidth to 2MHz, 50mA bias, f = 9.375GHz. BS9322/1411. (A2dBmimprovement in tangential sensitivity may be obtained by limiting the bandwidth
to 1kHz to 1MHz).
3. Measured at 30/iA bias, f = 1kHz, 50Hz bandwidth. 1^ noise is unchanged with
f
values of bias up to 150/xA.
4. Measured at 50fiA forward bias.
MullardBAV97 Page 2
MICROWAVEDETECTOR DIODE BAY97
on 74
impedance
Zv5
(fl)
10000
7
1000
100
100 1000D.C. forward bias (jiA)
VIDEO IMPEDANCE AS A FUNCTION OF D. C. FORWARD BIAS
MullardBAV97 Page 3
s.
— ffi M3ts
(dBm)
65
eo4 W ••».
t/
J55
fii -i
//
/i
|
50i)f f-i ,2 7!»e 13r
f
45
40
35
J
30 111
f
/?5 / .
20 40 GO 80 100
D.C. forward bias (jiA)
TANGENTIAL SENSITIVITY AS A FUNCTION OF D. C. FORWARD BIAS
MilliardEIAV97 Page 4
MICROWAVEMIXER DIODES
BAW95DBAW95EBAW95FBAW95G
A range of silicon Schottky barrier mixer diodes in reversible cartridge outline. -
The diodes are suitable as replacements for the 1N23 and 1N415 series and conform
to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Maximum noise figure at X-band
BAW95D 8.2 dB
BAW95E 7.5 dB
BAW95F 7.0 dB
BAW95G 6.5 dB
Unless otherwise stated , data is applicable to all types
OUTLINE AND DIMENSIONS
Compatible with J . E .D . E . C. DO- 22 with collet
Compatible with J.E.D.E.C. DO-23 without collet
1.2.382.34
r*\4.854.65
Q.75max.
T
—
05.6max
21.4
20.4
5.09
£.95
L_L
*.06.0
max.
,6.35'6.25
^_X
1.4
1.2
-07.527.42
A = concentricity tolerance =±0.2
All dimensions in mm. 04866
Terminal identification : Diode symbol indicates polarity.
JUNE 1977Milliard
BAW9SD-Page 1
LIMITING VALUES (Absolute max. rating system)
Electrical
Maximum peak pulse power (at 9. 375 GHz, 0. 5 its pulse length) 1.0 WMaximum burn out *) 20
0.2 erg
55 to +150 °C
55 to +150 °C
Temperature
Tstg range
Tamb 1*11^ELECTRICAL CHARACTERISTICS (Tamb = 25 °C
Min. Typ. Max.
N Noise figure 2)
BAW95DBAW95EBAW95FBAW95G
v.s.w.r. Voltage standing wave ratio ^)
zif Intermediate frequency impedance v 250
7.8 8.2 dB
7.2 7.5 dB
6.8 7.0 dB
6.3 6.5 dB
- 1.3:1
415 500 a
1)Burn out is defined as the r.f. pulse energy necessary to cause 1 dB degradation in
noise figure when the diode is subjected to 2 x 10& pulses of 2 ns width
2) Measured at 9.375 GHz, 1 mA rectified current, RL = 15 Q. N includes N|f = 1.5 dBwith 45 MHz intermediate frequency. BS9321/1406
3)With respect to JAN -106 holder measured at 9. 375 GHz, 1 mA rectified current,
RL - 15 Q. BS9321/1409
4) Measured at 9. 375 GHz. 1 mA rectified current, RL = 15 8 with 45 MHz intermediate
frequency. BS932 1/1405
MilliardBAW95D-Page2
MICROWAVEMIXER DIODES
t.o 2.0 3.0 4.0 5.0
Oscillator power (mW)
BAW95DBAW95EBAW95FBAW95G
5.0
Rectified
D2315
current
(mA)
4.0
3.0
2.0
1.0
n
TYPICAL RECTIFIED CURRENT AS A FUNCTION OF LOCAL OSCILLATOR POWER
ANIdB)
+0.5
-0.5-50 50 100 150
Operating temperature (*C)
TYPICAL CHANGE IN NOISE FIGURE WITH TEMPERATURE
MilliardBAW95D-Page 3
02313
Noise
(dB)
80 —
tf «*n_S ^ ^ • '<» m \** .
\- -___----= -BAW95E
r n _ _ _±_1.0 2.0 3.0 4.0
Rectified current (mA)
TYPICAL NOISE FIGURE AS A FUNCTION OF RECTIFIED CURRENT
D23U
l.F.
Impedance
(A)
500
400
300
1.0 2.0 3.0 4.0
Rectified current (mA)
TYPICAL DEPENDENCE OF I. F. IMPEDANCE ON RECTIFIED CURRENT
MilliardBAW95D-Page 4
BACKWARD DIODES
D
MICROWAVEDETECTOR DIODE
AEYI7
Sub-miniature germanium bonded backward diode primarily intended for broad- •
band low level detector applications at X-band. It conforms to the environmental
requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range 1 to 18 GHz
Typ. zero bias tangential
sensitivity in X-band -53 dBm
OUTLINE AND DIMENSIONS
V 2.S302.51max
'i:es
TT
XX = reference plane All dimensions in mmAA = concentricity tolerance =+ 0.15
-<-
02527a
TERMINAL IDENTIFICATION
The AEY17 is colour coded according to K1007 Issue 3, Section 1. 3. 4. 4.
That is: the positive end (cathode) is marked red and the negative end (anode is
marked blue.
The positive end indicates the electrode which becomes positive in an a. c. rectifier
circuit.
JUNE 1977Milliard
AEY17 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Temperature
T ^ max.stg
T min.stg
T . max.amb
T min.amb
ELECTRICAL CHARACTERISTICS (T =25°C)
150 °C
-55 °C
150 °C
-55 °c
Min. TyP- Max.
Static
lR Reverse current
V =0.3VK
lF
Forward current
V =0.3VF
Dynamic
Sts
Tangential sensitivity
(see note 1)
M Figure of merit
(see note 2)
ZV
Video impedance(see note 3)
120
100 - nA
12 - mA
-53 - dBm
300 - a
v.s.w.r. Voltage standing wave ratio - - 5:1
(see note 4)
Notes
:
1. Measured at 9.375GHz, zero bias, video bandwidth = 1.0MHz. K1007
Issue 3, Section 8B.4.3.
2. Measured at 9.375GHz, M is taken as the product of current sensitivity
expressed in ftAperfzW, and the square root of video impedance in ohms
.
K1007 Issue 3, Section 8B.4.2.
3. Zero bias, input l.OmV max. (d.c. or a.c. r.m.s.). K1007 Issue 3,
Section 8B.4.8.
4. With respect to50fi, measured at f = 9.375GHz, zero bias and c.w. input
power less than 1.0/xW. The nominal rectifier admittance at a reference
plane X-X taken at the end faces of the ceramic insulator (see outline
drawing on page 1) is
:
(2.0- j 2.0) -i- mho
Milliard —
—
AEY17 Page 2
MICROWAVEDETECTOR DIODE
AEYI7
APPLICATION INFORMATION FOR AEY17
1. Detector performance at other than Test Radio Frequency
Mln. Typ.
S. Tangential sensitity
f=1.0 to 18GHz, B = 1.0MHzts
v.s.w.r. Voltage standing wave ratio
f = 1.0 to 18GHz, Zo = 500
2. Mixer performance (I.F. =45MHz)
N„
*if
Measured overall noise figure
f = 9.375GHz, Nif= 1.5dB
PT ^ =200uW, I = 1.0mAL.O. out
f = 16.5GHz, Nif=1.5dB
PT = 200pW, I = 1.0mAL.O. out
I.F. impedance
I =1.0mAout
v.s.w.r. Voltage standing wave ratio
f=l to 18GHz, Zo =50C
I =1.0mAout
3. Doppler mixer performance (I.F. = 3kHz)
NQ Measured overall noise figure
f = 9. 375GHz, Nif= 2.0dB
-53
9.0
9.5
130
Max.
dBm
5:1
dB
dB
2.5:1
18 dB
MullardAEY17 Page 3
MICROWAVEDETECTOR DIODES
AEY29AEY29R
Germanium bonded backward diodes primarily intended for low level detector
applications at J -band (Ku band). The AEY29 and AEY29R are packaged in the
standard coaxial outline for this frequency band, similar to 1N78 types. Theencapsulation is hermetically sealed and the devices conform to the environmental
requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range 12 to 18 GHz
Typ. zero bias tangential sensitivity at J-band -53 dBm
MECHANICAL DATA
DO- 37
Unless otherwise stated , data is applicable to both types
Dimensions in mm
19.4.318.67
0**1*5.49'
-» D740S
A = concentricity tolerance = ± 0. 35
"These limits apply only over 10. 32 dimensions
TERMINAL IDENTIFICATION
AEY29 Pin cathode
Body (red) anode
AEY29R Pin anodeBody (green) cathode
OCTOBER 1978Milliard
AEY29-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Temperature
T . min.stg
T A max.stg
T , min.amb
T , max.amb
-55 °C
+85 °C
-55 °C
+85 °c
ELECTRICAL CHARACTERISTICS (T =25°C)amb
Min.Static
*RReverse current
V =0.3VK
JF
Forward current
V = 0.3VF
Dynamic
hs Tangential sensitivity
( see note 1
)
M Figure of merit
(see note 2)
ZV
Video impedance
( see note 3
)
v.s.w.r. Voltage standing wave ratio
(see note 4)
50
Typ.
100
12
-53
300
Max.
(LiA
mA
dBm
5:1
Notes
:
1. Measured at 16.5GHz in JAN201 holder, zero bias, 1.0MHz video band-
width. (K1007 Issue 3, Section 8B.4.3.).
2. Measured at 16.5GHz in JAN201 holder, M is taken as the product of
current sensitivity expressed in i*A per iXW, and the square root of
video impedance in ohms. (K1007 Issue 3, Section 8B.4. 2.).
3. Zero bias, input l.OmV max. (d.c. or a.c. r.m.s.). (K1007 Issue 3,
Section 8B.4. 8.).
4. With respect to JAN201 holder, measured at f = 16.5GHz, zero bias
and c. w. input power less than l.O^iW.
Milliard AEY29-Page 2
MICROWAVEDETECTOR DIODES
AEY3IAEY3IA
Sub-miniature germanium bonded backward diodes primarily intended for broad-band low level detector applications at X-band. It conforms to the environmental
requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range 1 to 18 GHz
Typ. zero bias tangential
sensitivity at X-band
AEY31 -53 dBm
AEY31A -50 dBm
Unless otherwise stated , data is applicable to both types
OUTLINE AND DIMENSIONS
02.2 -1.63.
max 1.58
t M0.38.0.25
All dimensions in mm
2.00' 1.80"
5.20U. Si.
1.60
1.52
30'
J. 63
'l.58
0.380.25
A = concentricity tolerance =10.15
TERMINAL IDENTIFICATION
The AEY31 and AEY31Aare colour coded accordingto K1007 Issue 3, Section 1. 3.4.4.That is: the positive end (cathode) is marked red and the negative end (anode) is
marked blue.
The positive end indicates the electrode which becomes positive in an a. c. rectifiercircuit.
JUNE 1977Mullard
AEY31-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Temperature
T . max.stg
T . min.stg
T . max.amb
T , min.amb
ELECTRICAL CHARACTERISTICS (T = 25°C)v amb
150vc
-55 °C
150 °C
-55 °C
Min.
Static
XR
Reverse current
VR=0.3V
lF
Forward current
V =0.3VF
namic
Sts
Tangential sensitivity
(see note 1)
AEY31AEY31A
M Figure of merit
(see note 2)
AEY31AEY31A
ZV
Video impedance(see note 3)
v.s.w.r. Voltage standing wave
Typ.
100
12
-53
-50
Max.
120
50
300
fiA
mA
dBmdBm
(see note 4) 5:1
Notes
:
1. Measured at 9.375GHz, zero bias, video bandwidth = 1.0MHz. K1007 Issue 3,
Section 8B.4.3.
2. Measured at 9.375GHz, M is taken as the product of current sensitivity expressed
in nA per ^tW, and the square root of video impedance in ohms. K1007 Issue 3,
Section 8B.4.2.
3. Zero bias, input l.OmV max. (d.c. or a.c. r.m.s.). K1007 Issue 3, Section
8B.4.8.
4. With respect to 50B, measured at f = 9.375GHz, zero bias and c.w. input power
less than l.OuW. The nominal rectifier admittance at a reference plane X-X taken
at the end faces of the ceramic insulator (see outline drawing on page 1) is
:
(2.0 J 2.0) — mho
MilliardAEY31-Page 2
MICROWAVEDETECTOR DIODES
AEY3I
AEY3IA
APPLICATION INFORMATION FOR AEY31 AND AEY31A
1 . Detector performance at other than Test Radio Frequency
Min. Typ.
S Tangential spnsitivitv
Max.
ngential sensitivity
f=1.0 to 18GHz, B=1.0MHz
AEY31 - -53 - dBmAEY31A - -50 - dBm
v . s .w . r . Voltage standing wave ratio
i = 1.0 to 18GHz, Z =50flo
2. Mixer performance (I.F. =45MHz)
N Measured overall noise figureo
f=9. 375GHz, N =1.5dBif
PT „ =200mW, I = 1.0mAL.O. out
f = 16.5GHz, N =1.5dBif
PT ^ =200nA, I = 1.0mAL.O. out
z I.F. impedance
I = 1.0mAout
v . s .w . r . Voltage standing wave ratio
f=l to 18GHz, Z =50fio
I =1.0mAout
3. Doppler mixer performance (I.F. =3kHz)
N Measured overall noise figureo
f = 9. 375GHz, N. =2.0dBif
9.0
9.5
130
5:1
dB
dB
2.5:1
18 dB
MilliardAEY31-Page 3
MICROWAVEDETECTOR DIODE
AEY32
Sub-miniature germanium bonded backward diode primarily intended for broadband -
low level detector applications in K-band and in Q-band (Ka-band). It conforms to
the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Frequency range 18 to 40 GHz
Zero bias current sensitivity
in the band 18 to 40 GHz (typ. ) 2.0 fiA/juW
OUTLINE AND DIMENSIONS
M.Q.M.
02.2 -1.63.
max 1.58
0.38.0.25
All dimensions in mm
2.001.80"
1.601.52'
30*
i\
5.20A. 84
A = concentricity tolerance =±0.15
J.63
1.58
0.380.25
Terminal identification: red end indicates Cathode
JUNE 1977Milliard
AEY32 Page 1
POLARITY IDENTIFICATION
The positive end (cathode) is marked red and the negative end (anode) is markedblue. The positive end indicates the electrode which becomes positive in an a.c.rectifier circuit.
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Max. pulsed r. f. input power(f = 9. 375GHz, t
p= 0. 5j*s , p. r. f. = 2000 p. p. s.
)
40 mW
Tamb ran«e
Tstg ran8e
ELECTRICAL CHARACTERISTICS
1/f noise (see note 1)
Swept v. s. w. r. (26. 5 to 40GHz)(see note 2)
Zy video impedance (see note 3)
Sj current sensitivity (see note 4)
M figure of merit (see note 5)
Min.
3.0
55 to +100 °C
55 to +100 °C
[yp. Max.
7.0 dB
5: 1
5.0 kn
.0 MA/^W
50
NOTES
1. Measured at an i.f. of 1kHz with 50Hz bandwidth and zero bias.
2. Measured in a Q-band broadband mount (Mullard specification 7313-731-0091).The v.s.w. r. measurement is swept over the band 26.5 to 40GHz at a powerlevel not exceeding lOOfiW and with zero bias.
3. Measured at an i. f. of 1. 6kHz with an input not exceeding lmV and with zerobias.
4. Measured in the same mount as described in note 2 at frequencies of 27GHz,34GHz and 40GHz , with an input power not exceeding 1/xW and with zero bias.
Rectified current measured by a microammeter of resistance less than 108.
5. Measured at frequencies of 27GHz, 34GHz and 40GHz. M is the product of currentsensitivity expressed in /iA//xWand square root of the video impedance expressedin ohms.
MullardAEY32 Page 2
MICROWAVEDETECTOR DIODE
AEY32
Current
sensitivity
Si
luA/iiW]
4.0
3.0
2.0
1.0
B*'
,«'*
.4*l
' »_ ilk4
•' %\ ,'
«•* u: :__,
r-
1* \
H1 »J tf
<*
f
20 25 30 35
Typical current sensitivity as a function of frequency
40Frequency GHz
til •(
Figure of —
M -
180 - + S~ -=
-- --
a - N *- :1 _ -V _
+*?v i \ --ifio *£ - + - - -i - J160
^r 3 / C 5C — -
—
A J V 4* 4- -* \ 1 f tz
-tf u I 3
HO _t_ JL _ _ ,-*__ _ _ _
J /J ,/
--£ton „ _ _«""_ ____
inn _ _20 25 30 35
Typical figure of merit as a function of frequency
Milliard
40Frequency GHz
AEY32 Page 3
VARACTOR DIODESMultiplier
Special purposeTuning
SILICON PLANAREPITAXIAL VARACTOR DIODE BAY96
Silicon planar epitaxial varactor diode for use as a high efficiency frequency multi-
plier in the v.h. f. and u.h. f. bands. As a tripler from 150 to 450 MHz it has a
typical efficiency of 64% and can handle inputs up to 40 W. The BAY96 has a very
low series resistance and is packaged in a low inductance, hermetically sealed,
welded ceramic -metal envelope, DO -4 with stud cathode. It conforms to the
environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
VR max.
Ptot max -
T- max.
Cr (VR = 6. V, f = 1. MHz)
Rs max. (VR = 6.0 V, f = 400 MHz)
at Vn = 120 V typ.2ttR. Or 'R
120 V
20 W175 °C
28 to 39 pF
1.2 Q
25 GHz
MECHANICAL DATA
Conforming to J. E.D.E.C. DO-4
Dimensions in mm
10-32UNF
t_ I
4,83max
...
1.98.,max
„ 11.5
10.7
Diameter of clearance hole : max. 5. 2 mmAccessories supplied on request:
56295 (PTFE bush, 2 mica washers, plain washer, tag)
56262A (mica washer, insulating ring, plain washer)
Supplied with device : 1 nut , 1 lock washer
Nut dimensions across th*» flats: 9. 5 mm
Torque on nut : min. 0. 9 Nmmax. 1. 7 Nm
MilliardAPRIL 1978 BAY96 Page 1
RATINGS
limiting values of operation according to the absolute maximum system.
Electrical
VR max. 120 V
ptot
max- ^mb = 25
°C> 20 W
Temperature
Tstg min. -65 °c
Tgtg max. 175 °C
Tj max. (operating) 175 °C
THERMAL CHARACTERISTIC
Rthj-mb 7.5 °C/W
ELECTRICAL CHARACTERISTICS
Min. Typ. Max.
Op Total capacitance
VR
= 6.0V, f = 1.0 MHz 28 - 39 pF
Rs Series resistance
Vr = 6.0V, f = 400 MHz - 0.9 1.2 Q
fco Cut-off frequency
VR = 120 V
1 - 25 - GHz2irR
g. Cj,
MullardBAY96 Page 2
SILICON PLANAREPITAXIAL VARACTOR DIODE
BAY96
APPLICATION INFORMATION
TYPICAL OPERATING CHARACTERISTICS AS A FREQUENCY TRIPLER
IB5646I
itLi L 3
Wf .} < 1 ji—'WRXJOO^—
o
ii <»-'flow)w l-Mt-^ >— c
sort. 50.n.
!> BAY> 96 I
sfc 100kA <> ^ 1
T2 *&
/7?77Fig1
Frequency tripler circuit - 150 to 450 MHz
L =6.5 turns 18 s.w.g. wire 0.297" I.D. 0.562" long
L =2 turns 14 s.w.g. wire 0.266" I.D. 0.312" long
L =l" x 0. 25" x 0. 020" copper strip 0. 562" from chassis
C «7.0 - lOOpF variable
C , C , C =2. - 13pF variable
C_ =2. - 25pF variable5
tj Efficiency
P. = 25W, f. =150 MHz
Min. Typ.
60 64
Milliard BAY96 Page 3
APPLICATION INFORMATION (cont'd)
n ! 1
1-
1-f-i * I
"+
j
BAY96 j |<
BS048(°/o)
!
I
i Mill M '
Frcaucncv triDter
,
|
150 to 450MMZ IT
^•"*L±**H ^ **^^
^ ^^^^S^
m*•*•
,1
•»
j
!
1! I
1 | i
j i
|
1!
I
J
!
1 jI [
i j j
on !
j I I : 1
10 20 30 40 Pin(W) 50
TYPICAL TRIPLER EFFICIENCY PLOTTED AGAINST INPUT POWERSee circuit on page 3
IB5649I
14-3
" ($/
413
128-6
All dimensions in mm.
COMPONENT LAYOUT OF TRIPLER CIRCUIT
Milliard BA.Y96 Page 4
SILICON PLANAREPITAXIAL VARACTOR DIODE
BAY96
rtot
(W)
25
20
15
10
50
B5654RAY96 _ ", *
5!SS8SS?C _*** $ & ^ v k«h *- m m> ^* *n yMM ««N- W ^«.^
«^ w ^ w ^^ w **hJ^
,m -»4«<r£*«»*.»««M -M»t.-»«l^
^^^^^^^^--^r--"--3 ^
$^lll?$$^#$^^^^^^ rr\! V*-^
;':':' $ $ ^ *| ^ Wf& W-* ::" £ A*: :- : *-:' ":" :
':
-
1
. V :: -^ '^\ '
fa
*** *H^»W*« *£ ^
^^^^^^^^^ii^^Lu^^^^«^-^Lji^^^-i: ...T..i .1..1 1 r--.-.ffv-fft-.lftll 1—I'll
50 100 150 mb CO
TOTAL DISSIPATION PLOTTED AGAINST MOUNTING BASE TEMPERATURE
Milliard BAY96 Page 5
IfIf(CIf
CC
-
-
-
-
- -
-
: O
ii
f
-
- -
- -
- -
- -
- -
- / N NXooH
*»aU)
a:
-
C>*
3n
I
2on
-
(Q
iv
o-
- -
- -
- -
- -
1
.
- -
-
- -
- -
-
-
K *» <*> k in n |n. m r>
§ <r£ "w§
TYPICAL DIODE CAPACITANCE AND SERIES RESISTANCE PLOTTEDAGAINST REVERSE VOLTAGE
Milliard BA.Y96 Page 6
SILICON PLANAREPITAXIAL VARACTOR DIODE
BAY96
c Tn i
i
i n l
r- BAY96 DUDOO(pF) V t MM! t^
"I -1-0MHZ
i
j
-4— i
:
1 —!
100-
i VR = 0-5V_^
j
I I I
-fI--
^+ +- —!
50 j1
~*~. I
-j j
- 11
1- 6-OV-f-H-i 1- ..(.
-I ;
j in Mil
I60Va- !
I
i
!
j
i
r>1
'
1 i 1 zb I MM50 100 150 200 Tj (°C)
R u^
_
:
|
]i
\"~
i
I I|
|
1
| BAY96 '
;
<n) -I i i
j
1
1-51
f» 400MHZT
| 1
!1
t r
rr r j_[
T... - ! ; M I ! 1
{
i-i- I,Vp = 6-OV
- _4_ !
! -T
'
i —l^j
!' i
-f-
10 1L ! ;
"*"
--++-,--
!
l!
i
!
I
j
I- + +-I
,
i ; j
i
I |
I
|
1
|
t
t; l ! ;
'
:f.E1
f
_4-- !
'^ -^-M-.
,
0-5 j1
L!
1'
|
! ;
Ii
I
i
!
\~l!
- J 1 !
I
it I
-
!. T'""
! :i
'
1
4- I
'
1
, ;xrr r~T;
; 1 T'i
! H+4- - 1 ! ;
- i
! ri
'
r> 1 ! 1
~'~| : : !
50 100 150 200 Tj (°C)
TYPICAL DIODE CAPACITANCE AND SERIES RESISTANCE PLOTTEDAGAINST JUNCTION TEMPERATURE
MilliardBAY96 Page 7
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY27
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics, -
especially suitable for use in frequency multiplier circuits up to ' S* band output
frequency.
It is a diffused silicon device and is mounted in a small double-ended ceramic-metal case with hermetic seal and conforms to the environmental requirements of
BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a frequency doubler 1 to 2 GHz in a typical circuit.
Pin
10 WPout
5-° WResistive cut-off frequency typ. (VR = 6.0V) 100 GHz
Total capacitance typ. (Vr = 6. V) 4. 5 pF
Tj max. 150 °C
OUTLINE AND DIMENSIONS
Heatsink/ end
/W1.52
1*2.08p 1.98
1 —
2.21 -j1
2.03 *
*
*\\ •
+ve
k.
^
-ve 0j-|O
*
1.63"*~1.52~*
Taf .
D5769
1
0.61_0.48"*'
«,_2.362.03
(83.10
A: concentricity tolerance = ±0.13
All dimensions in mm
JUNE 1977Milliard
BXY27 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V max.K
P4 4max. R.F..T . =£70°Ctot pin
T > 70°C , derating factorpin
Temperature
T , min.stg
T max.stg
T. max.J
THERMAL CHARACTERISTIC
Rx, . . max.th j-pm
ELECTRICAL CHARACTERISTICS (Tamb= 25°C )
(BR)R
I_
Reverse breakdown voltage
Reverse current
V =6.0VR
Cut-off frequency27TT C.
s ]
V =6.0VR
Total capacitance (C . + C )
V =6.0V, f = 1.0MHz
Stray capacitance
Series inductance
Min.
55
55
4.0
50
-55
150
150
20
Max.
50
3.0
Typ.
70
0.001 1.0
100
4.5
0.25
650
V
WmW/degC
°C
°C
°C
degC/W
6.0
MA
GHz
pF
pF
PH
Series resistance
VR=6.0V
Overall efficiency
P =10W, f. =1.0GHzin in
frequency doubler
frequency trebler
50
0.4
60
40
MilliardBXY27 Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE BXY27
<—M*1"i r ~i r
Pin
zi»-5on
I
#
*
B9931
—T— Jt—1—JL -
1GHz matching section Varactor mount
poutzout -50-a
2GHz bandpass -filter
APPLICATION INFORMATIONFREQUENCY DOUBLER CIRCUIT (1 to 2GHz)
MullardBXY27 Page 3
75
\(°/o)
70
65
60
55
50
45
40
!
J: 1 i
; ji i
''
'
' y-_-.L_L 1 '
1
I i
- ,'
i
'' i
1
:i
, 4-i ... 1 ! :
|
'
i-
:
'*-- a—
i—i-f-i -i 4m -
rl !
1
!.
4 - ,.---
r4-
, : ^ :
j
!i
I
-4- i --!--
i:
i'
! ; 1 ; :
.;..... 4-K-j-j-j.[T
jj
Tl !
' fjn-1.0GH2„T II,'
-TJ-rf!_[_, -4-4-4---
:ziil.. r ... j. .. 11
-M--f-
+-T-+-
4-4-4-
-f-*-4-
iri
a.r
.7^ *
—i.
!:
i !
-if j
"jj
_J | i
'
i-
1
i
!
1
I ,
j ''
; -- T • -t-
HJ 4 V
- * i-
1 1 l-ii-
r> tzj.;_Ljl-i.- t - - L L.„.I-
Hi -444 - {
. i ) ii 4-4-71 - -b
1
,
T "Tlrf !
;
j
1
t "i" r T"
!!
• ---f-t-T- -
4-+-I-£-
3*|--1
in-
i Aj
;
i
j
_ ]_ Ti/n -4-4
i Pi( _J i
-f-f- rPrl--+-
mTT" rn1
1 4—
I
-Htt..;.!_,.. u , ^ [
-r 4._4 !
1J j j .-i-.i-.t.I i
1-11 1:1
i
"1111 T.L.L1
i
i- •
\ \
'.
l
= \
Til-
:
'> _j
'
'
j
U-~fi.nt"
t:t:— * .; 4
T
: !
:
i ::j:-<-
n1 !
\
i i
r"i4 -
4j/_.
i !
1
-Mill -r
! \: -
44-1-1. !
!:
!"j
! |
i t]_l ~i ;
! -H 1:1-tift !
i
-4-t-~i -M-Mi HI1
Ii
T
1
1 I
! !
'
.
-i'
; W I
]
! -\ ! :
—
r
i
!
:
|
i1 ! _^ |
;
! ;
~\- -I- r-f- 44- -
iL i
t
;
- r | T-r- ~r~
'
j1 -tii-jL .-+. .4 -
T -;
:
! ! ^~~
!i
i
i
!1
-r— - 44-! j
1i
i j
; j 4.j ;
|
-4-' .|
:j 4 '
j
i !
>
1
!!
1! 1
1
i
-lirj_- _I-;..U-i
j
i
-
.1 4-U-. .-4 4 -
! :'
-
Tt"|T i
i
i \
j= ; 1 Mi i"
'
! : i ' :
i-u Lul l ;
!
I
! ! ji
:
ii i
~Tr
r1
1 ! !
, .;a .. 14, : : i
.1.-1+1:-U-1-1-.
i-!-.4-
~ 4 ~~~t"
|i
1\~T~
4tH"-;4
t
l-t-r-r--
~t'l t~! M-j-4- 4—4-
'tft 1 !
;::i::i-4- !
i~ -4-.l_.L-i--.
i?: 4
:
:.:i!: ii:|i- -M- 7
1
_U j_ _[ _.i_' | :
-j-1-4--fft"r-
-J L 4-t
w 4-t--i-i -
'Ti"X .1 44.4t:: {
-1-4j
-f.ffr. '[.:::. l
8 Pin(W) 10
OVERALL EFFICIENCY PLOTTED AGAINST INPUT POWERFOR DOUBLER OPERATION
MilliardBXY27 Page 4
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY28
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics ,
.
especially suitable for use in frequency multiplier circuits up to C-band output
frequency.
It is a diffused silicon device and is mounted in a small double-ended ceramic-
metal case with hermetic seal and conforms to the environmental requirements of
BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a frequency doubter 2 to 4 GHz in a typical circuit.
Pin 7-° W
Pout 3' 5 WResistive cut-off frequency typ. (Vr = 6.0 V) 120 GHz
Total capacitance typ. (VR = 6. V) 1.
5
pF
T, max. 150 °C
OUTLINE AND DIMENSIONS
+ve
5769
A; concentricity tolerance r +0.13
All dimensions in mm -
JUNE 1977Milliard
BXY28 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V max.R
P, 4 max. R.F. ,T . =£70°Ctot pin
T > 70 C , derating factorpxn
Temperature
T ^ min.stg
T x max.stg
T. max.J
THERMAL CHARACTERISTIC
n, . . max.th j-pm
ELECTRICAL CHARACTERISTICS (Tamb= 25°c)
(BR)RReverse breakdown voltage
Reverse current
V =6.0V
Cut-off frequency27TT C.
s ]
V =6.0V
Total capacitance (C. + C )
V =6.0V, f=1.0MHzR
Stray capacitance
Series inductance
Series resistance
V =6.0VR
Overall efficiency
P. =7.0W, f. =2.in m
frequency doubler
Min.
45
45 V
2.7 W34 mW/degC
-55 °C
150 °C
150 °C
30
Max.
80
1.0
Typ.
60
0.001 1.0
120
1.5
0.25
650
1.0
2.5
degC/W
HA
GHz
pF
pF
PH
50
Milliard BXY28 Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY28
Pin
Zin-5on
#-"i r ~i r
LU
BXY28
#
« ft*
-If*.
routZout -SOil.
r ___jL ,JL,
1
2GHz matching section Varactor mount 4GHz bandpass filter
APPLICATION INFORMATIONFREQUENCY DOUBLER CIRCUIT (2 to 4GHz)
MullardBXY28 Page 3
| | j
"1
|
,
bATiO >°"CO
1
i
"""! 1 1
'
'
1
Doubler operation 2 to 4GHz
f|n-2GHZ
'1
e/o)
-
70
65
- -,-'
60
55
-
50
45
i
8P;„(W)
OVERALL EFFICIENCY PLOTTED AGAINST INPUT POWERFOR DOUBLER OPERATION
Mullard BXY28 Page 4
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY29
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics,
especially suitable for high order frequency multiplier circuits up to X-band output
frequency.
It is a diffused silicon device and is mounted in a small double-ended ceramic-
metal case with hermetic seal and conforms to the environmental requirements of
BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a frequency quadrupler 2. 25 GHz to SI. GHz in a typical circuit :-
Pin ^ W
Pout °-3 W
Resistive cut-off frequency typ. (VR = 6. V) 120 GHz
Total capacitance typ. (VR = 6. V) 1.0 pF
Tj max. 150 <>C
OUTLINE AND DIMENSIONS
+ve
5769
A= concentricity tolerance = +0.13
All dimensions in mm
JUNE 1977Mullard
BXY29 Page 1
25 V
2.0 W
-55 °C
+150 °C
+150 °C
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V„ max.. nP^ max. R.F. (T . s=70°C)tot
xpin
'
Temperature
T ...min.
stg
T A max.stg
T. max.J
THERMAL CHARACTERISTIC
Rthj-pin max. 40 degC/W
ELECTRICAL CHARACTERISTICS W^b** 2500)
Mln. Typ. Max.
V Reverse breakdown voltage(BR)R
a =i. mA) 25 - - VK
I Reverse current
(V =6.0V) - 0.001 1.0 nAR
f Cut-off frequencyC° (V= 6.0V) (see note) 90 120 - GHz
R
Cj Total capacitance (C. + C )
(V =6.0V, f = 1.0MHz) 0.8 1.0 1.5 pFR
C Stray capacitance - 0.25- pF
L Series inductance - 650 - pHs
7j Overall efficiency
P, =1.0W, t =2. 25GHzin in
frequency quadrupler 30 - - %
Note . The cut-off frequency f is defined as
:
f -1
CO 27TT C.S ]
Where, Cj is the junction capacitance and is measured at 1.0MHz
rg is measured on a slotted line at 2. 0GHz.
MullardBXY29 Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY29
S-X BAND QUADRUPLES,
Outputtuningcapacitor
(C 3 )
Sliding short circuit
Variable idler capacitor (C2)
Idler circuit
(L 2 )
Inputimpedancetransformer
(LLC,) '
DiodeBXY29
Diode mount
View A-A
Reduced width waveguide
Input
2.25 GHz1 W o Output
9.0 GHz (Waveguide)
Approximate equivalent circuit
MilliardBXY29 Page 3
B0930
'1
Ouadrupler ODeration 2.25 to 9.0 GHz.<"/o)
f in =2.25 GHzfout=9.0 GHz
45
•
Typical -40
35
30
?50.5 1.0 1.5 P
jn(W)
OVERALL EFFICIENCY PLOTTED AGAINST INPUT POWERFOR QUADRUPLER OPERATION
MilliardBXY29 Page 4
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY32
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics, •
especially suitable for high order frequency multiplier circuits up to X-band output
frequency.
It is a diffused silicon device and is mounted in a small double-ended ceramic-metal case with hermetic seal and conforms to the environmental requirements of
BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a high order frequency multiplier 1 GHz to 10 GHz in a typical
circuit :-
Pin
500 mWP ,.
out20 mW
Resistive cut -off frequency typ. (VR = 6. V) 150 GHz
Total capacitance typ. (Vr = 6. V) 0.75 pF
T, max. 150 °C
OUTLINE AND DIMENSIONS
+ve
A: concentricity tolerance z +0.13
All dimensions in mm
JUNE 1977Mullard
BXY32 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V_, max.IV
PA A max. R.F. (T . ^70°C)tot
v pin
Temperature
T A min.stg
T A max.stg
T. max.]
20 V
1.6 W
-55 °C
+150 °C
+150 °C
THERMAL CHARACTERISTIC
R^, . . max.th j-pin
ELECTRICAL CHARACTERISTICS (Tamb= 25°c)
(BR)RReverse breakdown voltage
(I
R= 1.0mA)
Reverse current
(VR=6.0V)
Cut-off frequency
(V =6.0V) (see note)R
Total capacitance (C. + C )
(V =6.0V, f=1.0MHz)
cs
Stray capacitance
Ls
Series inductance
tt
Transition time
T Life time
Min.
20
100
Typ.
50
Max.
0.5
0.001 1.0
150
0.75
0.25
650
1.0
150
degC/W
HA
GHz
PF
pF
PH
ps
50
Note . The cut-off frequency f is defined as
:
CO
f =
—
i
CO 27TT C.s ]
Where, C* is the junction capacitance and is measured at I.OMH2
r„ is measured on a slotted line at 8.0GHz
MULTIPLIER PERFORMANCE
outf = 1.0GHz, P. =500mW,in in
f =10GHzout
Min.
15
Typ.
20
Max.
mW
MullardBXY32 Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE
BXY32
140
Pout
(mW)
120
100
80
60
40
20
I I I I
fjn = 1.63GHz
Pf-= 1.0W
f:_x«S
'In~«
in*>
f in x8 -
I I
10 12 fout
(GHz) 14
TYPICAL PERFORMANCE IN HIGH ORDERMULTIPLIERS
MullardBXY32 Page 3
li
! i 1' j__L4. 1
'
i
!
n -44-
4+-
'
:\
4±I4| i ;
-ftTT III!! ill 1
_„*£ - Multiplier' 4 1 A *"* /-I 1.
35operation 1 to 10 uriz
"t"!
'n...:..!_..
-r-4i4
1 Mi! "^Tl
Pout ut 10 ^HV i^^^L J4
. i_.._j
(mW) ii
;j 4
i!
1 M i 1 \.t .. .,_. L_,_,__l_ -L^----> 1
i
• T
rt44 -
V- * - - -t -H^-- - .^4-I
-+- -\2|
*~
i 1
|
;j 1
iT
30^
:!
i !—
i
1
: ;'
.14-:
i
..[._T;..l
! !
11 W
-fJ— -r-
!
!
ii
'
,.. j... j. ....... ..j.44- ~~xi
I
..
r
14_J_l._..^ __! l_ L~-._ _I !"!
;/ M, L . _. i- .._ . - h- --
r 1 J !
i i
1i
4+H 4- ..... ..j# i i j
25.!444-itti
! ^_ j/i
~"S- —
"i-
—1 j
-4 "3-•
_ .._|_.
jt_+. ..i ....
201
__J_ __. _. . - .„_ _H _t JLIJ- . - -— 1
!
i
j
i
I
!
15
1
! .
! !;
_| L..1,...
10 1
t ! , 1~
_j , i
|_ ji
1
1 i.
l „.. _4_ . ^4 -_ _
1
! 1
51
i
, [i
t I |
i
Mf
i
f~ ,
1
"j H~1
i
!
!
i
!
in 1'
+|
250 500 750 1000 Pin
( mW )
TYPICAL PERFORMANCE AS A FREQUENCYMULTIPLIER
MilliardBXY32 Page 4
yv
BXY35to
BXY41
SILICON VARACTOR DIODES
Silicon planar varactor diodes .exhibiting step recovery characteristics, especially suitable for use in
frequency multipliers. They conform to the environmental requirements of BS9300 where applicable.
B-XY35
Reverse breakdown
voltage
lR =10*iA
V(BR)R
Cut-off frequency
VR = 6V'co
Diode capacitance
VR -6VC
i
Transition time *tr
Storage time ts
Thermal resistance
junction to mounting
base, types A.D.E
Rth j-mb
Thermal resistance
junction to pin,
types B and C
Rth j-pin
MunfptiBr pelfofusance
Typical output
frequency range
Outlines available
mm.max.
max.
typ.
mm.max.
100
25
6.0
12
10
10
0.75
2
BXY36
70
75
4.0
6.0
500
150
20
20
BXY37
70
100
2.0
4.0
350
100
20
20
BXY38
50
120
1.2
2.0
300
75
30
30
BXY39
40
150
0.8
1.2
200
50
40
40
BXY40
25
180
0.4
0.9
150
50
50
50
8
10
BXY41
25
200 GHz
0.25
0.5
100
25
pF
PF
50 °C/W
50 °C/W
10 GHz14 GHz
B
CDE
Devices may be selected to suit
customers' specific requirements
Zl MilliardApril 1978
BXY35to
BXY41 yvMECHANICAL DATA
Outline ADO-4
Dimensions in mm
10-32UNF
* I
4>,83
max
max
. 11.5
10,7" -
Diameter of clearance hole: 5.2 mmAccessories supplied on request:
56295 (PTFE bush, 2 mica washers, plain washer, tag)
56262A (mica washer, insulating ring, plain washer)
Supplied with device: 1 nut, 1 lock washer
Nut dimensions across the flats: 9.5 mm
Torque on nut: min. 0.9 Nmmax. 1.7 Nm
Outline B Outline C
Heotsinkend
Cathode 05.97 Anode
05772
A= concentricity tolerance = +0.13
1,Ii
1
'
llt
R0.76min ^
t
9 2 31
I
399
V04.85max
2.39-
min
3.75max
7.25 __,.).02
11.8210-85 03242
April 1978
Mullard V
Silicon varactor diodes
Outline D
^V.Outline E
BXY35to
BXY41
t 3 - 12* 2.98
02.1max
A-
3-48 UNCthread
D7839
V 1.53
03243
0.66 40.36
T,1
801.50
1.621.53
0.2 5 max. _x45»chamfer A = concentricity tolerance =±0.13
U MullardApril 1978
SILICON VARACTORTUNING DIODES
BXY53BXY54BXY55
Epitaxial silicon varactor tuning diodes supplied in a standard microwave package. -<—
They conform to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Vr max.BXY53
60
BXY54 BXY55V
Op at -4V typ. 1.0 4.7 15 pF
Cto7m— mm. 4.0 6.5 7.0 pF
Unless otherwise shown , data is applicable to all types
OUTLINE AND DIMENSIONS
Conforms to B. S. 3934 SO-86
A: concentricity tolerance z +0.13
All dimensions in mm
Normal operation with reverse bias, i.e. heatsink end positive.
MilliardJUNE 1977 BXY53-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
VR
max. (see note 1 60 V
T=^ ran8estg
-55 to +175 °C
T max.case
125 °C
:TRICAL CHARACTERISTICS (at T = 25°C)amb '
BXY53 BXY54 BXY55
V(BR)R
(10^ min«> 60 60 60 V
I at 55V max.K
1.0 1.0 1.0 MA
C at -4V min. 0.8 3.7 12 PF
(see note 2) typ. 1.0 4.7 15 PF
max. 1.2 5.7 18 PF
Total capacitance ratio
CTOmin.
T60V4.0 6.5 7.0
Insertion loss (zero bias)
(see notes 3,4 and 5) max. 0.8 0.5 0.25 dB
Phase swing min. 80 85 63 degrees
(0 to 60V)
(see notes72 74 57 degrees
3, 4 and 5)
NOTES
1. At 25 C; below 25 C this figure must be derated at 7 x 10~ V/°C. Diodes with
different values of V. D are available on request.(BR)R
2. Capacitance tolerances of ±10% and lower are available on request.
3. Measurements made with the diode at the end of a 50J2 transmission line and with
small signal conditions.
4. Measured at 2.0GHz for BXY53 and BXY54; at 1.0GHz for BXY55. For values at
other frequencies see graphs on page 4.
5. The heatsink pin should be located in a hole of 1. 6 to 1. 65mm dia. The location
of the other end should be a hole of 1. 8 to 2. 2mm dia. , bearing on flange B witha force not exceeding 10 N.
APPLICATION NOTE
When designing tuning circuits at high frequencies it is not sufficient to specify acapacitance swing and loss resistance in the tuning varactor. The parasitic reac-tances of the microwave package have a significant effect on the terminal impedanceof the device. Although strictly speaking one must consider the entire circuit whenquoting impedance values the method of measurement adopted here has been foundto give values of useful accuracy in a variety of coaxial and waveguide test mounts.
MullardBXY53 - Page 2
SILICON VARACTOR BXY53TUNING DIODES BXY54
BXY55
APPLICATION NOTE (contd.)
One may 'simply take the measurements as giving values of r. f. impedance as a
function of bias for small signal conditions or they can be used as a more funda-
mental design aid. This is because the significant factors for the design of a micro-
wave varactor tuned circuit are the available phase swing in the circuit and the loss
incurred by the varactor. Both these quantities can be increased or decreased by
lowering or raising respectively the characteristic impedance of the circuit. Both
these quantities are also invariant under transformation down a uniform loss less
transmission line and apply whatever impedance is required to be presented by the
varactor circuit.
At large signal levels the r.f. swing may drive the varactor into forward conduc-
tion for part of the cycle. This has two effects, firstly there is a rectified voltage
built up on the varactor terminal and secondly the effective insertion loss rides at
low bias voltages. These effects are fundamental to any varactor diode.
Under forward d. c. bias conditions, the maximum bias current must not exceed
100mA or permanent damage may occur.
Mullard ^.^
DS891
Degrees
125
100 N *• ^ - . ,•* >vK \ / >
/^ v \ / \ B)/ \ \ / iLJ
Af s V r \
75 / * > L
/ s p\ \
/ ^k / \f \/ \ 1
/ / x ^
v50 / /\ \/ J' \ \/ r \ s,/ A
'v^ \/ > ' v \
25 -4' >
L \ BXYbA
s/* X s
_s>s s^ •s
fs^-^* s
n0.1
0.1
5 71.0
2 5 710
TYPICAL PHASE SWING AS A FUNCTIONOF FREQUENCY
Frequency(GHz)
35892
Insertion
loss
(dB)
>S^
0.5
-5*SNN
o^
*\^ v V BXVS5s
1.0
1.5
V BXY53>n
5 ' 1.0 2 5 7 10 2 Frequency (GHz)
TYPICAL INSERTION LOSS AS AFUNCTION OF FREQUENCY
MilliardBXY53 - Page 4
SILICONVARACTOR DIODES
BXY56BXY57
High efficiency silicon varactor diodes suitable for operation in low and high order -
multiplier circuits with output frequencies in the range 3 to 8 GHz. These diodes
are of the diffused epitaxial type, having mesa construction for optimum perform-
ance and conform to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
VBR(R) min' (JR= 10 **A min -
)
60 V
BXY56 BXY57
Cj (VR = 6 V) min. 1.5 2.5 pF
max. 2.5 3.5 pF
fc (VR = 6 V min.
)
160 140 GHz
Unless otherwise shown , data is applicable to both types
OUTLINE AND DIMENSIONS
Conforms to BS3934 SO-86
Heatsinkend
«1.60w1.52
A: concentricity tolerance - +0.13
All dimensions in mm
Normal operation with reverse bias , i. e. heatsink end positive.
JUNE 1977Milliard
BXY56-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
VD max.R
P max. (T, max. 50 C) (see note 1)tot
vhs
Rth
(J~hs > max -
T rangestg
T. max.J
CHARACTERISTICS (T . = 25°C)pin
BXY56 BXY57
60 60 V
5.2 6.6 W24 19 °C/W
-55 to +175 -55 to +175 °C
+175 +175 °C
V(BR)R
min ' (IR
= 10MA)
C . (V = 6V , f = 1MHz)(see note 2)
60 60
nun.
max.
fco"^ (VR -6V)
(see note 3)
tttyp. (transition time)
t typ. (lifetime)
Cs
typ.
Ls
typ.
MULTIPLIER PERFORMANCE (see note 4)
Low order multiplier efficiency in a
2. 1 to 4. 2GHz doubler
High order multiplier efficiency in a
0. 45 to 3. 6GHz 8 x multiplier
1.5 2.5 PF2.5 3.5 PF
160 140 GHz
150 200 ps
60 150 ns
0.25 0.25 PF
650 650 PH
60
20
NOTES
1. P P. -Ptot in out.
Derating curves are used for value of T. greater than 50 C:
Pto<
(W)
5.2
BXY56
permissiblearea pf operation'
50 175 T hs (°C)
Fig. 1
tot
(W)
6.6
BXY57
permissible
area of operation
'
50 175 T hs (°C)
Fig. 2
MilliardBXY56 - Page 2
silicon BXY56VARACTOR DIODES BXY57
NOTES (contd.
)
2. A particular diode specification within this range may be selected to suit the
application. Furthermore, it is recommended that devices are functionally tested
by the supplier in the customer* s circuit.
3. Cut-off frequency is measured using a slotted line system at 2GHz. f( 2*R
sCj
4. For high power applications it is essential that the heatsink end of the devices
is gripped by a collet or equivalent clamping system to ensure the best possible
thermal conductivity, this in turn should be coupled to an adequate heatsink.
Care must be taken to avoid unnecessary deformation of this diode pin, as this
may cause cracking of the metal -ceramic hermetic seal.
The location of the top cap should be a hole of diameter 1.8 to 2.2mm. bearing
on flange B with a force not exceeding ION.
MilliardBXY56 - Page 3
GALLIUM ARSENIDEVARACTOR DIODE
CAYIO
Gallium arsenide varactor diode with a high cut-off frequency for use in parametric
amplifiers , frequency multipliers and switches. The diodes are of the diffused
mesa type, are mounted in a small ceramic -metal case with a welded hermetic seal
and conform to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Vr max. 6.
IF (AV)max- 70
Ptot
max-Tstud
uP tol07 °C 50
for higher temperatures see derating curve
Operating temperature range -196 to +150
fc
typ. (VR = 6.0V) 240
V
mA
mW
°C
GHz
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO86
A 2.36* 2.03
a
1 l
02.
I t08 01.6098 1.52
1 1
r
^
-y
4
01.1.
1
50 03.52 3.
101. DO
}
1
1.63 _
1
f
0.61
0.48
2.21
1.5?"
2.03
A : concentricity tolerance = +0 13
All dimensions in mm
MARCH 1978Milliard
CAY10 Page 1
Limiting values of operation according to the absolute maximum system.
Electrical
V_, max.R
6.0 V
70 mAI max.F(AV)
P, max. (T , ^lO?^) 50 mWtot stud
Temperature
T min. ~196 cstg o
T _.max. +150 c
stg oT. (operating range) -196 to +150 C
ELECTRICAL CHARACTERISTICS (Tamb
= 25 C)
Min. Typ. Max.
Static
I Reverse currentR V =6 0V " °' 1 1 «° ^
R '
V Forward voltage dropF
I =1.0fzA (seenote3.) - 0.9 - VF
Dynamic
f Series resonant frequency°
Zero bias (see notes 1,2.) 8.9 10 11.6 GHz
f Cut-off frequencyCO
Zero bias 'see note 2.) 125 150 - GHz
f Cut-off frequencyC V =6.0V (see note 2.) 240 - GHz
C Effective diode capacitance
at X band frequency
Zero bias (see notes 1,2.) *0.3 0.4 0.5 pF
y Capacitance variation coefficient
Q (see note 3.) 0.12 0.15 -
C Stray capacitance (see note 1.) - 0.10 - pFSI
Cco Stray capacitance (see note 1.) - 0.15 - pF
L Series inductance (see note 1.) - 625 - pHs
Mullard CAY10 Page 2
GALLIUM ARSENIDEVARACTOR DIODE CAYIO
Notes
1 . A suitable lumped circuit equivalent for the device may be drawn as
follows
:
i
\
CS1 Cs2i
r
Cm=Ci+C,Rs ^m=*-j +^S2
fB57T71
2. Measurements at and about the series resonant frequency, in a suitable
waveguide holder, enable the values of fQ and the diode Q factor to bedetermined . The effective diode capacitance andthe cut -off frequency can
be calculated taking Lsto be the typical value.
f =Q £ where f is the series resonant frequencyco o00
and Q is the Q factor at zero biaso
andmo A 2* 2 T4jt f L
o s
3 . The capacitance variation coefficient 6 is defined as
I-C max. -C min.m m2(C max. + C min.)m m
where C min. = effective capacitance at V_ = 1.0Vm RC max. = effective capacitance at I_ = l.OjuAm F
Mullard CAYIO Rage 3
This can be re -written in the form
I = jl-V)"i-g'i
2{(l-V)^+ 2^}+ ^2]o
where V = V„ at l.OuAF
C. =C -o,„]o mo S2
Mullard CAYIO Page 4
GALLIUM ARSENIDEVARACTOR DIODE
CAYIO
D
o>-
<u
o«ji_
o Cv
'm p
F atow »-Q. O
2l0^ E
TOTAL DISSIPATION PLOTTED AGAINST STUD TEMPERATURE
Milliard -CAYIO Page 5
CXY10
GALLIUM ARSENIDE VARACTOR DIODE
Gallium arsenide varactor diode with a high cut-off frequency suitable for use in parametric amplifiers
and may be used in frequency multipliers and switches. The diodes are of the diffused mesa type,
mounted in a small ceramic-metal case with a hermetic welded seal and conform to the environmental
requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Vr max.
Ptot max.Tpin <25°C
Typical X-band parametric amplifier performance
Signal frequency
Gain
Bandwidth (3dB)
Noise temperature
6.0 V
50 mW
8.5 GHz
15 dB
70 MHz
200 °K
Dimensions in mmMECHANICAL DATA
Anode
Pressure to be Avoidavoided f lexing ofin this area Preferred area flange
of pressure
Compression force onmounting surfaces X-X & Y-Ymust not exceed 2.65N
U MilliardApril 1978
CXY10
RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC134)
Voltage
Continuous reverse voltage
Power dissipation
Total power dissipation (Tpjn < 25 °C)
Temperatures
Storage temperature
Junction temperature (operating range)
THERMAL RESISTANCE
From junction to pin
CHARACTERISTICS
Reverse current
VR = 6.0 V
Series resonant frequency
Vr = (note 1
)
Cut-off frequency
Vr = (note 1
)
Product of capacitance variation
coefficient and cut-off frequency
at Vr = V (note 2)
Microwave value of effective
device series resistance
(notes 1,4)
Microwave value of effective
device capacitance Vr = V(notes 3, 4)
Stray capacitance
(L.F. measurement)
Microwave value of effective
device series inductance
(note 3)
VR
Ptot
Tstg
6.0 V
50 mW
-196 to +175 OC
-196 to + 135 °C
Rth j-pin max. 0.9 0C/mW
TamD = 25 °C unless otherwise stated
Min. Typ. Max.
0.1 1.0"R
fr 27
7fco 35
30
200 350
50
2.25
0.2
0.3
140
AiA
34 GHz
GHz
GHz
ft
pF
- . pF
pH
April 1978
Milliard r?
Gallium arsenide varactor diode
Notes
1. Measured in a reduced height waveguide holder at Q-band.
2. yfc is guaranteed by a functional X-band paramp test at room temperature.
The capacitance variation coefficient, 7, is defined as follows:
7 V.
CXY10
Cm (max) - Cm (min)7=
2[Cm (max) + Cm (min)]
where Cm (min) = capacitance at Vr = 1.0 V
Cm (max)= capacitance at \f= 1.0 /iA
3. Cm is calculated using the frequency cut-off and the series resistance:
27rRmfco
Ls is also calculated using fres and Cn,:
1
Ls =
res um
4. (a) Diode circuit model.
(b) Equivalent circuit in measuring holder.
Not seen in
measuringholder
rzj—i
1
1
Lbd
±c's ±c
J^C r
08208 (a)
V MilliardApril 1978
CXY10
Operating note
The CXY10 varactor diode will give good noise performance in a parametric amplifier of suitable
design.
For example:
The effective input noise temperature of the amplifier, less the contribution due to the circulator,
would be typically 200 °K and a maximum of 250 °K, with the amplifier at room temperature
under the following conditions:
gain 15 dB
bandwidth 50 MHz (3 dB)
signal frequency in X-band
overcoupled ratio 4 to 5 dB
pump frequency in Q-band
In cooled parametric amplifiers, the device would give appropriately lower effective input noise
temperatures due to its low temperature working capability.
Devices and alternative encapsulations
may be selected to suit customers'
specific requirements
April 1978
Milliard C?
GALLIUM ARSENIDEVARACTOR DIODE CXYI2
Gallium arsenide varactor diode suitable for use in frequency multiplier circuits •
up to Q-band output frequency. The diodes are of the diffused mesa type, are
mounted in a small ceramic -metal case with hermetic welded seal and conform to
the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a frequency quadrupler 9 . GHz to 36 GHz in a typical circuit: -
Pin
max. 500 mWPout
mln ' 50 mWResistive cut-off frequency typ. (V^ = 6.0 V) 500 GHz
Tj max. 175 °C
OUTLINE AND DIMENSIONS
Anode
Pressure to be Avoidavoided flexing ofin this area Preferred area flange
of pressure
Dimensions in mm
Compression force onmounting surfaces X-X & Y-Ymust not exceed 2.45N
MARCH 1978Milliard
CXY12 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V max.RP max. (T . =25°C) (see note 1)tot
x pin
P. R.F. max.in
Temperature
T A min.stg
T x max.stg
T. max.J
10
300
500
-55
+175
+175
V
mWmW
°C
°C
°C
THERMAL CHARACTERISTIC
RiU .. . . max.th(j-pin)
ELECTRICAL CHARACTERISTICS (Tamb= 25°c )
(BR)RBreakdown voltage
I_, = 100nAK
Min.
10
Reverse current
V =6.0VXV
Series resonance frequency
V = 6 . 0V (see note 2) 27
Cut-off frequency
V = 6 . 0V (see note 2) 300R
Microwave value of effective
device capacitance V = 6 . 0V
(see note 3)
0.5 degC/mW
Typ. Max.
15 - V
0.001 1.0 nA
29 35 GHz
500
0.25
GHz
pF
Microwave value of effective
device series resistance
V =6.0V (see notes 2 and 4)R
Stray case capacitance
(L.F. measurement)
Microwave value of effective device
series inductance (see note 3)
1.3
0.3
120
PF
PH
MilliardCXY12 Page 2
GALLIUM ARSENIDE CXYI2VARACTOR DIODE
Notes
1. The maximum value of Ptot is based on a d.c. dissipation life test. The R.F.power may well exceed this figure in a practical circuit
.
2. Measurements on semiconductor devices at microwave frequencies are veryniuch
dependent upon the kind of holder used. The dynamic parameters are quoted using
a holder which takes the form of a double four section Q-band (Ka-band) 26 to
40GHz waveguide wide band low v.s.w.r. transformer to a reduced height of
0.25mm. The transformer is step down followed by step up in order to use standard
Q-band components on either side . A d . c . isolated coaxial choke system allows
the diode to be inserted across the 0.25mm reduced height section and to be
biased.
Using a swept frequency transmission loss measurement system, the series
resonant frequency and the Q of the diode holder system can be measured . Hencethe resistive cut-off frequency which is defined as Q x freg .
Separately, by measuring the transmission loss past the diode at resonance, the
effective diode series resistance can be found
.
3 . C is calculated using the frequency cut-off and the series resistancem
C =—±—m 2rfR fm co
L is also calculated using f and Cs res m
47r2f2
Cres m
MilliardCXY12 Page 3
4. (a) Diode circuit model.
(b) Equivalent circuit in measuring holder.
Not seenin measuringholder
a.
'Cm
(a)
6( b)
Application note
In a suitable frequency quadrupler , this device is capable of producing50mW at 36GHz for an input power of 400mW at 9.0GHz.
MilliardCXY12 Page 4
GALLIUM ARSENIDEVARACTOR DIODE
CXYI2
pout
(mW)
fjn= 9.0GHz
fout 36 QHZ80
A
A*
f_
2~2
a'
f
~i
,f~
~i_
A
£~i_
jf~40 y
~1
T/
a'
A~2
f£_
~2
f
/jjf
~1
j*~
f1/T 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
200 400 600 Pjn(mW)
OUTPUT POWER AGAINST INPUT POWERQUADRUPLER OPERATION
MilliardCXY12 Page 5
GALLIUM ARSENIDELIMITER DIODES
CXY22ACXY22B
Gallium arsenide varactor diodes for limiter applications from C to X-band. Very lowinsertion loss and high isolation characteristics may be obtained. The diodes are of thediffused mesa type and are mounted in standard microwave packages. They conform tothe environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Operating frequency range
GratOV (typ.)
Insertion loss* (typ.
)
High power attenuation* tfyp.)
*Depends on circuit configuration, see page 2
CXY22A
2.0 to 7.0
0.85
0.2
20
CXY22B
7.0 to 12
0.55
0.3
16
GHz
pF
dB
dB
Unless otherwise shown, data is applicable to both types.
OUTLINE AND DIMENSIONS
Conforms to B.S. 3934 SO-86
Heatsinkend
Dimensions in mm
05772
A= concentricity tolerance = ±0.13
MARCH 1978Milliard
CXY22A-Page 1
LIMITING VALUES (Absolute max. rating system)
rstg
range
max. 6.0 V
-55 to +150 °C
-55 to +100 °C
CXY22A CXY22B
max. 1.0 1.0 HA
typ. 0.85 0.55 pF
max. 1.45 1.45 V
typ. 1.0 1.2 £2
Tamb^S6
CHARACTERISTICS
IR atVR = 6 V
Op at VR = V, f = 1 MHz
Vp at IF = 50 mA
Rgat VR = V
TYPICAL X-BAND LIMITER USING CXY22B
This is a resonant circuit in rectangular waveguide, operating by reflection of a highpower input.
Centre frequency
Bandwidth (v. s. w.r. = 1. 2 : 1) at 1 mW max.
Insertion loss at 1 mW max.
Insertion loss at 100 mW (c. w.
)
Insertion loss at 5 W (pk), p.r.f. 1 kHz, 1 jzs
Safe peak power handling* , p.r.f. 1 kHz, 1 us
*Peak power handling depends on pulse length and duty cycle, as well as circuit design.
*o 9.4 GHz
**o 300 MHz
0.3 dB
6.0 dB
16 dB
50 W
/Section through
WG16
/Limiter diode
Circularcoupling post
Circular tuningcavity
D784S
A particular diode specification within this range should be selected to suit
a particular customer* s requirement. It is recommended that the diode is
functionally tested by the supplier, in the customer* s circuit.
Requests for devices in alternative packages will be considered by the supplier.
MullardCXY22A Page 2
GALLIUM ARSENIDEVARACTOR DIODES
CXY23ACXY23BCXY23CCXY23D
Gallium arsenide Schottky barrier diodes having a low series resistance and a wide
capacitance range. This ensures low losses with a wide tuning range in microwaveapplications. They conform to the environmental requirements of BS 9300 whereapplicable.
QUICK REFERENCE DATA
V(BR) R <min - > 12 V
VR (max.
)
12 V
Cj (at VR = 0V) (typ.
)
CXY23A 1.0 pFCXY23B '1.5 pFCXY23C 2.0 pFCXY23D 3.0 pF
(Development Nos. 821CXY/A, B, C and D)
Unless otherwise stated , data is applicable to all types.
OUTLINE AND DIMENSIONS
Conforms to BS 3934 SO-86
+ve -ve fl1 -60
5759
A= concentricity tolerance r +0.13
All dimensions in mm
MARCH 1978Milliard
CXY23A-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
VR (max.)*
TEMPERATURE
range
ELECTRICAL CHARACTERISTICS (at Tamb = 25 °Q
V(BR)R
Cj (VR = OV) CXY23A
CXY23B
CXY23C
CXY23D
Min.
12
65 to +150
Typ. Max.
°C
12 - - V
0.8 1.0 1.2 pF
1.2 1.5 1.8 pF
1.6 2.0 2.5 pF
2.5 3.0 3.5 pF
Capacitance ratio
Cj (VR = 0V)
Cj (VR = 12V)3.0: 1
R Q (VR = 0V) CXY23A
CXY23B
CXY23C
CXY23D
Pacakage capacitance
VR
0.2
3.0 a
2.0 Q
1.5 Q
1.0 J2
- pF
2 V
"Versions of these diodes with VR (max. ) up to 30V may be made available to special
order.
These devices may be supplied in alternative
packages to suit customers' specific requirements
MilliardCXY23A-Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODES
IN5I52
IN5I53
Silicon planar epitaxial varactor diodes exhibiting step recovery characteristics
,
especially suitable for use in frequency multiplier circuits up to S-band output
frequency. They conform to the environmental requirements of BS9300 where
applicable.
QUICK REFERENCE DATA
Operation as a frequency doubler 1.0 to 2.0 GHz in a typical circuit.
P. 12in
W
P 6.0rout
W
Typical resistive cut-off frequency (Vr = 6.0 V) 100 GHz
Typical total capacitance (VR = 6. V) 6. pF
Unless otherwise stated , data is applicable to both types
OUTLINE AND DIMENSIONS
OUTLINE DRAWING OF 1N5152
Heat sink
Cathode.+V(2
/end
^152 163152
1.9F-*
3.1_
3.0
l*±1.52
Anode'
2.362.03
0.61
0.48
"T2.21
2.03
-VC
OUTLINE DRAWING OF 1N5153
Anode
>
^7^
05.97
..k *~S ^Heat sinkCathode^ end
As concentricity tolerance « ±"0.13
All dimensions in mm D7840
JUNE 1977Mullard
1N5 152-Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V_, max.XV
P. . max. R.F.. (T . <70°C)tot pin — '
Temperature
T . min.stg
T . max.stg
T. max.J
THERMAL CHARACTERISTIC
R., .. . vmax.
th(j-pin)
ELECTRICAL CHARACTERISTICS (T = 25°C)* amb '
BR(R)
R
V_
Reverse breakdown voltage
(IR= 10M)
Reverse current
(VR= 60V)
Forward voltage
aF= 10mA)
Cut-off frequency
(V =6.0V, f = 2.0GHz)R measured
Total capacitance
(V =6.0V, f = 1.0MHz)XV
Overall efficiency
P. =12W, f. =1.0GHzin in
frequency doubler
Min.
75
55
5.0
50
75 V
5.0 W
-55 °C
+175 °C
+175 °C
20 degC/W
Typ. Max.
0.001 1.0 nA
1.0
100 GHz
7.5 pF
60
Milliard1N5152-Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE
IN5I55
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics ,
.
especially suitable for use in frequency multiplier circuits up to C-band output
frequency. It conforms to the environmental requirements of BS9300 where applic-
able.
QUICK REFERENCE DATA
Operating as a frequency tripler 2. to 6. GHz in a typical circuit.
Pin 5'° W
Pout2'° W
Typical resistive cut-off frequency (VR = 6. V) 120 GHz
Typical total capacitance (VR = 6. V) 2. pF
OUTLINE AND DIMENSIONS
Heotsinkend
+ve
A= concentricity tolerance = +0.13
All dimensions in mm
JUNE 1977Milliard
1N5155 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
V_ max.R
tot
Temperature
T . min.stg
T . max.stg
T. max.J
max. R.F. (T . <70°C)pm — '
THERMAL CHARACTERISTIC
R., ,. . . max.th(j-pin)
ELECTRICAL CHARACTERISTICS (T = 25°C)* amb
BR(R)
R
VF
fCO
Min.
35
Reverse breakdown voltage
(Ir=10mA)
Reverse current
(VR= 26V)
Forward voltage
(IF= 10mA)
Cut-off frequency
(V =6.0V, f = 2.0GHz) 100R measured
Total capacitance
35
3.0
-55
+175
+175
120
V
W
35 degC/W
Typ. Max.
0.001 1.0 nA
1.0
(V =6.0V, f=1.0MHz)
Overall efficiency
P. =5.0W, f. =2.in in
frequency tripler
1.0
GHz
3.0 pF
40
Milliard1N5155 Page 2
SILICON PLANAR EPITAXIALVARACTOR DIODE
IN5I57
Silicon planar epitaxial varactor diode exhibiting step recovery characteristics,
especially suitable for use in frequency multiplier circuits up to X-band output fre-
quency. It conforms to the environmental requirements of BS9300 where applicable.
QUICK REFERENCE DATA
Operation as a frequency doutder 5. to 10 GHz in a typical circuit.
Pin
2' 6 W
Pout 1-0 WTypical resistive cut-off frequency (VR = 6. V) 200 GHz
Typical total capacitance (VR = 6. V) 0.
8
pF
OUTLINE AND DIMENSIONS
+ve * W K52
A= concentricity tolerance = ±0.13
All dimensions in mm
0«7O
JUNE 1977MuHard
1N5157 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Electrical
VR max. 20 vPtot
max. R.F. (Tp
.
n<70°C) 2.5 W
Temperature
Tstg
min. _55oc
Tstg
max- +175 °C
T. max. +175 °c
THERMAL CHARACTERISTIC
Rth(j-pin)
maX - 38 - 5 degC/W
ELECTRICAL CHARACTERISTICS (T = 25°C)amb '
Mln. Typ. Max.
VTjr>/r»v Reverse breakdown voltageBR(R)
aR= 10MA) 20 - - v
IR Reverse current
(VR =16V)
- - o.l nA
V Forward voltage
(IF= 10mA) - - 1.0 V
f Cut-off frequency
(V 8 - 07'
fmeasured
=8 ' 0GHz) 18° 200 " GHz
C _ Total capacitance
(VR= 6.0V, f = 1.0MHz) 0.6 - 1.0 pF
Overall efficiency
P. =2.6W, f. =5.0GHzin m
frequency doubler 38
Milliard1N5157 Page 2
GUNN OSCILLATORS
X-BAND GUNNOSCILLATOR
CL83I0
QUICK REFERENCE DATA
Solid state oscillator featuring wide electronic
in local oscillators employing A. F.C. systems
tuning range. For application
Output connector WG . 16/WR.90
Centre frequency 9.4 GHz
Mechanical tuning range (min.
)
±50 MHz
Electronic tuning range (min.
)
200 MHz
Power output (typ.
)
5.0 mW
Operating voltage -7.0 V
Supplyvoltage
-7VO
—
Electronic tuning
BZY88 . _ J_ r|" ~ = -
-1
8V2 p"~l
10nF lJF___^j
Tuning
voltage
0A91
=i= 10nF
Gunn device
25max
Varactor diode
W.G. Plain flange
5985-99-083-0052
Mechanicaltuning
T
585DOD T
±5 f
31.5 ~J
i
1f
,6
_LL.2JAll dimensions in mm
JULY 1978Milliard
CL8310Page 1
OPERATING CONDITIONS
Supply voltage (see note) -7.0 V
Supply current 140 mA
Tuning voltage to -10 V
Tuning current 1.0 mA
out5.0 mW
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max
.
-8.0 V
Supply current max. running 200 mA
starting 250 mA
Tuning voltage max
.
-12 V
Tuning current max
.
2.0 mA
Load v.s.w.r. max. 1.5:1
CHARACTERISTICS at 25 C
Centre frequency
Mechanical tuning range
Electronic tuning range
*pout
Variation in P , overout
electronic tuning range
Electronic tuning sensitivity
Frequency temperature coefficient
Frequency pushing
9.4 GHz
Min. Typ. Max.
±50 - - MHz
200 250 - MHz
3.0 5.0 - mW
_ 1.5 _ dB
- 25 - MHz/V
- -1.0 - MHz/degC
- 30 - MHz/V
<P , min. measured under all conditions of tuning,out
TEMPERATURE
Range max.
OPERATING NOTE
-30 to +70
The active element will be damaged if the supply voltage is reversed. The oscillator
circuit provides some protection against forward transients greater than -8V but
care should be taken to avoid such transients as far as possible
.
MilliardCL8310 Page 2
X-BAND GUNNOSCILLATOR
CL8630
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator for operation in the 10. 7GHz hand. Applies
-
tions include all forms ot miniature radar systems.
Centre frequency 10,687 GHz
Power output (at TV) typical 8.0 mWFrequency temperature coefficient -0.25 MH?./°C
Output via square plain flange WC16. WR90. 5985-99 -083-0052
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v. s, w. r. max.
Starring current max.
Running current max.
+7.0 V
us: i
200 mA
160 mA
MullardMAY 1978 CL8630 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max.
Supply current max. running
starting
Load v.s.w. r. max.
CHARACTERISTICS at 25°C
Centre frequency
Power output (at 7. OV)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
A.M. noise to carrier ratio (1Hz to
1 kHz bandwidth)
Second harmonic
+7. 5 V
160 mA
200 mA
1. 5: 1
10.687 GHz
Min. Typ. Max.
5.0 8.0 - mW10.675 10.687 10. 699 GHz
- -0.25 -0.4 MHz/°C
- 1.5 - MHz/V
-94 dB
-35 dBm
TEMPERATURE
Range max. to-HlO
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care should
be taken to avoid transients in excess of 8 volts. An 8. 2V voltage regulator diode
to shunt the power supply is recommended for this purpose.
2. The minimum supply voltage is 6. 5V for the frequency of oscillation to remain
within the characteristic limits.
3. It is recommended that a small capacitor (e.g. 10nF)- is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4. Modulation of the supply voltage within the 1 Hz to 1 kHz bandwidth will degrade
the a. m. noise to carrier ratio as a result of direct conversion by the Gunn device
to both a.m. and f. m. noise components . The f.m. component may be demodulated
by the non -linear response characteristic of the associated detecting element.
MilliardCL8630 Page 2
X-BAND GUNNOSCILLATOR
CL8630
OUTLINE DRAWING
m i1.9naxii
i i ®- 441 .9
i—
max i
i' {&: ©j
4 holes
4J5positioned to
suit standard
W.G.16 flange
5.8
4.7
HE
H5
J6.8.max
-E. o
o+7V
n:
05538
MullardCL8630 Page 3
X-BANDGUNNOSCILLATOR
CL8630S
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator for operation In the 10 7GHz band as a self-
oscillating mixer (auto detector)
.
Centre frequency 10.637 GHz
Power output (at 7V) typical 8.0 mW
Frequency temperature coefficient -0.25 MHz/°C
Output via square plain flange WG16. WR90. 5)965-99-083-0052
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v.s.w.r. max.
Threshold current max.
Operating current max.
+7.0 V
1.5:1
200 mA
160 mA
MilliardMAY 1478 CL8630S Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max . (d . c .
)
Supply voltage max. (for less than 1ms)
CHARACTERISTICS at 25°C
Centre frequency
Power output (at 7.0V)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
Output voltage for input 66dB down
on output power (at 12 dB min.
signal + noise
noise
Second harmonic
Threshold current
Operating current
TEMPERATURE
Range max.
+7.5 V
+9.0 V
10.687 GHz
Min. Typ. Max.
5.0 8.0 - mW10.675 10.687 10.699 GHz
- -0.25 -0.4 MHz/°C
_ 4.0 - MHz/V
80 120 - mv
-35 - dBm
- 200 mA
120 160 mA
to +40
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care
should be taken to limit transients. An 8.2V 5% voltage regulator diode to shunt
the power supply is recommended for this purpose
.
2. The minimum supply voltage is 6.5V for the frequency of oscillation to remain
within the characteristic limits
.
3. It is recommended that a smallcapacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply
.
4 . A return signal 66dB down on radiated power will be achieved from a man target
of radar cross-section 1.0m2 at a range of 12m, when operating with an antenna
gain of 20dB.
5. System bandwidth 1Hz to 1kHz.
6. Power supply ripple in the amplifier passband will degrade the signal to noise
performance
.
MullardCL8630S Page 2
X-BAND GUNNOSCILLATOR
CL8630S
OUTLINE DRAWING
4 holes
4.45
4.35
positioned to
suit standard
W.G.16 flange
5.8
4.7J 6.8.
max
-E. o
o+7V
TV
D5538
MilliardCL8630S Page 3
a.f. output -•
+ 13.8V
O -ve
Gunn oscillator
VR is used to set voltage at 7.0V across Gunn oscillator.
CIRCUIT USED FOR SENSITIVITY MEASUREMENT
MilliardCL8630S Page 4
X-BAND GUNNOSCILLATOR
CL8631
QUICK REFERENCE DATA
Fixed frequency Guim oscillator for operation tn the 9. 35Gllz band,
tions Include all forms of miniature radar systems.
Applies -
Centre frequency 9. 35 GHz
Power output (at 7V) typical B.O raW
Frequency temperature coefficient -0. 25 MHzy°C
Output via square plain flange WG16. WR90, 5985-99-083-0052
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v.s.w.r. max.
Starting current max..
Running current max
+7. V
1.5: 1
200 mA
160 mA
MullardMAY 1978 CL8631 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max.
Supply current max. running
starting
Load v. s.w.r. max.
CHARACTERISTICS at 25°C
Centre frequency
Power output (at 7. OV)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
A. M. noise to carrier ratio
(1Hz to 1kHz bandwidth)
Second harmonic
TEMPERATURE
Range max.
OPERATING NOTES
+7.5 V
160 mA
200 mA
1.5: 1
9.35 GHz
Min. Typ. Max.
5.0 8.0 - mW
9.338 9.35 9.362 GHz
- -0.25 -0.4 MHz/degC
- 1.5 - MHz/V
-94 dB
-25 dBm
to +40 °C
1. The active element will be damaged if the supply voltage is reversed. Care
should be taken to avoid transients in excess of 8 volts. An 8. 2V voltage reg-
ulator diode to shunt the power supply is recommended for this purpose.
2. The minimum supply voltage is 6. 5V for the frequency of oscillation to remain
..within the characteristic limits.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4. Modulation of the supply voltage within the 1Hz to 1kHz bandwidth will degrade
the a. m. noise to carrier ratio as a result of direct conversion by the Gunn
device to both a. m. and f . m. noise components.
MilliardCL8631 Page 2
X-BAND GUNNOSCILLATOR
OUTLINE DRAWING
41.9max
4 holes
{/* t
»
i
f©-©> positioned to
suit standard
41.9W.G. 16 flange
max
]'
(©• -©J
CL8631
5.8
4.7
.19.5.
max
-Eo
o+ 7V
D5541
MilliardCL8631 Page 3
X-BAND GUNNOSCILLATOR
CL8631S
QUICK REFERENCE DATA
Fixed frequency Gumi oscillator for
oscillating mixer (auto detector).
operation in the 9. 3SGHz band as a self-
Centre frequency 9.35 GHz
Power output (at 7V) typical 8.0 mW
Frequency temperature coefficient -0.25 MHz/OC
Output via square plain flange WG16, WR90. 59R5-99-OR3-0O52
OPERATING CONDITIONS
Supply voltage {see operating notes)
Load v. s. w. r. max.
Threshold current max.
Operating current max.
+7.0 V
LS: 1
200 mA
160 mA
MullardMAY 1978 CL8631S Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max. (d. c.
)
Supply voltage max. (for less than 1ms)
CHARACTERISTICS at 25°C
Centre frequency
+7.5
+9.0
9.35
Output voltage for input 66dB down
on output power (at l2dB min.
signal + noise80
to +40
GHz
Min. Typ. Max.
Power output (at 7. 0V) 5.0 8.0 - mW
Frequency (fixed) 9.338 9.35 9.362 GHz
Frequency temperature coefficient - -0.25 -0.4 MHz/°C
Frequency pushing - 4.0 - MHz/V
ZU " HV
25 - dBm
- 200 mA
20 160 mA
noise
Second harmonic
Threshold current
Operating current
TEMPERATURE
Range max.
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care
should be taken to limit transients. An 8. 2V 5% voltage regulator diode to shunt
the power supply is recommended for this purpose.
2. The minimum supply voltage is 6. 5V for the frequency of oscillation to remain
within the characteristic limits.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4. A return signal 66dB down on radiated power will be achieved from a man target
of radar cross-section 1.0m2 at a range of 12m, when operating with an antenna
gain of 20dB.
5. System bandwidth 1Hz to 1kHz.
6. Power supply ripple in the amplifier passband will degrade the signal to noise
performance.
MullardCL8631S Page 2
X-BAND GUNNOSCILLATOR
OUTLINE DRAWING
41.9max
4 holes
^•"»i
r©- -©> positioned to
suit standard
41.9W.G.16 flange
max
1 ' w -©J
CL8631S
05541
MilliardCL8631S Page 3
T -0+13.8V
33H
a.f. output -*-
BFY52 (>10nF==
IOOuFS
470A
VR1250A r ^pre -set (±\ BZY88
1 I
1.2 k£l
C8V2
-O -ve
Gunn oscillator
VRi is used to set voltage at 7.0V across Gunn oscillator.
CIRCUIT USED FOR SENSITIVITY MEASUREMENT
MullardCL8631S Page 4
X-BAND GUNNOSCILLATOR
CL8632
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator for operation In the 9. 47GHz hand. Applica-
tions include all forms of miniature radar systems.
Centre frequency 9.47 OHb
Power output (at 7V) typical 8.0 mW
Frequency temperature coefficient -0, 2S MHz/°C
Output via square plain flange WGI6. WR90. 59B5 -99-083-0052
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v. s.w. r. max.
Starting current max.
Running current max.
+7,0 V
1.5: 1
200 rnA
16Q mA
MAY 1978Milliard
CLS632 Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max.
Supply current max. running
starting
Loadv.s.w. r. max.
•CHARACTERISTICS at 25°C
Centre frequency
Power output (at 7.0V)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
A.M. noise to carrier ratio
(1Hz to 1kHz bandwidth)
Second harmonic
+7.5 V
160 mA
200 mA
1.5: 1
9.35 GHz
Min. Typ. Max.
5.0 8.0 - mW9.458 9.47 9.482 GHz
- -0.25 -0.4 MHz/degC
- 1.5 - MHz/V
-94 dB
-25 dBm
TEMPERATURERange max.
OPERATING NOTES
Oto+40
1. The active element will be damaged if the supply voltage is reversed. Care should
be taken to avoid transients in excess of 8 volts. An 8. 2V voltage regulator diode
to shunt the power supply is recommended for this purpose.
2. The minimum supply voltage is 6.5V for the frequency of oscillation to remain
within the characteristic limits.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4. Modulation of the supply voltage within the 1Hz to 1kHz bandwidth will degrade
the a.m. noise to carrier ratio as a result of direct conversion by the Gunndevice to both a.m. and f. m. noise components.
MilliardCL8632 Page 2
X-BAND GUNNOSCILLATOR
CL8632
OUTLINE DRAWING
41.9max
W41.9max
\®:
-<±f-
©
4 holes
w4.35
positioned to
suit standard
W.G.16 flange
5.84.7
05541
MilliardCL8632 Page 3
X-BAND GUNN CL8632SOSCILLATOR
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator for
oscillating mixer {auto detector).
operation in the 9 .47GI11-. band as a self-
Centre frequency 9.47 QHs
Power output (at 7V) typical 8.0 mW
Frequency temperature coefficient -0.2S MHz/°C
Output via square plain flange WG16 WR90. 5985-99-083-0052
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v.s.w.r. max,
Threshold current max.
Operating current max.
+7.0 V
1.5:i
200 MlA
1G0 mA
MullardMAY 1978 CLB632S Page 1
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max . (d . c.
)
+7.5 V
Supply voltage max . (for less than 1ms) +9.0 V
•CHARACTERISTICS at 25°C
Centre frequency 9.47 GHz
Min. Typ. Max.
Power output (at 7.0V) 5.0 8.0 - mWFrequency (fixed) 9.458 9.47 9.482 GHz
Frequency temperature coefficient - -0.25 -0.4 MHz/°C
Frequency pushing - 4.0 - MHz/V
120 - MV
-25 - dBm
- 200 mA
120 160 mA
to +40 °C
Output voltage for input 66dB downon output power (at 12dB min.
signal + noiseffl
noise
Second harmonic
Threshold current
Operating current
TEMPERATURE
Range max.
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care
should be taken to limit transients. An 8.2V 5% voltage regulator diode to shunt
the power supply is recommended for this purpose
.
2 . The minimum supply voltage is 6 . 5V for the frequency of oscillation to remain
within the characteristic limits
.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4 . A return signal 66dB down on radiated power will be achieved from a man target
of radar cross-section 1.0m2 at a range of 12m, when operating with an antenna
gain of 20dB
.
5. System bandwidth 1Hz to 1kHz.
6 . Power supply ripple in the amplifier passband will degrade the signal to noise
performance
.
MilliardCL8632S Page 2
X-BAND GUNNOSCILLATOR
CL8632S
OUTLINE DRAWING
41.9max
i
f©- &41.9max
'[© ©J
4 holes
w4.35
positioned to
suit standard
W.G.16 flange
05541
MilliardCL8632S Page 3
a.f. output -»
10nF
0+13.8V
O -ve
Gunn oscillator
VR1
is used to set voltage at 7.0V across Gunn oscillator.
CIRCUIT USED FOR SENSITIVITY MEASUREMENT
MullardCL8632S Page 4
X-BAND GUNNOSCILLATOR
CL8633
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator for operation in the 10.5GHz band. Applica-
tions include all forms of miniature radar systems.
Centre frequency
Power output {at 7V} typical
Frequency temperature coefficient
Output via square plain flange WG1S, WR90. 5985-99-083-0052
10.525 GHz
8.0 mW-0.25 MHz/°C
OPERATING CONDITIONS
Supply voltage (see operating notes)
Load v.s.w.r- max.
Threshold current max.
Operating current max.
+7.0 V
i.5:i
200 mA
160 mA
MilliardMAY 1978 CLS633 Page 1
Min. Typ. Max.
5.0 8.0 - mW10.513 10.525 10.537 GHz
- -0.25 -0.4 MHz/°C
- 4.0 - MHz/V
-94 dB
-35 dBm
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max. (d.c.
)
+7.5 V
Supply voltage max.
(for less than lms) +9.0 V
CHARACTERISTICS at 25°C
Centre frequency 10.525 GHz
Power output (at 7 . V)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
A.M. noise to carrier ratio (1Hz to
1kHz bandwidth)
Second harmonic
TEMPERATURE
Range max. to +40 °C
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care should
be taken to limit transients. An 8. 2V 5?L voltage regulator diode to shunt the
power supply Is recommended for tills purpose.
2. The minimum supply voltage is 6.5V for the frequency of oscillation to remainwithin the characteristic limits.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation which
may occur in the power supply.
4. When used in aDoppler radar system, modulation of the oscillator supply voltage
will degrade the a.m. signal to noise ratio at the output of the associated mixer,
as a result of direct conversion by the Gunn device to a.m. and f.m. noise
components. The a.m. component will contribute directly and the f.m. componentmay contribute from demodulation by the slope of the bandpass characteristic of
the mixer.
5. Second harmonic level is measured into a W.G.16 load with a v.s.w.r. <1.1:
1
at fundamental frequency. The level is equivalent to that radiated from a low
v.s.w.r. X-band antenna, for example, Mullard ACX-01A.
MilliardCL8633 Page 2
X-BAND GUNNOSCILLATOR
OUTLINE DRAWING
iU.9nax
4 holesr
^/ *435,
t . %- $ positioned to
suit standard
41.9j
— W.G.16 flange
max!
' 1 if- 4
CL8633
5.8
4.7^.16.8.max
-Eo
o+7V
n05538
MullardCL8633 Page 3
X-BAND GUNNOSCILLATOR
CL8633S
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator fur operation in the 10 5GJI^ hand as a sclf-
oscillating mixer (auto detector).
Centre frequency KK523 omPower output (at 7V) typical 8.0 raW
Frequency temperature coefficient -o.zr> MH/./^C
Output via square plain flange WGlfi wnuo, r iS EJ-99-083-0052
OPERATING CONDITIONS
Supply voltage {see operating notes)
Load v , s .w . r . mux .
Threshold current max.
Operating current max.
+7.0 V
1 .5:1
200 mA
160 mA
MullardMAY 1978 CL8633S Page 1
+7.5 V
+9.0 V
10.525 GHz
Min. Typ. Max.
5.0 8.0 - mW10.513 10.525 10.537 GHz- -0.25 -0.4 MHz/°C
- 1.5 - MHz/V
120 - MV
-35 - dBm- 200 mA
120 160 mA
RATINGS (ABSOLUTE MAXIMUM SYSTEM) at 25°C
Supply voltage max . (d . c.
)
Supply voltage max. (for less than 1ms)
CHARACTERISTICS at 25°C
Centre frequency
Power output (at 7 . 0V)
Frequency (fixed)
Frequency temperature coefficient
Frequency pushing
Output voltage for input 66dB downon output power (at 12dB min.
signal + noise
noise 80
Second harmonic
Threshold current
Operating current
TEMPERATURE
Range max
.
to +40 °C
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Careshould be taken to limit transients . An 8 . 2V 5% voltage regulator diode to shuntthe power supply is recommended for this purpose.
2. The minimum supply voltage is 6.5V for the frequency of oscillation to remainwithin the characteristic limits
.
3. It is recommended that a small capacitor (e.g. lOnF) is connected across the
oscillator supply voltage terminals to suppress low frequency oscillation whichmay occur in the power supply.
4 . A return signal 66dB down on radiated power will be achieved from a man target
of radar cross-section 1.0m2 at a range of 12m, when operating with an antennagain of 20dB.
5. System bandwidth 1Hz to 1kHz.
6 . Power supply ripple in the amplifier passband will degrade the signal to noiseperformance
.
MilliardCL8633S Page 2
X-BANDGUNNOSCILLATOR
OUTLINE DRAWING
iU.9nax
U holesr ^ 435,
i i % Or positioned to
suit standard
41.9j
— W.G.16 flange
max!
'' w 4
CL8633S
5.8
4.7J6.8.max
-E. o
o
+7V
D5538
MilliardCL8633S Page 3
33H
a.f. output -*-
BFY52 Q-ioouf:
" F
f~ff 1 V
T -0+13.8V
470fl
VR125011/\J 250n >»-"v
T 1.2 kn
4-\ BZY88C8V2
Gunn oscillator
VR is used to set voltage at 7 . OV across Gunn oscillator
.
CIRCUIT USED FOR SENSITIVITY MEASUREMENT
MilliardCL8633S Page 4
X-BAND GUNNOSCILLATOR
CL8640RCL8640T
Mechanically and electronically tuned Gunn -effect oscillators In the 10. 5GHz band.
The high Q cavity offers frequency stability compatible with application as the
transmitter (CL8640T)and receiver local oscillator (CL864GR) in short range data
link systems.
QUICK REFERENCE DATA
CL8640R CL8640T
Centre frequency 10.49 10. 56 GHz
Mechanical tuning range min. 120 120 MHz
Electronic tuning range min. 30 8.0 MHz
Power output typ. 6.0 6.0 mWOperating voltage -7.0 -7.0 V
Output via square plain flange WC. 16.WR90. 5985-99-083 -0052
CLS640R - receiver local oscillator
CL8640T - transmitter
MARCH 1978Mullard
CL8640R-Page 1
TYPICAL OPERATING CONDITIONS
Supply voltage (note 1)
Starting current
Running current
-7.0
250
170
V
mA
mA
VV
Tuning voltage (modulation) (notes 1 and 2) CL8640R -0. 5 to -7. 5
CL8640T -0.5 to -1.5
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage ma*.
Supply voltage (transient) max.
Tuning voltage max.
Tuning current max.
Load v. s.w. r. max.
CHARACTERISTICS (at 25°C)
Centre frequency CL8640RCL8640T
Mechanical tuning range
Electronic tuning range CL8640R
(notes 2 and 3) CL8640T
Power output at -7.0V
Frequency pushing
Frequency pulling (note 4)
Frequency temperature coefficient
Tuning current
TEMPERATURE
Operating range
Storage range
OPERATING NOTES
1. The active element will be damaged if the supply voltage is reversed. Care
should be taken to avoid transients in the supply voltage.
2. The electronic tuning provided by the varactor diode circuit is non -linear,
following an approximately exponential rate of change of capacitance at low tuning
voltages.
3. For CL8640R the tuning voltage range is -0.5V to -7.5V with the electronic
centre at -2.5V.
4. V.S.W.R. = 1.5:1
-7.2 V
-8.0 V
-12 V
100 MA
1. 5:1
10.49 GHz10.56 GHz
Min. Typ. Max.
±60 - - MHz
±15 - - MHz
±4.0 - - MHz
4.0 6.0 - mW- 3.0 MHz/V
- 1.5 - MHz
- -0.25 -0.3 MHz/°C
- - 10 piA
CL8640R CL8640T
-15 to +70 +25 to +70 °C
-30 to +100 -30 to +100 °C
MilliardCL8640R-Page 2
X-BAND GUNNOSCILLATOR
CL8640RCL8640T
4 holes 04'3
positioned to suit
standard W-G-16 flange
CL8640Ronly
«K
168"max"
4030
~rAll dimensions in mm
OUTLINE DRAWING
MilliardCL8640R-Page 3
CL8690
X-BAND GUNN OSCILLATOR
This is an electronically and mechanically tuned oscillator suitable for use as a solid state replacement
for reflex klystrons. It may be used as a local oscillator in marine radar systems. The device has been
tested to ensure its compliance with the requirements of Board of Trade specification
BOTSBN 115 10057/1.
QUICK REFERENCE DATA
Output connector
Centre frequency
Mechanical tuning range
Electronic tuning range
Power output
Operating voltage
WG16
9.375 GHz
min. ±75 MHz
min. ±25 MHz
min. 5 mW-7.5 V
u Mullard rNovember 1978
CJL8690
Jk.TYPICAL OPERATING CONDITIONS
Supply voltage (note 1
)
Supply current
Tuning voltage (notes 1 and 2)
Tuning current
LIMITING VALUES at 20 °C
In accordance with the Absolute Maximum System
Supply voltage
Supply current (note 3)
Tuning voltage
Tuning current
Storage temperature
Ambient operating temperature
CHARACTERISTICS at 20 °C
Centre frequency (note 4)
Mechanical tuning range
Electronic tuning range
Power output (note 5)
Frequency deviation over temperature range
Frequency pushing
Frequency pulling (note 6)
Mechanical tuning rate
-7.5 V
160 mA
-1to-12 V
10 juA
max. -8 V
max. 200 mAmax. -15 V
max. 100 /*A
-45 to +85 °C
15 to +50 °C
9.375 GHz
min. typ. max.
±75 ±100 MHz
±25 ±30 MHz
5 8 mW±15 ±25 MHz
10 15 MHz/V
20 MHz
250 MHz/turn
Notes
1. The active element will be damaged if the supply voltage is reversed. In addition, care should be
taken to avoid transients in the supply voltage as far as possible.
2. The tuning voltage should have a source impedance of less than 1 kifi.
3. During the switch-on period, the Gunn device current will rise to a peak of up to 300 mA at
approximately —4 V and then fall to the specified operating current at —7.5 V.
4. The centre frequency is measured with supply voltages of —7.5 V to the Gunn device and —5 V to
the varactor diode.
5. Power output is measured under all conditions of tuning and temperature.
6. The load v.s.w.r. is 1.3 max. Frequency pulling is measured over all phases of mismatch.
November 1978Y Milliard C?
X-band gunn oscillator CL8690
APPLICATION NOTES
1. Three solder pins are provided for connection of the supply voltages and the earth contact.
2. To prevent parasitic low frequency oscillation, a 1 nF capacitor is connected across the Gunn device.
3. The centre frequency may be set within the limits given in the characteristics, by turning the screw.
4. A zener diode should be connected across the Gunn device supply for transient protection.
MECHANICAL DATA Dimensions in mm
29.7max
4> 3:5min for tuning screw access
Gunn supply voltage
Tuning supply voltage
-7.5V -25Vmax ±~ CL 8690
Mullard
40. 5max
A.
~T24.5max
9.6nom
T-;
LA2.5max
Mechanical
tuningr
4 notes<t> 4.35/4.45 positioned
to suit standard waveguide 16
V
B&-nt-Lj
7
41 .7max
41 .7max
U Mullard YNovember 1978
CL8690
20 1 D8278
Tuning
voltage
(V)
15 —
10 Howeroutput
A \
Ti
5
-50
20
Powpoutpi
(mW)
15
10
-25 +25 +50 TemperaturefC) +100
Typical power output and tuning voltage as a function of temperature.
(Output frequency constant at 9.385 G Hz)
9.45
Frequency
(GHz)
9.40
9.35
9.30
November
|I I | | | |
--.-^j^ -g—Tamb 25 C '
r-*.-"*'
ILW'' **"""««^ — >a "* *
r ^^»" -+20Cj~^<"^^^ A^^v\ - ^^""^
^ "^. ^^ 7p. r - — ^^>^ ^^ » —^^^
^^ ^^ •* ^ S'
. ^ ^ ^ ^^ '"
> ^ ^ <* ^^ ? ^^
^ > ^ ^/ ^ ^?
2 > rf!^^ ^ jW
~*Z i?
^ ^ ^/ ^
^ ^
r7
i_5 -10 Tuning voltage (V)
Typical output frequency as a function of tuning voltage at
three ambient temperatures
1978]
[ Milliard
-20
U
X-band gunn oscillator CL8690
15 D8280
Power t .- jvr
output
(mW)
'amb zo
=+2(TC
10=+ -7K-r
5
1
—5 —10 Tuning voltage (V)
Typical power output as a function of tuning voltage at
three ambient temperatures
-20
9.45 D8281
Frequency
(GHz)
9.40 -12V
5V
r
9 35
-1V
9.30
-100 -75 -50 -25 +25 +50 +75 Temperature (°C)
Typical output frequency as a function of temperature
at three tuning voltages.
V Milliard Y November 1978
CL8690
20 08282
Power
output
(mW)
15
10-12V
•% -5V-1V
5
.
-50 -25 +25 Temperature (°C) +75 +100
Typical power output as a function of temperature at
three tuning voltages
6 November 1978T Milliard U
DOPPLER AND TRAFFICRADARS
CL8880BN
X-BAND TRAFFIC RADAR SENSOR
Fixed frequency radar traffic sensor, with direction sense, for operation in the 10.6 GHz band. The
sensor uses Ooppler radar to provide vehicle actuation for permanent or portable traffic light signals.
It complies with national government regulations {in the U.K. P.o.E. specifications MCE01 11,
MCE01 14 and MCG0500 and Home Office regulation BR14, 1975 specification).
QUICK REFERENCE DATA
Centre frequency
Transmitted power
Detection range for small vehicle moving at 30 m.p.h.
with sensor mounted 2.5 m above typical road surface
Supply voltage (a.c.)
typ.
10.587 GHz
5 mW
100 m110 V
u MilliardOctober 1978
CL8880BN
OPERATING CONDITIONS
Supply voltage (110 V^ centre-tapped) 55-0-55 V
Power consumption typ. 7 W
LIMITING VALUES \In accordance with the Absolute Maximum System
Supply voltage (a.c.) 55-0-55± 20% V
Storage temperature — 20 to + 70 °C
Ambient operating temperature — 15 to + 50 °C
CHARACTERISTICSmin. typ. max.
Centre frequency
fixed in the range 10.577 10.587 10.597 GHz
Transmitted power — 5 10 mW
Detection range for vehicle moving
at 30 m.p.h. with sensor mounted2.5 m above typical road surface 85 100 140 m
Mass 3 kg
CABLE ENTRY
At bottom rear of sensor
October 1978"Y Milliard~~~ V
X-band traffic radar sensor CL8880BN
OPERATING NOTES
1. The sensor is of single-chassis construction.
2. It is recommended that the sensor is mounted so that the centre of the microwave window (radome)
is not less than 150 mm above the cowl of the red signal. There will then be minimal interruption of
the beam by the cowl and the near-field performance of the sensor will not be impaired.
3. In operation, the traffic signal controller demand input is connected to the 'relay output' terminals.
In the standard unit for use with portable signal heads, the relay is energized closed, except when a
demand is present.
4. Units with 'normally open' relay connections are available on request.
5. A 47 n resistor in series with the relay output terminals is included for overcurrent and overvoltage
protection.
6. Upon detection of oncoming traffic, the relay in the sensor is de-energized and a pair of isolated
contacts is opened to signify detection.
7. These contacts remain open during the detection of a stream of oncoming traffic. The minimum
open time is nominally 1 second.
8. Signals caused by departing vehicles are ignored.
9. Should a fault occur in the sensor, or its supply voltage be interrupted, then the sensor relay will be
permanently de-energized and a continuous demand will be applied to the controller. The traffic
signals will then operate automatically in a fixed-time manner.
10. The power supply for the sensor is derived from the main traffic control unit; a 55-0—55 V centre-
tapped a.c. supply is necessary.
11. The cable colour code shown in table 1 must be observed.
TABLE 1
Cable colour code
Red 55Vac
Orange 55Vac
Black V (centre tap of 1 10 V a.c. supply)
Green/Yellow I
Green J
Normally closed output contacts (isolated)
12. The equipment detects lone vehicles approaching the traffic signals in the presence of large
departing vehicles or a heavy stream of departing traffic. This is an important feature of the design
philosophy of the radar process circuit.
13. The equipment does not give false outputs in the absence of moving targets.
14. Signals reflected from fluttering or waving trees at reasonable distances from the sensor do not
cause unwanted outputs, even if the sensor is aimed directly at the trees.
15. For temporary traffic light systems, a 'NUDGE' facility is included.
16. The NUDGE facility is such that in the absence of a demand from approaching traffic for a period
of 2Y2 minutes, a 'phantom' demand is applied. The relay in the sensor is de-energized and the
sensor then returns to the vehicle-actuated mode. The period is set by a digital timer which is
indenendent of the ambient temperature.
U Milliard October 1978
CL8880BN
J\.OPERATING NOTES (continued)
1 7. The 'phantom' demand overcomes the rare lock-up situations in traffic flow at temporary traffic
lights where the possibility of a permanent 'red-red' can occur, caused by the non-detection of
approaching vehicles.
SITE TESTS
1
.
To check the operation of a sensor, set it up in the operating position with the power supplies
connected and connect a multimeter such as the AVO Model 8, switched to a resistance-measuring
range, across the normally-closed contacts. (Note: high-voltage circuit testers, such as the Megger,
must not be used as they will damage the sensor). The measured resistance should be approximate!'
47 £2; this is the value of the protection resistor incorporated in the circuit.
2. Check the a.c. supply voltages at the microwave head. The line-to-line voltage should be 1 10 Vrmsand the voltage between each line and the V terminal should be 55 Vrms . The tolerance on these
voltages is ±20%.
3. Arrange for a vehicle, preferably a small car, to be driven towards and past the sensor at approx-
imately 30 m.p.h. When the car is between 140 and 80 metres from the sensor (see fig.2), the
measured resistance between the normally-closed contacts should quickly increase to indicate an
open-circuit. This condition should continue for approximately 1 second after the car has passed
out of the sensor's detection range.
WORKSHOP TESTS FOR INOPERATIVE SENSORS
1
.
These tests are intended to reveal inoperative sensors only. It must be noted that they do not
replace any range tests carried out with a vehicle under site conditions.
There is no attempt to correlate range measurements with these tests as they will only inform the
operator that a sensor is functioning correctly, not functioning or is functioning in reverse. They
will, however, ensure that there is some consistency of testing between different operators.
2. Ideally, the sensor should be sited in an environment free, as far as possible, from extraneous
movements of large bodies such as people, fork lift trucks, etc.
3. The sensor should be placed on a level surface, e.g. a bench, as near to the edge as possible to
avoid reflections from the bench surface.
KWWWVj\W^
Incorrect Correct 08198
It should not be pointed directly at fluorescent lights as they may cause false demands to beregistered due to interference.
4. Ensure that the environment is free as far as possible from microwave interference, for example,
radar traffic sensors on soak test in the vicinity of the beam could cause interference giving rise to
false demands.
October 1978r
Milliard C?
X-band traffic radar sensor CL8880BN
5. The supply cable should be connected in accordance with the coding given in table 1 on page 3.
6. Demands may be observed by connecting the signal output leads (green and green/yellow) to a
controller with a lamp which indicates presence of a demand. Alternatively, a bulb and power
supply may be connected in series with the signal leads via a simple connector block such as the
push-button type 'quick connector' available from Radiospares. See diagram below
Connector
Signal leads from
radar traffic sensor
D8199
Green / yellow
Green Supply (battery or low
voltage transformer)
10.
This simple method will eliminate the possibility of controller faults.
With the supply connected and switched on, the indicator lamp should be illuminated.
A demand will be indicated when the lamp is extinguished.
Leave the sensor pointing into free space and check for false demands. The lamp should remain
alight for approximately 2 to 2% minutes until the 'nudge' circuitry puts in a 'phantom' demand.
These 'nudge' demands will reappear at regular intervals of 2 to 2Vi minutes; no other demands
should occur between them.
With the sensor placed on a level surface, (see note 3), about 1% metres from ground level, the
operator should stand about 5 metres away from the sensor in a direct line with the microwave
window (radome) and should have the demand indicator lamp in view. He should then walk at
normal walking pace towards the sensor, stopping at about 1 metre from it. If the sensor is
functioning correctly, a demand will be registered between starting to walk and stopping. He
should then wait for the demand to clear and then walk backwards to his starting point No
demand should be registered. If a demand is observed, the sensor is working in reverse and is
therefore faulty.
V Mullard 1October 1978
CL8880BN
MECHANICAL DATA Dimensions in mm
Mounting p4gn«
Radome (screen) anglFinish — Semi matt block enamel
Minimum external length of cable (supplied) = Imetn
October 1978 Mullard
X-band traffic radar sensor CL8880BN
D6201963/3
V
Fig.1 Typical polar diagram of traffic radar sensor.
The broken line indicates the preferred mounting
angle of 15°. This affects only the orientation of
the vertical pattern
Milliard YOctober 1978
CL8880BN
08202(963/21
Fig.2 Detection curves obtained from road tests using six different traffic radar sensors
I I
* Energised closed under no -demand condition
V— Relay output *Relay output
-0V
-55V a.c.
-J— 55V a.c.
, Supply cable
(see Table D
Fig.3 Terminal block connections. The two 55 V terminals on the supply cable are of
opposite phase and are part of a 55—0—55 V a.c. supply.
October 1978T Milliard Zl
X-band traffic radar sensor CL8880BN
QUALITY APPROVAL OF TRAFFIC RADAR SENSORS
The sensors are currently produced at the Mullard plant at Hazelgrove, Cheshire. The Quality
Department within Mullard Hazelgrove operates to standards set by BS9000 and is supported by a
resident E.Q.D. inspector. Product developments are steered through a rigorous release procedure;
development sample are appraised before approval for production.
In the case of these radar sensors, the individual semiconductor diodes are the subject of a separate
quality release exercise, in addition to that carried out on the final sensor. In production, the semi-
conductor diodes are batch-approved by the Quality Department before assembly.
Quality control procedures for production include:
1. Raw material inspection.
2. Quality control within the assembly areas.
3. 100% electrical testing of primary parameters and sample testing to appropriate A.Q.L.
4. Environmental sample testing.
5. Measurement of secondary electrical parameters on batch samples.
6. Calibration and standardization of test procedures.
Where customer requirements differ from the standard commercial product, liasion is established
with specific customers and suitable procurement specifications are agreed.
U Mullard Y-October 1978
CL8880BNC
X-BAND TRAFFIC RADAR SENSOR
Fixed frequency radar traffic sensor, with direction sense, for operation in the 10.6 GHz band. The
sensor uses Doppler radar to provide vehicle actuation for permanent or portable traffic light signals.
It complies with national government regulations (In the U.K. D.o.E. specifications MCE0111,
MCE0114 and MCG0500 and Home Office regulation BR 14, 1975 specification!.
QUICK REFERENCE DATA
Centre frequency
Transmitted power
Detection range for small vehicle moving at 30 m.p.h.
with sensor mounted 2.5 m above typical road surface
Supply voltage (a.c.)
typ.
10.587 GHz
5 mW
100 m
110 V
u MilliardOctober 1978
CL8880BNC
OPERATING CONDITIONS
Supply voltage (1 10 Vac centre-tapped)
Power consumption
LIMITING VALUES
In accordance with the Absolute Maximum System
Supply voltage (a.c.)
Storage temperature
Ambient operating temperature
CHARACTERISTICS
Centre frequency
fixed in the range
Transmitted power
Detection range for vehicle moving
at 30 m.p.h. with sensor mounted
2.5 m above typical road surface
Mass
CABLE ENTRY
Through the mounting foot
55-0-55 V
typ. 7 W
55-0-55±20% V
-20 to + 70 °C
-15 to + 50 °C
min. typ. max.
10.577 10.587 10.597 GHz
5 10 mW
85 100 140 m3 kg
October 1978Y Milliard U
X-band traffic radar sensor CL8880BNC
OPERATING NOTES
1. The sensor is of single-chassis construction.
2. It is recommended that the sensor is mounted so that the centre of the microwave window (radome)
is not less than 150 mm above the cowl of the red signal. There will then be minimal interruption of
the beam by the cowl and the near-field performance of the sensor will not be impaired.
3. In operation, the traffic signal controller demand input is connected to the 'relay output' terminals.
In the standard unit for use with portable signal heads, the relay is energized closed, except when a
demand is present.
4. Units with 'normally open' relay connections are available on request.
5. A 47 S2 resistor in series with the relay output terminals is included for overcurrent and overvoltage
protection.
6. Upon detection of oncoming traffic, the relay in the sensor is de-energized and a pair of isolated
contacts is opened to signify detection.
7. These contacts remain open during the detection of a stream of oncoming traffic. The minimum
open time is nominally 1 second.
8. Signals caused by departing vehicles are ignored.
9. Should a fault occur in the sensor, or its supply voltage be interrupted, then the sensor relay will be
permanently de-energized and a continuous demand will be applied to the controller. The traffic
signals will then operate automatically in a fixed-time manner.
10. The power supply for the sensor is derived from the main traffic control unit; a 55-0—55 V centre-
tapped a.c. supply is necessary.
1 1
.
The cable colour code shown in table 1 must be observed.
TABLE 1
Cable colour code
Red 55Vac
Orange 55Vac
Black V (centre tap of 1 10 V a.c. supply)
Green/Yellow 1
GreenJ
Normally closed output contacts (isolated)
12. The equipment detects lone vehicles approaching the traffic signals in the presence of large
departing vehicles or a heavy stream of departing traffic. This is an important feature of the design
philosophy of the radar process circuit.
13. The equipment does not give false outputs in the absence of moving targets.
14. Signals reflected from fluttering or waving trees at reasonable distances from the sensor do not
cause unwanted outputs, even if the sensor is aimed directly at the trees.
15. For temporary traffic light systems, a 'NUDGE' facility is included.
16. The NUDGE facility is such that in the absence of a demand from approaching traffic for a period
of 2% minutes, a 'phantom' demand is applied. The relay in the sensor is de-energized and the
sensor then returns to the vehicle-actuated mode. The period is set by a digital timer which is
independent of the ambient temperature.
u Milliard Y October 1978
CL8880BNC
OPERATING NOTES (continued)
1 7. The 'phantom' demand overcomes the rare lock-up situations in traffic flow at temporary traffic
lights where the possibility of a permanent 'red-red' can occur, caused by the non-detection of
approaching vehicles.
SITE TESTS
1. To check the operation of a sensor, set it up in the operating position with the power supplies
connected and connect a multimeter such as the AVO Model 8, switched to a resistance-measuring
range, across the normally-closed contacts. (Note: high-voltage circuit testers, such as the Megger,
must not be used as they will damage the sensor). The measured resistance should be approximately
47 J2; this is the value of the protection resistor incorporated in the circuit.
2. Check the a.c. supply voltages at the microwave head. The line-to-line voltage should be 1 10 Vrmsand the voltage between each line and the V terminal should be 55 Vrms . The tolerance on these
voltages is ±20%.
3. Arrange for a vehicle, preferably a small car, to be driven towards and past the sensor at approx-
imately 30 m.p.h. When the car is between 140 and 80 metres from the sensor (see fig.2), the
measured resistance between the normally-closed contacts should quickly increase to indicate an
open-circuit. This condition should continue for approximately 1 second after the car has passed
out of the sensor's detection range.
WORKSHOP TESTS FOR INOPERATIVE SENSORS
1
.
These tests are intended to reveal inoperative sensors only. It must be noted that they do not
replace any range tests carried out with a vehicle under site conditions.
There is no attempt to correlate range measurements with these tests as they will only inform the
operator that a sensor is functioning correctly, not functioning or is functioning in reverse. They
will, however, ensure that there is some consistency of testing between different operators.
2. Ideally, the sensor should be sited in an environment free, as far as possible, from extraneous
movements of large bodies such as people, fork lift trucks, etc.
3. The sensor should be placed on a level surface, e.g. a bench, as near to the edge as possible to
avoid reflections from the bench surface.
y\v^v\v\\v\v^
HiIncorrect Correct 08198
It should not be pointed directly at fluorescent lights as they may cause false demands to be
registered due to interference.
4. Ensure that the environment is free as far as possible from microwave interference, for example,
radar traffic sensors on soak lest in the vicinity of the beam could cause interference giving rise to
false demands.
October 1978¥ Mullard U
X-band traffic radar sensor CL8880BNC
5. The supply cable should be connected in accordance with the coding given in table 1 on page 3.
6. Demands may be observed by connecting the signal output leads (green and green/yellow) to a
controller with a lamp which indicates presence of a demand. Alternatively, a bulb and power
supply may be connected in series with the signal leads via a simple connector block such as the
push-button type 'quick connector' available from Radiospares. See diagram below
Connector
Signal leads from
radar traffic sensor
D8199
Green / yellow
Green Supply {battery or low
voltage transformer)
10.
This simple method will eliminate the possibility of controller faults.
With the supply connected and switched on, the indicator lamp should be illuminated.
A demand will be indicated when the lamp is extinguished.
Leave the sensor pointing into free space and check for false demands. The lamp should remain
alight for approximately 2 to 2% minutes until the 'nudge' circuitry puts in a 'phantom' demand.
These 'nudge' demands will reappear at regular intervals of 2 to 2% minutes; no other demands
should occur between them.
With the sensor placed on a level surface, (see note 3), about VA metres from ground level, the
operator should stand about 5 metres away from the sensor in a direct line with the microwave
window (radome) and should have the demand indicator lamp in view. He should then walk at
normal walking pace towards the sensor, stopping at about 1 metre from it. If the sensor is
functioning correctly, a demand will be registered belween starting to walk and stopping. He
should then wait for the demand to clear and then walk backwards to his starting point Nodemand should be registered. If a demand is observed, the sensor is working in reverse and is
therefore faulty.
U Milliard^r
October 1978
CL8880BNC
MECHANICAL DATA
yv.Dimensions in mm
Radome (screen) angle
-Minimum external length of cable
(supplied) =1 metre
Section on X
,|, Irl 3 notes \ in BSW[Fastening screws not
Recommended depth
engagement in body
Supplied.1
of
13mm J
Finish - Semi matt block enamel
October 1978
fMilliard V
X-band traffic radar sensor CL8880BNC
90° 8006201963/3
u
Fig, 1 Typical polar diagram of traffic radar sensor.
The broken line indicates the preferred mounting
angle of 15°. This affects only the orientation of
the vertical pattern.
MullardOctober 1978
CL8880BNC
Fig.2 Detection curves obtained from road tests using six different traffic radar sensors
^— Relay output *- Relay output
-j-OV
-r- 55V a.c.
-j— 55V a.c.
, Supply cable'(see Table 1)
II
* Energised closed under no -demand condition P963/M
Fig.3 Terminal block connections. The two 55 V terminals on the supply cable are of
opposite Dhase and are Dart of a 55—0—55 V a.c. suddIv.
October 1978T Milliard U
X-band traffic radar sensor CL8880BNC
QUALITY APPROVAL OF TRAFFIC RADAR SENSORS
The sensors are currently produced at the Mullard plant at Hazelgrove, Cheshire. The Quality
Department within Mullard Hazelgrove operates to standards set by BS9000 and is supported by a
resident E.Q.D. inspector. Product developments are steered through a rigorous release procedure;
development sample are appraised before approval for production.
In the case of these radar sensors, the individual semiconductor diodes are the subject of a separate
quality release exercise, in addition to that carried out on the final sensor. In production, the semi-
conductor diodes are batch-approved by the Quality Department before assembly.
Quality control procedures for production include:
1. Raw material inspection.
2. Quality control within the assembly areas.
3. 100% electrical testing of primary parameters and sample testing to appropriate A.Q.L.
4. Environmental sample testing.
5. Measurement of secondary electrical parameters on batch samples.
6. Calibration and standardization of test procedures.
Where customer requirements differ from the standard commercial product, liasion is established
with specific customers and suitable procurement specifications are agreed.
U Mullard YOctober 1978
X-BAND DOPPLERRADAR MODULE
CL8960
yUlCK REFERENCE DATA
Fixed frequency Gtinn oscillator and mixer cavity for operation In the 10,7GHz
hand. Applications Include all forms of Doppler radar systems.
Centre frequency
Power output (at 7. OV) typ.
Output voltage (typ, ) for input power
lOOdB down on output powersignal ( noise
at l&iB min. — ;
noiee
(see page 6 and note 1)
Supply voltage
10.687
10
40
7.0
mW
V
MullardOCTOBER 1978 CL8960 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D. C. mixer bias current (into a. f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb ranSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
,„,„ . signal + noise. .
18dB min. —
—
:) (see
noise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Second harmonic
Diode current (see note 3)
Polar diagram
Min.
20
10. 675
+7. ± 0.
1
V
40 mA
30 to 35 MA
10 kn
+7.5
9.0
-10 to +70
to +40
Typ. Max.
V
°C
GHz
40 - «v
10 - mW
10. 687 10. 699 GHz
-0.2 -0.3 MHz/OC
4.0 - MHz/V
35 - dBm
30 165 mA
see page 7
MASS 170
Alternative antennae and operating frequencies may be made to suit customers
'
specific requirements.
MilliardCL8960 Page 2
X-BAND DOPPLER CL8960RADAR MODULE
OPERATING NOTES -*"
1. A return signal lOOdB down on radiated power will be achieved from a mantarget of radar cross-section 1.0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
Extended range may be obtained for a reduced —*-—: and this may be6 } noise '
acceptable if the environment in which the system operates is stable, i.e. , free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross-section 1.0m2 at a range of 25m and
the ———: is reduced to l5dB with an output voltage of l6fzV min.noise
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Milliard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunnvoltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti- static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
—™—
_
performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MilliardCL8960 Page 3
OUTLINE DRAWING
a^rA4
2 holes 04.2/4.051.5/51. centres
Recommendedscrews - M4
Antenna
12.3
MilliardCL8960 Page 4
X-BAND DOPPLERRADAR MODULE
CL8960
Max curve
I mo* 250
Max 165
Pt>3 7 Voltage (V)
Gunn device characteristic
®9 A.F. terminal
CL8960mixer
X
-7V
R1
100kn
R2lOkO
Bandwidth 1Hz to 1kHz
Z in >100kfl
Circuit used to measure A. F. performance
Notes
1. The current lb should be approximately 35/jA with the Gunn device disconnected
and approximately 42/nA with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8960 Page 5
> 1000
3n 7
100
10
,F:e et
Metres
M HK \— - nc
le
)ise — ^-
vel
—
10 100 1000
Target range (m and ft)
Minimum output for a man target
MullardCL8960 Page 6
X-BAND DOPPLERRADAR MODULE
CL8960
Vertical B
Horizontal oQH°
Polar diagram for antenna supplied.
MilliardCL8960 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antenna
are mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-sions as shown on page 9.
In this configuration , the metal plate forms the front panel of the equipment , andthe antenna radiates into free space. If the equipment housing is all metal , anyback radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42/xA.
(35^A d.c. Was + l\ih from -19dBm of coupled l.o. power.)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture , then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic material
is detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60/^A.
The increase in 1. o. power will , in general give rise to an increase in a. f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled 1. o. power arising from the use
of thick or ' microwave ' reflective covering materials , will
:
(a) continue to increase the a. f . output voltage from the mixer (N. B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching andrunning performance and may 'pull' the frequency outside the allocated operat-
ing frequency band.
The following table compares the l.o. coupling level obtained for different covering
materials at the antenna.
L. 0. coupling
(dBm)
Mixer total bias
(HA)
Antenna covering
material
- 35 (d.c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene or
polystyrene
-11 61 0. 25mm Gobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division
,
Brantham Works
,
Brantham
,
Manningtree, Essex CO 11 1NJ
MilliardCL8960 Page 8
X-BAND DOPPLERRADAR MODULE
CL8960
Cobex' plastic sheet(or equivalent)
ML screw
Aluminium panel1.6mm (16s.w.g.)
2 holes drill
04.2-CSK 07.0
Cobex 0.25mm sheet
Panel mounting details
MullardCL8960 Page 9
X-BAND DOPPLERRADAR MODULE
CL8961
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator and mixer cavity for operation In the 9.4 GHz
band. Applications include all forms of Doppler radar systems.
Centre frequency
Power output (at 7. OV) typ.
Output voltage (typ. ) far input power
IQOdB down on output powersignal + noise
at lSdB min.s
wn ,,_noise
(see page 6 and note 1)
Supply voltage
9.350
10
40
7,0
GHz
mW
V
OCTOBER 1978Mullard
CL8961 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D. C. mixer bias current (into a. f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d.c.J
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb ranSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
, .„ . signal + noise . .
18dB nun. —
-
fi :) (see
noise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Second harmonic
Diode current (see note 3)
Polar diagram
MASS
20
9.338
+7. ± 0. 1 V
140 mA
30 to 35 MA
10 kn
+7.5
9.0
- 10 to +70
to +40
Min. Typ.
9. 350
Max.
V
°C
GHz
40 - MV
10 - mW9.350 9.362 GHz
-0.2 -0.3 MHz/>C
4.0 - MHz/V
35 - dBm
30 165 mA
see page 7
210
Alternative antennae and operating frequencies may be made to suit customers
'
specific requirements.
MilliardCL8961 Page 2
X-BAND DOPPLER CL8961RADAR MODULE
OPERATING NOTES
1. A return signal lOOdB down on radiated power will be achieved from a mantarget of radar cross -section 1. 0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. )•
j , j signal + noise , „,
.
,
Extended range may be obtained for a reduced —=- : and tins may be° ' noise
acceptable if the environment in which the system operates is stable , i.e., free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross -section 1.0m2 at a range of 25m and
thesi^n + nolse
is reduced to 15dB with an output voltage of l6piV min.noise
Alternatively , the range may be increased by an increase in target radar cross -
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Milliard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunn
voltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti- static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
10. —SHr— performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
Milliard :
CL8961 Page 3
OUTLINE DRAWING
69
rffw*fl—
_
A7 :
2 holes 0C559.3/58.8 centres
Recommended screw M4
Antenna
12.5
MullardCL8961 Page 4
X-BAND DOPPLERRADAR MODULE
CL8961
I mov250
9 A.F. terminal
Max curve
%3 7 Voltage (V)
Gunn device characteristic
+7V
i
CL8961mixer
R1
lOOkfl Bandwidth 1Hz to 1kHz
Z in >100kQ
T
R2iokn
Circuit used to measure A.F. performance
Notes
1. The current lb should be approximately 35fiA with the Gunn device disconnected
and approximately 42^A with the Gunn device operational and the antenna oper-ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8961 Page 5
> 1000
eno
100
,F:e et
Metres
M n* \— - nc
le
>ise — *-
vel
10 100 1000
Target range (m and ft)
Minimum output for a man target
MullardCL8961 Page 6
X-BAND DOPPLERRADAR MODULE
CL8961
90° 80 «
Vertical B
Horizontal |qQDo[
Polar diagram for antenna supplied.
MilliardCL8961 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antenna
are mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-sions as shown on page 9.
In this configuration , the metal plate forms the front panel of the equipment , andthe antenna radiates into free space. If the equipment housing is all metal , anyback radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42jtA.
(35*/A d.c. bias + 7/iA from -19dBm of coupled l.o. power.)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture, then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic materialis detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60/xA.
The increase in l.o. power will, in general give rise to an increase in a. f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled l.o. power arising from the useof thick or * microwave' reflective covering materials, will:
(a) continue to increase the a. f. output voltage from the mixer ON* B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching and
running performance and may ' pull * the frequency outside the allocated operat-
ing frequency band.
The following table compares the 1. o. coupling level obtained for different coveringmaterials at the antenna.
L. 0. cbupling
(dBm)
Mixer total bias
(tiA)
Antenna covering
material
- 35 (d.c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene or
polystyrene
-11 61 0. 25mm Cobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division,
Brantham Works
,
Brantham,
Manningtree, Essex CO 11 1NJ
MilliardCL8961 Page 8
X-BAND DOPPLERRADAR MODULE
CL8961
Cobex' plastic
sheet (or equivalent)
ML screw
Aluminium panel
1.6mm (16s.w.g.)
2 holes drill
0LS -CSK
Cobex0.25mm sheet
MullardCL8961 Page 9
X-BAND DOPPLERRADAR MODULE
CL8962
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator and mixer cavity for operation In the 9. S GHzband. Applications Include all forms of Doppler radar systems.
Centre frequency 9, 47 GHz
Power output (at 7. OV) typ. 10 mwOutput voltage (typ. ) for input power
lOOdB down on output power
„ lft_ . signal + noiseat 18dB mln, " ig
noise
(see page 6 and note 1) 40 tiV
Supply voltage 7. V
MilliardOCTOBER 1976 CL8962 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D.C. mixer bias current (into a.f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.
(1.0ms max.)
Tstg ran8e
Tamb ranSe
•CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
,-,_ . signal + noise . .
18dB min. —* : ) (seenoise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Diode current (see note 3)
Polar diagram
20
9.458
+7. ± 0. 1 V
40 mA
30 to 35 MA
10 kS2
+7.5
9.0 V
10 to +70 °C
to +40 °C
Min. Typ.
9. 470
Max.
GHz
40 - »V
10 - mW
9.470 9.482 GHz
-0.2 -0.3 MHz/»C
4.0 - MHz/V
130 165 mA
see page 7
MASS 210
Alternative antennae and operating frequencies may be made to suit customers
'
specific requirements.
MilliardCL8962 Page 2
X-BAND DOPPLER CL8962RADAR MODULE
OPERATING NOTES ^1. A return signal lOOdB down on radiated power will be achieved from a man
target of radar cross-section 1.0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
, . , , jo signal + noise . .,
.
,
Extended ranee may be obtained for a reduced —2-: and this may be° noise
acceptable if the environment in which the system operates is stable, i.e. , free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross -section 1.0m2 at a range of 25m and
theSlgPal +noise
is reduced to l5dB with an output voltage of 16/iV min.noise
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Milliard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunn
voltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti -static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
10. Signal + noise . .,,....., . j*_—g performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MilliardCL8962 Page 3
OUTLINE DRAWING
69
Aa^ A
2 holes 0L.5
59.3/58.8 centres
7121
Recommended screw ML
T12.5
Antenna
MilliardCL8962 Page 4
X-BAND DOPPLERRADAR MODULE
CL8962
Notes
©o—
*
Max curve
I m««250
Max 165
%3 7 Voltage (V)
Gunn device characteristic
+ 7V
9 A.F. terminal
CL8962
R1
lOOkfl Bandwidth 1Hz to 1kHz
Z in >100kQ
CI
X
R2iokn
Circuit used to measure A.F. performance
1. The current lb should be approximately 35^A with the Gunn device disconnected
and approximately 42jxA with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8962 Page 5
> 1000a.
o
100
10
,F:e et
Metres
M nx \— - nc
le
ise — ^-
vel
—
10 100 1000
Target range (m and ft)
Minimum output for a man target
MilliardCL8962 Page 6
X-BAND DOPPLERRADAR MODULE
CL8962
Vertical B
Horizontal <CC°
Polar diagram for antenna supplied.
MilliardCL8962 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antennaare mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-sions as shown on page 9.
In this configuration, the metal plate forms the front panel of the equipment, andthe antenna radiates into free space. If the equipment housing is all metal , anyback radiation will be totally contained. Alternatively a metal based adhesive tapemay be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42^A.(35/iA d. c. bias + 7^A from - 19dBm of coupled 1. o. power.
)
If, however, for environmental reasons, it is considered desirable to cover theantenna aperture, then it is recommended that a thin plastic material (approximately0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic materialis detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60/xA.
The increase in l.o. power will, in general give rise to an increase in a.f. outputvoltage for a given target, but this will be accompanied by a degradation in signalto noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled l.o. power arising from the useof thick or * microwave' reflective covering materials, will:
(a) continue to increase the a. f. output voltage from the mixer (N. B. the increasewill not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching andrunning performance and may * pull ' the frequency outside the allocated operat*ing frequency band.
The following table compares the l.o. coupling level obtained for different coveringmaterials at the antenna.
. 0. coupling
(dBm)
Mixer total bias
0*A)
Antenna covering
material
- 35 (d. c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene or
polystyrene
-11 61 0. 25mm Cobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division
,
Brantham Works
,
Brantham
,
Manningtree, Essex CO 11 1NJ
MullardCL8962 Page 8
X-BAND DOPPLERRADAR MODULE
CL8962
Cobex' plastic
sheet (or equivalent)
M4 screw
Aluminium panel
1.6mm (16s.w.g.)
2 holes drill
04.5 -CSK
Cobex0.25mm sheet
D8193a
Panel mounting details
MilliardCL8962 Page 9
X-BAND DOPPLERRADAR MODULE
CL8963
QUICK REFERENCE DATA
Fixed frequency Gunn osctEatoraud mixer cavity for operation In the 10. 5GHzband. Applications include all forms of Doppler radar systems.
Centre frequency
Power output (at 7.0V) typ.
Output voltage (typ. ) for Input power
lOOdB down on output powersignal + noise
at iSdB min. —= :
noise
(see page 6 and note 1)
Supply voltage
10. 525
10
40
7.0
GHz
mW
V
OCrrOBKR 1978
MullardCL8963 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D. C. mixer bias current (into a. f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb ranSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
, ,_ . signal + noise . .
18dB min. —- : > (seenoise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Second harmonic
Diode current (see note 3)
Polar diagram
MASS
Min.
20
10.513
+7.0 ±0.1 V
40 mA
30 to 35 HA
10 kg
+7.5
9.0 V
10 to +70 °C
to +40 °C
Typ. Max.
GHz
40 - fiV
10- mW
10. 525 10. 537 GHz
-0.2 -0.3 MHz/OC
4.0 - MHz/V
-35 - dBm
130 165 mA
see page 7
170
Alternative antennae and operating frequencies may be made to suit customers
'
specific requirements.
MilliardCL8963 Page 2
X-BAND DOPPLER CL8963RADAR MODULE
OPERATING NOTES -<
1. A return signal lOOdB down on radiated power will be achieved from a mantarget of radar cross -section 1.0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
si2H3I *+ noiseExtended range may be obtained for a reduced —" and this may be
acceptable if the environment in which the system operates is stable , i.e., free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross-section 1.0m2 at a range of 25m and
the—™
—
: is reduced to 15dB with an output voltage of 16/xV min.
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then becalculated from the radar range equation. Further related information may beobtained on application to Milliard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunnvoltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixera. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) And -static clothing should be worn.
d) No electrical testing should be carried out without specific, approved andwritten test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
10. Signal + noise—x : performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MullardCL8963 Page 3
OUTLINE DRAWING
jjSa^JL
^2 holes 04.2M.O51.5/51.0centres
Recommendedscrews - M4
Antenna
12.3
MullardCL8963 Page 4
X-BAND DOPPLERRADAR MODULE
CL8963
l ma«250
Max 165 Max curve
Voltage (V)
Notes
lb
©
Gunn device characteristic
>7V
9 A.F. terminal
CL8962
~x
1R1
iookn
R2iokn
Bandwidth lHztolkHzZ in >100kn
Circuit used to measure A.F. performance
1. The current lb should be approximately 35/xA with the Gunn device disconnected
and approximately 42pA with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8963 Page 5
> 1000
100
10
,F:e et
Metres
M nx \— - no
le
ise — ^-
vel
105 7 2
100 1000
Target range (m and ft)
Minimum output for a man target
MilliardCL8963 Page 6
X-BAND DOPPLERRADAR MODULE
CL8963
Vertical B
Horizontal p[XH
Polar diagram for antenna supplied.
MilliardCL8963 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antennaare mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-sions as shown on page 9.
In this configuration, the metal plate forms the front panel of the equipment, andthe antenna radiates into free space. If the equipment housing is all metal , anyback radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42/xA.
(35^A d.c. bias + 7nA from -19dBm of coupled l.o. power.)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture, then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic materialis detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60fiA.
The increase in l.o. power will, in general give rise to an increase in a. f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled 1. o. power arising from the useof thick or * microwave ' reflective covering materials , will
:
(a) continue to increase the a. f. output voltage from the mixer (N. B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching andrunning performance and may 'pull' the frequency outside the allocated operat-ing frequency band.
The following table compares the 1. o. coupling level obtained for different coveringmaterials at the antenna.
L. 0. coupling
(dBm)
Mixer total bias
0*A)
Antenna covering
material
- 35 (d.c. (only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene orpolystyrene
-11 61 0. 25mm Cobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics,
Sheet and Film Division
,
Brantham Works
,
Brantham,
Manningtree, Essex CO 11 1NJ
MilliardCL8963 Page 8
X-BAND DOPPLERRADAR MODULE
CL8963
Cobex' plastic sheet
(or equivalent)
M4 screw
Aluminium panel1.6mm (16s.w.g.)
2 holes drill
0U.2-CSK 07.0
Cobex 0.25mm sheet
51.5
51.0
Panel mounting details
MullardCL8963 Page 9
X-BAND DOPPLERRADAR MODULE
CL89E4
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator and mixer cavity for operation In the 9.9 GHzband. Applications include all forms of Doppler radar systems.
Centre frequency
Power output {at 7.0V) typ.
Output voltage (typ.) for input power
lOOdB down on output power
__ , signal + noiseat lSdB min. —E —
noise
(see page 6 and note 1)
Supply voltage
9.900
10
40
7.0
GHz
mW
V
MilliardOCTOBER I97ti CL8964 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D.C. mixer bias current (into a.f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb ranSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
, DJ r, , signal + noise. .
l8dB min. ^^. ) (see
noise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Second harmonic
Diode current (see note 3)
Polar diagram
20
9.978
+7.0 ±0.1 V
140 mA
30 to 35 MA
10 kQ
+7.5
9.0 V
-10 to +70 °C
to +40 °c
Min. Typ. Max.
- 9.990 - GHz
40 - VlV
10 - mW9.990 10.002 GHz
-0.2 -0.3 MHz/»C
4.0 - MHz/V
-35 - dBm
130 165 mA
see page 7
MASS 170
Alternative antennae and operating frequencies may be made to suit customers'
specific requirements.
MuHardCL8964 Page 2
X-BAND DOPPLER CL8964RADAR MODULE
OPERATING NOTES
1. A return signal lOOdB down on radiated power will be achieved from a man
target of radar cross-section 1. Om2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
Extended range may be obtained for a reduced ™. and this may be
acceptable if the environment in which the system operates is stable, i.e. , free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross -section 1. Om2 at a range of 25m and
thesignal + noise
ig reduced to l5dB ^^ ^ output voltage of 16^V min.noise
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Milliard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunn
voltage (+7V) and the d. c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti- static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
.gnal + no se
performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MilliardCL8964 Page 3
OUTLINE DRAWING
s^p_ jjl
+2 holes 04,2/4.051.5/51.0 centres
> -2b »>
c
or >rn |
4.6
i
rn
+11
1 27.4.
< =3—r 26.8
12.3
"1 i
Recommended screws -M4.
y"T12.3
Antenna
MullardCL8964 Page 4
X-BAND DOPPLERRADAR MODULE
CL8964
Max curve
%3 7
Gunn device characteristic
Voltage (V)
Notes
©9 A.F. terminal
CL8964-
mixer
I
+ 7V
R1
iookn
R210kfl
Bandwidth 1Hz to 1kHz
Z in >100kn
Circuit used to measure A.F. performance.
1. The current lb should be approximately 35j*A with the Gunn device disconnected
and approximately 42fiA with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8964 Page 5
D6010
> 1000a.
oo
G 5
o
at ,
put
voltag
o o
3O 7
10
k Fee t
Metres
Mnx \— — - rlOise — ^-
evel
1 „
10 100 1000
Target range {m and ft)
Minimum output for a man target
MullardCL8964 Page 6
X-BAND DOPPLERRADAR MODULE
CL8964
Vertical B
Horizontal [«>CD<>|
Polar diagram for antenna supplied.
MilliardCL8964 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antenna
are mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-
sions as shown on page 9.
In this configuration, the metal plate forms the front panel of the equipment, and
the antenna radiates into free space. If the equipment housing is all metal , any
back radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42jiA.
(35fiA d.c. bias + 7)iA from -19dBm of coupled l.o. power.)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture, then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic material
is detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60mA.
The increase in l.o. power will, in general give rise to an increase in a. f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled l.o. power arising from the use
of thick or * microwave ' reflective covering materials , will
:
(a) continue to increase the a. f . output voltage from the mixer (N. B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching and
running performance and may 'pull' the frequency outside the allocated operat-
ing frequency band.
The following table compares the l.o. coupling level obtained for different covering
materials at the antenna.
L. 0. coupling
(dBm)
Mixer total bias
G*A)
Antenna covering
material
- 35 (d.c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene orpolystyrene
-11 61 0. 25mm Cobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division,
Brantham Works
,
Brantham,
Manningtree, Essex OOll 1NJ
MilliardCL8964 Page 8
X-BAND DOPPLERRADAR MODULE
CL8964
Cobex' plastic
sheet (or equivalent)
ML screw
Aluminium panel
1.6mm (16s.w.g.)
2 holes drill
04.5-CSK
Cobex0.25mm sheet
MullardCL8964 Page 9
X-BAND DQPPLERRADAR MODULE
CL8965
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator and mtxer cavity for operation In the 10,
band. Applications include all forms of Doppler radar systems.
6GHz
Centre frequency 10.565 GHz
Power output (at 7.0V) typ. 10 raW
Output voltage (typ. ) for Input power
lOOdB down on output power
. , aJn j signal + noiseat 18dB rain. —^ :
noise
(see page 6 and note 1) 40 *v
Supply voltage 7.0 V
MilliardOCTOBER 1978 CL896S Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D.C. mixer bias current (into a.f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb TanSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
signal + noise>
+7. ± 0.
1
V
140 mA
30 to 35 MA
10 kQ
+7.5
9.0
-10 to +70
to +40
Min. Typ.
10. 565
Max.
V
°C
GHz
MASS
noise
notes 1 and 4 and page 6) 20 40 - MV
Output power at 7. 0V - 10 - mWFrequency fixed 10. 553 10. 565 10. 577 GHz
Frequency temperature coefficient - -0.2 -0.3 MHz/»C
Frequency pushing - 4.0 - MHz/V
Second harmonic - -35 - dBm
Diode current (see note 3)- 130 165 mA
Polar diagram see page
170
7
g
Alternative antennae and operating frequencies may be made to suit customers *
specific requirements.
MilliardCL8965 Page 2
X-BAND DOPPLER CL8965RADAR MODULE
OPERATING NOTES <-
1. A return signal lOOdB down on radiated power will be achieved from a mantarget of radar cross-section 1. 0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
, . , » , signal + noise , .. . ,
Extended range may be obtained for a reduced —— : and this may be° noise
acceptable if the environment in which the system operates is stable, i.e. , free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross -section 1.0m2 at a range of 25m and
the ^^—r-^— is reduced to 15dB with an output voltage of lojiV min.noise
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Mullard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunn
voltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary, namely:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti- static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
—££=_ performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MullardCL8965 Page 3
OUTLINE DRAWING
jjfUs-^ ,-lL
^2 holes 04..2M.O51. 5/ 51.0 centres
4>
Recommendedscrews - M4.
Antenna
12.3
MullardCL8965 Page 4
X-BAND DOPPLERRADAR MODULE
CL8965
I m„x250
Max 165 Max curve
%3 Voltage (V)
Notes
lb
Gunn device characteristic
+7V
A.F. terminal
® CL8965mixer
~T
R1
iookn
CI
R2ioi<n
Bandwidth 1Hz to 1kHz
Z in >100kfl
Circuit used to measure A.F. performance
1. The current lb should be approximately 35fzA with the Gunn device disconnected
and approximately 42^A with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8965 Page 5
D6010
> 1000a.
"O 7
oo
Cooc
fl» ,
put
voltag
o o
O 7
kFee t
10Metres
Max \— — - r»oise — ^-
evel
1
2 s 7 2 5 710 100 1000
Target range (m and ft)
Minimum output for a man target
MilliardCL8965Page 6
X-BAND DOPPLERRADAR MODULE
CL8965
Vertical B
Horizontal pQH<>
Polar diagram for antenna supplied.
MilliardCL8965 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antenna
are mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-sions as shown on page 9.
In this configuration, the metal plate forms the front panel of the equipment, andthe antenna radiates into free space. If the equipment housing is all metal , anyback radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42/xA.
(35fiA d. c. bias + 7piA from - l9dBm of coupled 1. o. power.
)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture, then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic material
is detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will nowbe approximately 60fiA.
The increase in l.o. power will, in general give rise to an increase in a.f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled l.o. power arising from the useof thick or ' microwave' reflective covering materials, will:
(a) continue to increase die a. f. output voltage from the mixer (N. B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching andrunning performance and may 'pull' the frequency outside the allocated operat-
ing frequency band.
The following table compares the 1. o. coupling level obtained for different coveringmaterials at the antenna.
L. 0. coupling
@Bm)Mixer total bias
(MA)
Antenna covering
material
- 35 (d.c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene orpolystyrene
-11 61 0. 25mm Gobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division,
Brantham Works
,
Brantham
,
Manningtree, Essex CO 11 1NJ
MullardCL8965 Page 8
X-BAND DOPPLERRADAR MODULE
CL8965
'Cobex' plastic sheet(or equivalent)
M4 screw
Aluminium panel1.6mm (16s.w.g.)
2 holes drill
04.2-CSK 07.0
Cobex 0.25mm sheet
Panel mounting details
MullardCL8965 Page 9
X-BAND DOPPLERRADAR MODULE
CL8967
QUICK REFERENCE DATA
Fixed frequency Gunn oscillator and mixer cavity for operation In tne 10. 4GHz
band. Applications Include all forms of Doppier radar systems,
10.365Centre frequency
Rower output (at 7.0V) typ.
Output voltage {typ. ) for Input power
lOOdB down on output power
_ _. , signal + noiseat l8dB mln. —E—
noise
{see page 6 and note 1)
Supply voltage
10
40
7.0
GHz
mW
V
MilliardOCTOBER 1978 CL8967 Page 1
OPERATING CONDITIONS
Supply voltage (see note 2)
Supply current (see note 3) (typ.
)
D. C. mixer bias current (into a. f.
terminal w. r. t. earth)
A.F. load (see page 5)
RATINGS (ABSOLUTE MAXIMUM SYSTEM)
Supply voltage (max. d. c.
)
Supply voltage transient max.(1.0ms max.)
Tstg range
Tamb ranSe
CHARACTERISTICS at 25 °C
Centre frequency
Output voltage for input powerlOOdB down on output power (at
, ,n signal + noise. .
18dB mm. —*: ) (see
noise
notes 1 and 4 and page 6)
Output power at 7. 0V
Frequency fixed
Frequency temperature coefficient
Frequency pushing
Second harmonic
Diode current (see note 3)
Polar diagram
MASS
20
10.353
+7. ± 0.
1
V
140 mA
30 to 35 MA
10 kn
+7.5
9.0 V
10 to +70 °C
to +40 °C
Min. Typ.
10. 365
40
10
10. 365
-0.2
4.0
-35
130
see page 7
170
Max.
10. 377
-0.3
165
GHz
mWGHz
MHz/0C
MHz/V
dBm
mA
Alternative antennae and operating frequencies may be made to suit customers'specific requirements.
MilliardCL8967 Page 2
X-BAND DOPPLER CL8967RADAR MODULE
OPERATING NOTES ^_
1. A return signal lOOdB down on radiated power will be achieved from a mantarget of radar cross-section 1.0m2 at a range of 15m, when operating with the
antenna supplied (antenna gain is 5dB typ. ).
signal + noise ,. ,
Extended range may be obtained for a reduced : and this may be° ' noise
acceptable if the environment in which the system operates is stable, i.e. , free
from extraneous moving or vibrating objects. For example, HOdB path loss is
obtained from a man target of radar cross-section 1.0m2 at a range of 25m and
the ———: is reduced to 15dB with an output voltage of 16/iV min.noise
Alternatively, the range may be increased by an increase in target radar cross
-
section or by the use of a high gain antenna. The performance may then be
calculated from the radar range equation. Further related information may be
obtained on application to Mullard Ltd.
2. It is essential that the earth terminal is used as the common return for the Gunnvoltage (+7V) and the d.c. bias supplied to the a. f. terminal.
3. The Gunn effect device has a voltage current characteristic as shown on page 5.
The power supply should have a low source impedance and be capable of supply-
ing up to 250mA at approximately 3V during the switch-on phase.
4. Noise measured at a frequency 1Hz to 1kHz from carrier.
5. The Gunn device will be damaged if the supply is reversed.
6. The module is supplied with a protection circuit connected between the mixer
a. f. and earth terminals. The mixer has a low junction capacitance and may be
damaged by transients of very short duration. It is therefore recommended that
soldering irons are isolated from mains supplies and that the protection circuit
is not removed when all wiring has been completed.
7. Precautions similar to those required for CMOS devices are necessary , namely
:
a) Earthed wrist straps should be worn.
b) Table tops or other working surfaces should be conductive and earthed.
c) Anti- static clothing should be worn.
d) No electrical testing should be carried out without specific, approved and
written test procedures.
e) To prevent the development of damaging transient voltages , devices should
not be inserted or removed from test fixtures with power applied.
8. The above conditions apply when operated into the antenna supplied with the
module.
9. A lOnF capacitor should be connected across and close to the +7V and earth
terminals to suppress parasitic oscillations in the power supply.
10. —™-
. performance may be degraded if the antenna is covered by a
radome of unsuitable construction. Page 8 describes the preferred arrangement.
MullardCL8967 Page 3
OUTLINE DRAWING
*2 holes 0L2/LO51.5/51.0 centres
27.4.
Recommended screws -M4
Z_
KAntenna
12.3
MilliardCL8967 Page 4
X-BAND DOPPLERRADAR MODULE
CL8967
I mn»250
Max 165 Max curve
P«3 7 Voltage (V)
Gunn device characteristic
©9 A.F. terminal
CL8967
X
+ 7V
1R1
iookn
CI
R2ioi<n
Bandwidth 1Hz to 1kHz
Z in >100kn
Notes
Qrcuit used to measure A.F. performance
1. The current lb should be approximately 35fiA with the Gunn device disconnected
and approximately 42/xA with the Gunn device operational and the antenna oper-
ating into free space.
2. The coupling capacitor should have a small impedance compared with Z^.
MilliardCL8967 Page 5
> 1000
^ 7
100
10
vf: ee1
Metres
N1ax \— - n
li
oise — ^~
jvel
—
I
10 100 1000
Target range (m and ft)
Minimum output for a man target
MullardCL8967 Page 6
X-BAND DOPPLERRADAR MODULE
CL8967
Vertical B
Horizontal pQD
Polar diagram for antenna supplied
MilliardCL8967 Page 7
MODULE MOUNTING
For optimum signal to noise ratio , it is recommended that the module and antenna
are mounted, using M4 screws, to a 1. 6mm thick metal plate with aperture dimen-
sions as shown on page 9.
In this configuration, the metal plate forms the front panel of the equipment, and
the antenna radiates into free space. If the equipment housing is all metal , any
back radiation will be totally contained. Alternatively a metal based adhesive tape
may be used to seal the joint between antenna and mounting plate.
The total mixer bias under the optimum operating conditions is approximately 42/iA.
(35juA d.c. bias + 7/iA from -19dBm of coupled 1. o. power.)
If, however, for environmental reasons, it is considered desirable to cover the
antenna aperture, then it is recommended that a thin plastic material (approximately
0. 25mm thick) is fixed to the metal plate with adhesive. A suitable plastic material
is detailed on page 9.
In this case, the l.o. power coupled to the mixer will be -lldBm, and the total
mixer bias current will now be approximately 60(xA.
The increase in l.o. power will, in general give rise to an increase in a.f. output
voltage for a given target , but this will be accompanied by a degradation in signal
to noise ratio. For -lldBm of l.o. power, the degradation in signal to noise ratio
should be acceptable for most applications.
However, further increase in the level of coupled l.o. power arising from the use
of thick or ' microwave ' reflective covering materials , will :
(a) continue to increase the a.f. output voltage from the mixer (N. B. the increase
will not be the same for all modules) but at the same time, degrade the signal
to noise ratio.
(b) present a mismatch to the Gunn oscillator which may impair the switching and
running performance and may 'pull' the frequency outside the allocated operat-
ing frequency band.
The following table compares the l.o. coupling level obtained for different covering
materials at the antenna.
L. 0. coupling
(dBm)
Mixer total bias
(jxA)
Antenna covering
material
- 35 (d. c. only) -
-19 42 No covering
-15 50 1 to 2cm expanded
polythene or
polystyrene
-11 61 0. 25mm Gobex plastic
-6 70 0. 5mm Cobex plastic
Cobex is a product of: British Industrial Plastics
,
Sheet and Film Division
,
Brantham Works*
.
Brantham,Manningtree, Essex CO 11 1NJ
MilliardCL8967 Page 8
X-BAND DOPPLERRADAR MODULE
CL8967
Cobex' plastic
sheet (or equivalent)
M4 screw
Aluminium panel
1.6mm (16s.w.g.)
2 holes drill
0U.S -CSK
Cobex0.25mm sheet
MullardCL8967 Page 9
MISCELLANEOUS
H
H
MICROWAVEHORN ANTENNA ACX-OIA
TENTATIVE DATA
A general purpose X-band antenna for miniature radar systems.
The unit gives a low v. s. w. r. and is of a strong cast construction.
CHARACTERBTICS
Frequency range
Gain
Beam angle (both planes)
v.s.w. r. max.
MECHANICAL DATA
Weight
Flange
9.0 to 11 GHz
16 dB
30 deg
1.2
160 g
UBR100 (UG135/U)
OUTLINE DRAWING
Atl dimensions in mm
MAY 1976Milliard
ACX-01APage 1
X-BANDMIXER/DETECTOR
CL7500
Waveguide single ended mixer designed, for use in the 10. 7 GHz band. It is primarilyintended for Doppler control systems, e.g. intruder alarms deriving local oscillator
drive from the transmitter output of a Gunn effect device such as Mullard CL8630.The CL7500 can be used as a microwave detector. Two examples of this are sensingdeliberate beam obstruction in a microwave protected area and as receiver in a micro-wave barrier or fence.
ELECTRICAL CHARACTERISTICS (at 25 °C)
Centre frequency
Mixer
Sensitivity for -95 dBm input
Noise level (32 nA d.c. bias,
1 Hz to 1 kHz bandwidth) J)
Detector
min.
typ.
typ.
max.
Tangential sensitivity at centre frequency typ.
10.687
QUICK REFERENCE DATA
Centre frequency 10. 687 GHz
Typical sensitivity for -95 dBm input 15 nv
Typical noise level (32 pA d.c. bias,
1 Hz to 1 kHz bandwidth) 1.0 HV
LIMITING VALUES (Absolute max. rating system)
IR (max.
)
5.0 mA
IpM P63^ forward current (max.
)
10 mA
Tstg range -10 to +100 °C
TYPICAL OPERATING CONDITIONS
Tamb range -10 to +50 °C
Local oscillator level -18 dBm
D.C. bias 32 VA
Total load (d.c. and i.f.
)
10 kn
GHz
Tangential sensitivity from 10. 1 to 11.0 GHz 2) typ
10 MV15 MV
1.0 \iV
2.0 MV
-50 dBm-49 dBm
Notes see page 2
JULY 1976Mullard
CL7500Page 1
OUTLINE DRAWING
-19.8
<
45.2
-15.9-H
31.0 41.3
All dimensions in mm
) When the local oscillator power is derived from a Gunn source with an a.m. noise to
carrier ratio of 94 dB (typically Milliard CL8630), the minimum sensitivity specified
represents a signal to noise ratio at the mixer output of 10 dB (typically 17 dB)*
2) When operated as a detector with 32 fiA. d. c. bias, measured in a to 2 MHz bandwidth.
3) The diode may be damaged if the bias supply is reversed.
4) The mixer diode will be damaged by forward current in excess of 10 mA. The moduleis supplied with a shorting strap connected between the mixer a.f. and earth terminals.
The mixer has a low junction capacitance and may be damaged by transients of veryshort duration. It is therefore recommended that soldering irons are isolated frommains supplies and that the shorting strap is not removed until all wiring has been
completed.
5) Connections to be made to W.G. 16 components.
MilliardCL7500Page2
X-BANDMIXER/DETECTOR
CL7520
Waveguide single ended mixer designed for use in the 9. 35 GHz band. It is primarily
intended for Doppler control systems, e.g. intruder alarms deriving local oscillator
drive from the transmitter output of a Gunn effect device such as Mullard CL8631 orCL8632.
The CL7520 can be used as a microwave detector. Two examples of this are sensingdeliberate beam obstruction in a microwave protected area and as receiver in a micro-wave barrier or fence.
QUICK REFERENCE DATA
Centre frequency 9.35 GHz
Typical sensitivity for -95 dBm input 15 MV
Typical noise level (32 pA d. c. bias
,
1 Hz to 1 kHz bandwidth) 1.0 mv
LIMITING VALUES (Absolute max. rating system)
IR (max.
)
IpKj P^k forward current (max.
)
l stgrange
TYPICAL OPERATING CONDITIONS
Tamb range
Local oscillator level
D.C. Mas
Total load (d. c. and i. f.
)
ELECTRICAL CHARACTERISTICS (at 25 °Q
Centre frequency
Mixer
Sensitivity for -95 dBm input
Noise level (32 jjA d.c. bias,
1 Hz to 1 kHz bandwidth) 1)
Detector
Tangential sensitivity 2)
min.
typ.
typ.
max.
typ.
5.0 mA
10 mA
10 to +100 °C
-10 to +50 °C
-18 dBm
32 MA
10 kfl
9.35
10
15
1.0
2.0
50
GHz
MVMV
MVf*V
dBm
Notes see page 2
JUNE 1978Mullard
CL7520 Page 1
OUTLINE DRAWING
t— 23.05-*) (—18.52-)
62.0
cur nrj
4 holes
4.4
4.3
41.3 -
[- 32.5 -j
[f -f1
,,
£ 31.0 41.3\k- -*,
All dimensions in mm
!) When the local oscillator power is derived from a Gunn source with an a. m. noise to
carrier ratio of 94 dB (typically Mullard CL8631 or CL8632) , the minimum sensitivity
specified represents a signal to noise ratio at the mixer output of 10dB (typically 14 dB).
2) When operated as a detector with 32^A d.c. bias, measured in a to 2 MHz bandwidth.
3) The diode may be damaged if the bias supply is reversed.
4) The mixer diode will be damaged by forward current in excess of 10 mA. The module
is supplied with a shorting strap connected between the mixer a. f. and earth terminals.
The mixer has a low junction capacitance and may be damaged by transients of very
short duration. It is therefore recommended that soldering irons are isolated frommain supplies and that the shorting strap is not removed until all wiring has been
completed.
5) Connections to be made to W.G. 16 components.
MullardCL7520 Page 2
CL9022
PARAMETRIC AMPLIFIER
A single-diode non-degenerate parametric amplifier designed for use as a low-noise pre-amplifier in
microwave applications. It is supplied in a temperature stabilized enclosure with a solid state Gunn-
effect oscillator pump and integral power supply.
QUICK REFERENCE DATA
Power gain
Tuning range min.
Noise figure max.
Bandwidth
Input and output impedance
Mains supply
20
2.7 to 3.1
2.8
15
50
240 V, 2A, 50 Hz
dB
GHz
dB
MHz
ft
MECHANICAL DATA Dimensions in mm
231 max-
Gain Gainadusting control
key access
p—249 max 80max
C
C
C
i
r
|--12i
Signal input
Type N pt"female coaxial
connectors
Signal output'
Mains input
(Plessey
connector)
74.
max
Tuning
Part view showingmicrometer guardremoved
u MilliardMay 1978
CL9022
RATINGS
Limiting values in accordance with the Absolute Maximum System (IEC134)
Continuous r.f. input power max.
Input spike energy max.
Mains supply voltage max.
Ambient operating temperature range
Storage temperature range
CHARACTERISTICS {note 1)
Tamb=25°C
Power gain (recommended setting) (note 2)
Operating frequency
Noise figure
Bandwidth (note 3)
Input saturation level (note 4)
Gain stability per hour
per day
Mains voltage supply limits
MASS
100 mW500 nJ
276 Vac
20 to +55 oc
•30 to +70 °C
mm. typ. max.
- 20 - dB
2.7 - 3.1 GHz- 2.6 2.8 dB
12 - 18 MHz
-35 -32 - dBm
±0.1 dB
±0.5 dB
204 240 276 Vac
5.4 kg
Notes
1. These are given for matched conditions.
2. The gain-set attenuator is adjusted with the hexagonal key provided.
3. Measured to the 3 dB points at a gain setting of 20 dB.
4. This is the input level at which the gain is compressed by 1 dB, at a gain setting of 20 dB.
5. The amplifier is designed for ease of maintenance; both the temperature control system and the
Gunn oscillator power supply use field-replaceable plug-in boards.
May 1978
Milliard U
ISOLATORS ANDCIRCULATORS
ISOLATORS AND CIRCULATORS
GENERAL
Contents
Isolators and circulators, general section
Coaxial circulator series, bands IV — V, 100 W, u.h.f., TV
Coaxial circulator series, 300 W, u.h.f., TV
Coaxial circulator series, 500 W/1 kW, v.h.f., TV
Coaxial circulator series, bands IV - V, 500 W/2 kW, u.h.f., TV
Coaxial circulator/isolator series, octave bandwidth
Coaxial circulator/isolator series (3-port versions), standard bands
Coaxial circulator series (4-port versions), standard bands
Waveguide circulator series (3-port versions)
Waveguide circulator series (4-port versions)
Industrial heating isolators
Waveguide isolator series
Conversion lists of CL numbers to catalogue numbers and vice versa
page
1
8
10
12
14
16
20
23
24
26
28
30
34
u Milliard
GENERAL
ISOLATORS AND CIRCULATORS
riVTRODUCTION
Only a brief general description of isolators and circulators is given here: those readers seeking fuller
information are referred to our Application Book 'Isolators and Circulators'.
Isolators
An isolator is a passive non-reciprocal device which permits microwave energy to pass through it in onedirection whilst absorbing energy in the reverse direction. In the forward direction, that is the directionin which the energy is passed, the insertion loss is usually 0,3 to 0,5 dB in the frequency range forwhich the isolator has been designed. In the opposite direction the isolation is normally 30 dB butfor certain applications isolation can be made as high as 55 to 60 dB.
In the field displacement type of isolator, which is described later, a ferrite bar is mounted in a wave-guide and biased by a magnetic field. The non-reciprocal t ->haviour of this type of isolator is producedby gyromagnetic effects which occur between the high frequency magnetic field and the electrons in
the ferrite.
Circulators
A circulator is a passive non-reciprocal device with three or more ports. It contains a core of ferrite
material in which energy introduced into one port is transferred to an adjacent port, the other ports
being isolated.
Although circulators can be made with any number of ports, the most commonly used are 3-pcrt and4-port, the symbols for which are given in Figs 1 and 2.
Fig. 1 Symbol for 3-port circulator. Fig. 2 Symbol for 4-port circulator.
Energy entering port 1 emerges from port 2; energy entering port 2 emerges from port 3, and so on in
cyclic order. In this direction of circulation an ideal circulator would have no losses, but in practical
constructions there are some losses.
In an ideal circulator no energy would flow in the direction opposite to the circulation direction. Againin practice this isolation is in the order of 20 to 30 dB; in very narrow bands it is even higher. The non-reciprocal behaviour of circulators is the result of gyromagnetic effects in the ferrite when this is biased
with a magnetic field.
u MilliardSeptember 1977
GENERAL
APPLICATIONS
Isolators
JK.
The main application of an isolator is to improve the behaviour of klystrons, magnetrons or travelling-
wave tubes by isolating the source from the load. The main factor is that an antenna or amplifier can-
not be matched ideally to the preceding function over the required frequency range, so that energy
would be reflected back into the tube and upset the frequency stability. The isolator will absorb this
reflected energy so that the tube is effectively protected from these disturbing influences.
The isolators are provided with adjusting screws that enable them to be matched so that the v.s.w.r. is
minimum over a certain frequency range. It is therefore possible to optimize the efficiency of wave-
guide runs by matching the isolator to minimum reflection. This means that long line effects can be
drastically reduced.
Circulators
The main application of circulators is the duplexing of systems for simultaneous transmission and
reception in low and medium-power telecommunication equipment; this is illustrated in Figs 3 and 4.
(b)
0---6—5—
i
<
Fig. 3 Duplexing one receiver and
one transmitter with (a) a 3-port
circulator and (b) a 4-port.
Fig. 4 Duplexing of a number of transmitters (T)
and receivers (R).
The reasons that both 3-port and 4-port circulators are used are:
- a 3-port circulator usually has a wider bandwidth than a 4-port circulator;
- a 4-port circulator (of which the fourth port is provided with a matched load. Fig. 3(b)), however,
does not require a very accurately matched receiver, so that a much simpler filter can be used on
the receiver input.
A 3-port circulator can also be used as an isolator by putting a matched load on one port; Fig. 5. The
characteristics of a circulator performing a decoupling function are superior to those of an isolator,
particularly at the lower frequencies. Decoupling can be increased by cascading circulators. Decoupling
and insertion loss are directly proportional to the number of circulators. For additional information
refer to our Application Book 'Isolators and Circulators'.
September 1977
Mullard r?
Isolators and circulators GENERAL
(a)
-Q^MD^-Q^(b)
Fig. 5 A 3-port circulator used as
an isolator.
Fig. 6 Cascaded circulators (a) in H-configu ration,
(b) ^--configuration.
CONSTRUCTION
Waveguide isolators
A field displacement isolator is shown in Fig. 7. The ferrite bar (1) can be seen inside the waveguide,
flanked by two sets of magnets (2) outside the waveguide. These magnets bias the ferrite bar. The ad-
justing screws (3) protruding into the waveguide are used to match the isolator for minimum voltage
standing wave ratio.
Fig. 7 Field displacement isolator.
Waveguide circulators
Three or four waveguides intersect at angles of 120° or 90° respectively in this type of circulator. A4-port waveguide circulator of the junction type is shown in Fig. 8. A piece of ferrite (1 ) is located
between two magnets (2) exactly in the centre of the intersection. Posts (3) are placed in the wave-
guide to achieve a good match.
V MilliardSeptember 1977
GENERAL
Fig. 8 Construction of a junction type waveguide circulator.
Coaxial circulators
A coaxial circulator of the junction type is shown in Fig. 9. Three copper strips (1 ) intersect at 120° in
the centre of the circulator. The strips are mounted between two earth plates (2) to form a matchedhigh-frequency conductor. Two ferrite discs (3) and magnets (4) are mounted in the exact centre of the
circulator.
Fig. 9 Construction of a junction type coaxial circulator.
TERMS AND DEFINITIONS
Frequency range
This is the range within which the isolator or circulator meets the guaranteed specification. Outside
of this range the electrical properties deteriorate rapidly. Circulators, however, will not be damagedif erroneously subjected to frequencies outside the range.
September 1977T Milliard V
Isolators and circulators GENERAL
JKIsolation
In an isolator, isolation is the ratio of the input power to the output power in the reverse direction,
expressed in dB. The power measurements are made with matched source and matched load.
In a circulator, isolation is the ratio of the energy entering a port to the energy scattered into the
adjacent port in the reverse direction to normal circulation, expressed in dB. Measurements are made
with a matched source and all other ports correctly terminated. The isolation between ports 1 and 3,
«1_3, is equal to eg—2 and «2— 1 ^'9- ')•
Insertion loss
This is the attenuation which results from including an isolator or circulator in the transmission system.
Insertion loss is the proportion of power lost between the ports of the device when energy is travelling
in the forward direction, expressed in dB. Measurements are made with the input and output matched.
Voltage standing wave ratio
The v.s.w.r. is the ratio of the maximum voltage to the minimum voltage along a lossless line. In cir-
culators the v.s.w.r. is measured with all unused ports terminated by a matched load. Coaxial circulators
are designed with a characteristic impedance of 50 ohms.
Maximum power
Under no circumstances should the maximum power value for isolators and circulators be exceeded.
In an isolator, the maximum power is the largest power that may be passed through it in the forward
direction into a load with a v.s.w.r. of 2.
In a circulator, the maximum power is the largest power that it can handle at sea level and maximumambient temperature — and with cooling applied if specified in the data — when one port is terminated
with a mismatch having a v.s.w.r. of 2, and the next port is matched having a v.s.w.r. < 1,2.
The maximum power for coaxial circulators is the maximum continuous-wave power unless a maxi-
mum peak power is separately stated. These power levels should not be exceeded.
The peak power is the maximum peak sync power as defined by the CCIR signal standard. This value
is given for isolators and circulators at the v.h.f. and u.h.f. television frequencies. If this value is ex-
ceeded the isolator or circulator can be damaged by arcing in its internal transmission structure.
Peak power values are valid for one signal passage only.
Since the sound power Ps passes through the circulator twice in a signal-combining circulator, the
average power when Ps = 0,2PSync is given by P * 1,17PSync
.
Under worst-case conditions, the peak power produced for the same signal is given by
pM -V Psync +V Ps = Psync M + 2V<>,2)2 - 3,6Psync .
Temperature range
The ambient temperature range within which isolators and circulators function to specification.
(When necessary, special temperature compensation is built in for circulators.) Circulators still function
outside the temperature range but their electrical behaviour may be far outside the guaranteed specifi-
cations. However, no permanent damage can be expected unless a large temperature rise is caused by
excessive power handling.
The storage temperature of isolators may be from —40 to + 125 °C unless otherwise specified in the
data.
U Milliard 1 September 1977
GENERAL
_yv_CAUTIONARY NOTES
1. Isolators and circulators have internal magnetic fields that are carefully adjusted for optimumoperation.
2. Isolators and circulators are not to be subjected to strong external magnetic fields.
QUALITY GUARANTEESubject to the Conditions of Guarantee the Manufacturer guarantees the isolators/circulators supplied
to the purchaser to meet the specifications as published in the Manufacturer's Data Handbook and to
be free from defects in material and workmanship.
Under this guarantee the Manufacturer will within one year after shipment to the original purchaser
repair or replace at the Manufacturer's option, free of charge, any isolator/circulator proved by the
Manufacturer's inspection to be thus defective.
STANDARD TEST SPECIFICATIONS
Initial measurements
These measurements have been carried out at room temperature and at the extreme temperatures, with
a power level not exceeding 10 mW.
Tropical test
This test has been carried out completely in accordance with IEC 68 test D, accelerated damp heat.
This test begins with the temperature at 55 + 2 °C and R.H. at 95 to 100% for a period of 16 hours,
followed by a period of 8 hours with the temperature at + 25 °C and R.H. 80 to 100% to complete the
24-hour cycle: the test consists of 6 uninterrupted cycles.
Vibration test
This test has been carried out completely in accordance with MIL-STD-202D, method 201 A: frequency
range 10 to 55 to 10 Hz for 2 hours in each of the X, Y and Z directions, with a total excursion of
1,5 mm.
Thermal shock test
This test has been carried out completely in accordance with MIL-STD-202D, method 107C undercondition A: 5 cycles with extreme temperatures of —55 °C and +85 °C; duration of one cycle is
1 hour.
Mechanical shock test
This test has been carried out in accordance with MIL-STD-202D, method 213A under condition G;peak value 100 g, duration 6 ms, and also with extreme peak values up to 800 g, duration approxi-
mately 1 ms for each device, referring to the results of the drop test.
Drop test
This test has been carried out in accordance with ISO 2248, part IV: packaging complete, filled trans-
port packages, vertical impact.
R. F. power test
The devices have been tested in accordance with the definition of maximum power in the Data Hand-book (v.s.w.r.= 2). The ambient temperature of 25 °C was increased to the maximum operating tem-
perature and the duration of the test was 1 hour for each device.
September 1977"Y Milliard D
Isolators and circulators GENERAL
Final measurements
On completion of the above tests final measurements were carried out at a temperature of + 25 °Cand with a power level not exceeding 10 mW. The results of these tests should be within the guaran-
teed values.
Dimensions and visual appearance
These have been checked in accordance with the published data.
Note
On request, different tests and/or additional tests to those above can be carried out.
c? Milliard 1September 1977
COAXIAL CRCULATORS100 W, UJHF., TV
OO
m co co^- in in cm
3 *- CO «- r- CO» 8 o o o o<D t
CM CM CM CM<o CO CO CO
£ 3O t CM CM CM CM
CM CM CM CMr»> r-s r* r>CM CM CM CM
.« xa o
E &w 8 O O Qo © o
•* ^J- ^- *
,_o _w _a> _aj _a>
* E illa> a> a> a>c H- »«- H- H-
oo z 2 2 2
Q) o o o o3 CO CO CO CO*-•
03
+ + + +O o o o oo *J
o o o o1 1 1 1
flj <o c o o o o§
• > o o o oa & CM CM CM CM
*5X(0
eS 8 8 8 8d *~ ^ f— T—
in id in *o.>+-*
5 c m in in in(0 TO CN CM^ CM^ CM_
> fc 0>to a>3 +5 V V V V
U) in in
1c
Q. eno*
CO CO COo* o* o"
c~ m c
(A
ra to
to <u
in
oin in mo* o* o
C ft*' V V V V
ain in in in
c CM CM CM CMo'+j CD<0 "D cO <o "a o o o o.12 <5
* CM CM CM CM3 +- A AAA
>uC ay
o 8 8 §9) 9) N «» CO CO «-3 C X
51oo
1 1 Io o or» o en
f- * «a- to r»
o «
° £
o 52"5 O
t H
E £
V) oCo J2
<0 >c:
X)
F <o
o Oo
September 1977T Mullard C?
Isolators and circulators COAXIAL CRCULATORS
100 W, U.HF., TV
r- IQ (O (0tf SS tO CMCO t- r- COO O O O
u Mullard If September 1977
COAXIAL CRCULATORS300 W, U.HF., TV
XD
OoCO
COyDCIII
CO
CCOI-
DOCC
o-I
X<oo
CM tN CM CM CM CM CM CMS W 00 CO e» ^- COin co tn to tn CO CO CD
-1o o o o o o o oCM CM CM CM CM CM CM CMCO CO CO CO CO CO CO CO
o *- CM CM CM CM CM CM CM CMCM CM CM CM CM CM CM CMr«« r>. i-» fv r^ r*» l-» (^CM CM CM CM CM CM CM CM
X8 2
E a(0
O) 8 8 8 OO OO oo 8 ooCM CM CM CM CM CM CM CM
o « CO .2? CO 0J CO a> CO
* 1CO CO
E ?; E r>. bCD
1** E I--
*T U. *T LL **7 u. LLo 2 I Z I z I z I
a> o o o o o o o oZ3 CO CO CO CO CO CO CO CO
s & Oo
+ + +o o o
+o
+o
+o
+o
+o
a. re
E*"
*•* *-»
o o o o o o o oa>
1 1 I 1 1 1 1 1
CO c o o o o o o o o5 se > o o o o a o o o
Q. « If) tO IT) in m in tn tn
a §X
g o o o o o a o oE
o o o o o o o oo CO CO CO CO CO CO CO 00
in m in in in in tn in
>
$c in m in in in in in in(tj T3 CM CM CM CM CM CM CM CM>CO Q>
O) V V V V V V V Vo o o o o o o oCM CM CM CM CM CM CM CM
.is
** o o o o O O O o
c in m in m in in in tnco X} CO CO CO CO CO CO 00 00CO OJ o o o o o o o o
c o> V V V V V V V V
a.in in m in tn in in in
•2 mCM CM CM CM CM CM CM CM
TO "D,
OV)
cro "a o o o o o o o oCO Q) CM CM CM CM CM CM CM CM
j
D) AAA A A A A A
>- o o o 8 o o o oc 92, N
Ir* i^- o CM CM CO CO^ <f (D
1 1 1
CO1 1 1
001
001
a- 2 5 o o o o o c^ o oo o r» r~» en o>"*" *t * >« <s- to m r»» f»»
aj _ca
O O
10 September 1977Y Milliard V
Isolators and circulators COAXIAL CRCULATORS300 W, U.H.F., TV
CM CM CM CMCM CO ^ (0(0(0 0(0
Ifl-
«-l
1o'oi+ —
Tt
-W
5e
U,
t
w
I Em in
Ji
CM CM CM CMMB 9 ^to 2S io «o^ T- T" 1-o o o o
1 'Li
iii
! K
U Mullard ySeptember 1977 11
COAXIAL CIRCULATORS
500 W/l kW, V.H.F., TVV_
U.
X>
I
oomCOUJ
ccLXJ
CO
cco
3occ
o-J<X<8
!*• O CO O) in oo l*~ 00
« CO CD CO CO 00 00CO CO
» s o O o o o o o o5 E
CM CM CN CM CM CM CM CM<0 CO CO CO CO CO CO CO
-• 3(0 c CN CM CN CN CN CN CN CN
CN CN CN CN CN CN CM CMr>» l~- l-» 1^ i-» r» r» r*CM CM CN CM CM CM CM CM
X
<2 D.E Q.
o> 8 Oin 8 o
ino oo in
o oo in
re CM CM CN CM CM CN CM CM
o 01CO 0) CO « CO .22 co
3) Q.
§ £ou
re
Ea>
>- Ea>
r» i - 1 -LL LL V u. T u.
Z I Z I Z I Z X* * • *
£ o c o o o o o oto ^f CO «* CO rt co «d-
re S, Oo
+ + + + + + + +o o o o o o o o
+j +-Q. re
E o o o o o o o o
o
Xre
E
.* o oin 8 o
inoo m o in o
00 00 00 00 CO CO CO 00
ooin
o8 in o
o oin o 8 8
in oo *" *"" ^ T~
a>in in in in in m in in
j
5 in in in in in in in in<0 73 CM CM CM CM CM CM CM CM
>re §>3 w V V V V V V V V
8JO
c.2 oa
Q. CO CO CO o CO CO CO CO> o o o o o ,o o o
m in in in in in m mre <D 0)
COo
COo*
CO
o"COo"
CO CO
o o*CO CO
o* o"c 3 *-• V V V V V V V V
Q. ^- ^r ** * Tt •* *fr "*CM CN CN CM CN CN CM CM
o•^ CDre -o C ,,o re TJ O o O O O O O O... re a) CM CM CM CM CM CM CN CM
§>~ A A A A A A A A
>o a,CO CO
r-. 3 s o oCO CO
o oI *— *— CM CN CM CN CM CM
8-s S 1o A 1
CO1
CO 441 1
in m(0 CO r^- r» CM CM
*• ^" CM CM CN CN
12 September 1977¥
•— do
a> min
o +oyi- g)
re 3x:
5 a.
•
Mullard r?
Isolators and circulators COAXIAL CIRCULATORS500 W/1 kW, VJHR, TV
S<o rs r*.00 CO ^
«~ *- «~ coo o o oCMtt>
82 o cooo o> *-
^ *r *- coo o o o
~ca
MullardSeptember 1977 13
COAXIAL CIRCULATORS500 W/2 kW, UMF., TV
U.
Z>
ICM
OolO
COQz<CD
COyorLUCO
ccO
3Occ
o-I<X<oo
CM CO CO 00 CO ^r r»
a>CM CM CO r- CM
CO t
O o o o o o oCM CM CM CM CM CM CMCO CO CO CO CO CO CO
e 3S c
CM CM CN CN CN CM CMCM CM CM CN CN CM CM1^ 1^ r»- r>- r»» r» r>»
CM CM CM CM CM CM CM
w) O
c a.
o> O00O |
O00o
o8 8o 23 So o
(0 CM CM CM CM CM CM CM
* * *w * * •O CO CO CD CO CO. » CO
a> a.5 >•
CO CO CO «-
E r^ ECO
f~ r^ E ^cu
Oou. u. u. T u-
Z X Z X X Z X* * * *
ai o o O o o o ok. r»» Tf r»» ^> «» r- tti <u + + + + + + +2 S> o o o o o o o o
4-* +» *»Q. TO
E*" £ o o o o o o
<u
o
X
+. .* o> CO c^ CD >.o a. ST
8 § 80) §
o8 8 8
o> oCN CN CN CM
58 £ 8 g 8 8 8in m m o
E u CN CN CM CM
in CM in CO m m>+•
5
l"gin in
>'CM CM CN CN CM CM CM
co a>3 * V V V V V V V
in r-. in in r-> m coin Q. CM CM CM r-
C
> o o o o o o o
O 00
S-RHi in in m m in inCO CO CO CO CO CO CO
a>inC
co a. oV
oV
oV
oVOV
o ©V V
a«*• *t * i^ «r Tf CDCM CM CM CN CN CM CM
<D "O ,
oCO $
CM O CN CM o CM CNCM CM CM CM CM CN CM
3 <"A A A A A A A
1
O* CO
8 o o o o o oo CM CM o CO CO
X2
CO1o
CO1o 1o ci
001
8
00 001 1o o
r» r-» a> OJH- *» *r in in CO r> r»
Ooo*fr 00
b in3 rE <XCO HI
E •a-o cc(0
c op
F r>-
o <oCJ Hifc_ »a>
CO<o CM< CM
f^E tE zinCM Q^_ Oo
a. XCO
j_o<->
Mu co cCB o ooE o
CO
+in
5CD
oo cu .Q
u -}
.t CO CO>
CD
-C a ob (A
£ CD <
14 September 1977T Mallard U
Isolators and circulators COAXIAL CIRCULATORS500 W/2 kW, UJ4F., TV
o o o o2
a
~ffl
-*i-
u Mullard rSeptember 1977 15
COAXIAL
CIRCULATORS/ISOLATORS,
OCTAVE BANDWIDTH
Q
QZ<CD
LU>
ooCO
ccLUCO
CC
R
o
cco
DOCC
o
OO
o> O 8 O r^ CM CM O CMt in in o 00 CO CO CNCM CM CM CN CN CO CM
2* o o o O O o O o o o O O Oof CM CM CM CM CM CM CN CN CN CN CM CN
CO SO CO CO CO CO CO CD CO CD CO CO
S c CM CM CM CN CM CM CN CN CN CM CM CMCN CM CM CM CM CM CM CM CN CM CM CMr» r~ r- r-» !-* r-> r^ r-» r~- r^ r* r-«-
CN CM CM CM CN CN CM CM CM CM CN CM
(0 L.
E °~
oo oo OO 8 OCM
OCM 8 8 o
CO 8 o oCM CM
CO CO CO CO ^" ^ ^ *— ^<o
wo 93 0)
E < E < < < < < < < < <5= S 5 S 5 s 2 s 2 5
u ^ CO J: CO CO CO CO CO CO CO CO CO
£a o o o o o o o o o o or» (*- i*» l-> r- r-. r- r» r» r> I
s* f»
IS (U + + + + + + + + + + + +2 o)
Ea>
Oo
o
oo
oo
oo
oo
oo
oo
oo
oo
oo
oo o
o o4->
a>
a>>a> 1 1 in m 1 m 1o
1 1 1
""
5 0)
o^5 aX b.(0
E ?o o o o o o o o o a in mm m in in CM CM r- ^-
£ID m m m in CMa CM CM
S5
-"8 m m m m in m m m in in o mCM CM CM CM CM CM CM CM CM CM CO CM
> • *ft' V V V V V V V V V V V V
in in in in in m in
1o CO
a COo*
COo"
CO COo*
COo*
CO
o"COo"
COo o'
COo
CO COo" cf
,
c"° 2^ m in m in in in m in CO CO CO CD
8 oVoV
oVoV
oV
oV
oV
oVoVoV
o" oV V
a *.• ^- ^ «t r*. i>. CO i^ CO m CM CMc £• CM CM CM CM CM CN CN CM CM CM CN CNo«D T3 MO 8 O O O O O O O O o 00 00.£ <c » CM CM CM CM CN CN CN CM CM *— «
a A A A A A A A A A A A A
>l*» r^.
CM CM 00 00§ c X »* ^- * * CO CO 00 00 ^ *— <P- T—
o- 29
o 1
CM1
CM1
CM1
CM1
CO1
CO1 1 1 1 1 1
CN CM o oZ O
16 September 1977T Milliard V
Isolators and circulators
COAXIAL
CIRCULATORS/ISOLATORS
OCTAVE BANDWIDTH
r—
tf>n
1
i
!
i
1
i F I
|
cf+1
m1
I
*
f
X
EE^IO
j
1'4 -r^- r
'
—
i
o°+1
o(M
4.l
1 i
1
1
oE
E5 t
" -4!»- i -±»
i i
! 1
r^
--
"ir,
*
*
— S3—
J
^1 *1«
u>g
rI i
^ 1 p-
c
I u
> j
c
|CO
t_"f-
1
i
1
i
4--
1
i
Xo
\ E
' ?
t i
1
!
H 1 i
i—Sp-I
ct ^ J
V Milliard rSeptember 1977 17
COAXIAL
CIRCULATORS/ISOLATORS,
OCTAVE BANDWDTH
e
in E
I/) X
-E3H
•-e-
H 3
= t
30 *"
,.
a"
S OE
—£
"pi
—i—»•
J.
B.T
i
*~i~*-1 i
o"+l
i i
,o> w
I
"*fvl
* *f
1-T+- rh~\
> !— }- *|
4} i- ' J
1,-^
-e-
"
HS
3>-
^r
o
&
QT
d-e
18 September 1977Y Mullard
"b t
J- °S
Lt-L, —:—
i
4-j-
.q
J
u
Isolators and circulators
COAXIAL
CIRCULATORS/ISOLATORS
OCTAVE BANDWDTH
*
3i-~e-r-ffiZ
EHLP A
cf-
i_t s
:«- S|—
|
1"
Fl- n
i
1 1 Lo
J.
f3 » <n in
I I
0.
ft
*
o-- E
(O
i
B
-^
*--$—r~*£erzH
. «»c> -
J3
-t-
PJ o
J J
-3-- * X
•
tzdl ' IfczJ
U3 CIfM O
0"
aE
u MullardSeptember 1977 19
COAXIAL
CIRCULATORS/ISOLATORS
STANDARD BANDS
COQZ<CD
QCC<QZ
CO
COzoCOCCLU>
cc
2I
CO
COyjCC111
CO
CCo
oto"^CCo
3oCC
o
oo
CO *J- in CD o> s CO * COCI OJ OJ CM in *f *f CM
a>CO CO CM CO CO CMo o o o o o o O O
ifS c
CM CM CM CM CM CM CM CM CMCD
CM
to
CM CM
(0
CM
CO
CM
CO
CM
CO
CM
CO CO
CM CMCM CM CM CM CM CM CM CM CMr». r«. r- r» r*. f* r-. r» r»CM CM CM CM CM CM CM CM CM
Xin m in 8 o O o o o
en CM CM CM CO O «- COr*. r~ l»» ^t ^1- m
k.o a> CD 0) 0) CD CD
8 »
o ^u
CO CO CO CO CO CO
Ea>
E ECD
ECD
ECD
bCD < < <? 2 Sz z z z z z CO CO C/3
a> o o o o o o o o or>» (»» f-. CO CO r»- r-« r>. r-»
+ + + + + + + + +O o o o o o o O o o
|io •f
o o o o o o o o oCD
a>
e03
3a>
1 1 1 1 1 CM 1 ' *-
o^5 a
co o o o 8 o O o o in
E io
in in m o in *~ *~
in in in ^r o CO o O COQ. CM CM CM CN o *•* *- CM
^5 in in in in in CM cm in
CO CO CO CM CM CM «- CM
> co a>3 *- V V V V V V V V V
ga> CM CM CO CO
inCO CO CM
inCM CO
O O o o o d o o o
in in in in inE 0° CO CO CO in in CO CM cm rt
$u
ca 3> o o o o o o o o* o"_c 3 ** V V V V V V V V V
a _ in CM CO r^ l"» CM
co
CM CM CM CM CM CM CM CN CM
« so^ CO "O
CO $CO 00 00 O o O in in o
in r— CM CM CM CM CM CM3 +J
D> A A A A A A A A Am
r-» CO o CM m ^-CM CO ^- CM en CM oc a, N O o © •* in »-
= cST 2
X inCM r» CO OS CO 00CM CM CO rv. O) < 00 >* o>
o o o o o ^" CO ^r r-
20 September 1977¥ Milliard C7
Isolators and circulators
COAXIAL
CIRCULATORS/ISOLATORS,
STANDARD BANDS
m I_
It
E «o
x «~i•O 00E •»
<2> ^e n
l-v
1 flj. t-
. J E M
o o oCM(0
&
,,JGE5
3^I I
1-4/
*1hn.
f«
U Mullard ySeptember 1977 21
COAXIAL
CIRCULATORS/ISOLATORS,
STANDARD BANDS
55
HE-EL %
Lj juU iJ
tt
«n »- »-
i
22 September 1977¥ Mullard U
Isolators and circulators COAXIAL CIRCULATORSSTANDARD BANDS
U
co ^ro o03 s s-1 CM CM
(O (0
£ => CM CMo t- CM CM
CM CM
4_
o+->
U 01<B Q.
o< <2 5
o en en
g> o o3 r» (^
+ +O o oo *" +->
o o1 1
x ""? a>
£ 5 Se o e 3 o o
-r- Q-
Q. V- «—>-
5<o "2
CM CM
CO tt)
3 **
V VCM
1 1 "* ^-
15 « 8* o oCO '5. «- CO
1 1 CM CMC/l(A
c
? S* o oCM f in in
o" o*
Va>
3 S' V Vc CO in in•— *-" CO CM CM
3 1
?1
CM o oV V
TCO
1 CM CMCOoa
€* ? in in
m > T CMTJ
**i 1 r» r*»
CO CM CMco
a <3
(D T3CM O O
o(CA
Q)0)
C§- ?
in in
A A
(0 ^r CM in m3 CM CM
<3 « A A>i &3 c
NCMtj-* in
X 1 1
o- S CJ CO M-co ^-
*-
<*> O"
o> cf
-
ro +|
allB. R
H FW
5 .1o a
Milliard YSeptember 1977 23
WAVEGUDECRCULATORS
QSLU>CCo
I
CO
CO
ccLUCO
DC
§
goLU
Q<3LU><
- I% §
E S
Q. «E
*"
* 1 ^
2 O
CO CO © 8 8 O) 00 r>»
CM CM CM CMCM CM CM CM CM CM CM CMO o o o o O o oCO CO CO CO CO CO CO CO
CMCMCMCMCMCMCMCM
o o § in toio in a> a en
If) tO If]
CM CM CMCO CO 00
OOOOO^-^-M-^^r^rvf^ooooooccorcctrccccGca:i|| in 1 1 1 in in in in Til
OOOOOOOOioif>r-r>r^^'»^-+ + + + + + + +OOOOOOOOOOOOOOOO
T T T + + +
OOOOOOOOmiooooiomif)
ssssssss
e e q, q. © ^ »-_ ©„
vvvvvvvv
OOOOOOOOTfCMCM«-CMinif)C)o* o* o* o* ©* o" o~ o*vvvvvvvv
AAAAAAAAIf) If) oCM CM lO
CO <N * «- N Ifl IO **co* it co* r-* I
s* oo* oo* oo*
I I I I I I I I
in in if)
CM CM CM* eo 9 < »-_ i--, r* en
co* co* in* co* r»* r** r>»* r»*
S
o cZ O
24 September 1977
Milliard U
Isolators and circulators WAVEGUDECIRCULATORS
"* £o **
-H
!
' ) :
cfH ——4
<;;
1
--, \ \ !
\ ))'
1
0>O 1
•^— ooo —^i<*> +1
en r» co»- en CM
a a aooo
^00lO +
4^4
4
4
4 *
o o
"'1 I
1
1
1
J
1
1
1
Iy N./ v.
/ \
/ \^* vy \s \s \
"''. %
^ 1
a
?,-* ,
4-t
- -&• X
2~f .
r1-—
'
—
S
aE
-$- i ir-r1
ifo -III m
--$--1
co toCM CMCM CMO O
CO 2
if5 1O Q
JOTn
&&
®*t &
1 1
Lr-rl ECO
o &V
o Muliard rSeptember 1977 25
WAVEGUIDECIRCULATORS
J\^
COzoCOccLU>I-DC
i
sCOLU
ccLUCO
DC
O
IDODC
OLU
QOLU><
00o o COo o 8 '3-
o 8 inoCO CO CO CO CO CO CO CO
i_ o o O o o o o oo> 0)
_oE
CD CO CO CO CO CO CO CO
+-» 3C CM CM CM CM CM CM CM CM
o CM CM CM CM CM CM CM CMr^ r^ r- 1^ r*. r^ 1^ r^CM CM CM CM CM CM CM CM
X<A o o o O O o O O OE
^ o» CM CM CM CM CM CM o> CM
CO
05 O) 03 05 a> 05 CO CO
_ o O OO O o o O o O o f ^CD UJ 1^ r^ f^ r^ f»» 1^O) ^ DC oc DC DC DC DC DC DC DC
UJ UJ Ul Ul Ul Ul Ul nu mO.> D D Z3 3 Z) _3 1) 13 Z>
CU o o O o o o o o2 CO CO CO CO CO CO CO CO
+ + + + + + + +2 ? o o o o o o o o o
£ o •*-» •*-»
Fo o o o o o o o
0} + + + + + + + +
5COc
*5 o o o o o o in infc in m o o o o CM CMoc o
Q.
•^- CO o 00 o o o o|
o o o
,_5" V V V V V V V V
</5 in CD o 00 o o o o> co
1
o O o *"» *~^
5" V V V V V V V V
^ o o in in in in in ina CO CO CM CO CM CM2(AV)o
>» o «- o o o o o oTJ— a>
o cCO o" o*
"3-
o"CO CO
o"CO
d)
cCO3 V V V V V V V V
m ^- o o o 00 00 o 00 oD 1 CM CM CN *— *— CM *~
Co
« A A A A A A A ACO CO o m in in o o in
"o1 CO CO CM CM CM CO CO CN
« A A A A A A A Ain in in in m inr- CM r*. CM CM CM r-- in
> ** 00 *-,;
^f r*. T- COo co CO CO r~- r^ r^c
1 1 I I 1 | 1
3 TO NC I in in in in in in
CM CM r«- CM CM CM r^ inE O O) m 00 «—
,
rj- O CM*" in CO CO CO r^ !>. ""
26 September 1977
Milliard <n
Isolators and circulators A WAVEGUIDE
CIRCULATORS
r
1
1
: i
|
1
4-- -
1
1
1
1
i
r1
i
i
00 »-,no »-
o o
a. ceid m
D+'
=> Z)
v <uO) Olc co O>i- »•-
o o -
UJ UJl-H 1—1
o o
< CD
*
I
1
•« 3 s
XCO -« iu-^u
2 -mt-
-4 »-"$-
-3+ "To
issss00 CO CO 00 COo o o o o
in+l
1
1
1
-J 1
1
1
l__
-f-
"~l1
11
r -
1
i
1
—*
4- >
> 4-
O) f
u MullardSeptember 1977 27
INDUSTRIAL HEATING
ISOLATORS
COCCO
o
oz
mi
CC
Qz
«> 1_
2. •S'-o5 ETO -I
co cu
CMOCOCO
CM(Nr^CM
CMoCMOCOCO
CMCM1^.
CM
massapprox
kg
h.f. monitoring terminal
<o
ECD4-
z
a>
CO
Ea>
z
flange
type(IEC) •
coCMCCOOl
COCMCCaa.
cooling
water
temp.
(°C)
(water
pressure
600
kPa
abs)
4-<
_0>
<-•
3O
Oin
oin
O o
max.
c.w.
power
forward/reverse W
8inco
8mCO
5>'
Q.>4-* - -
CO TJ!= «co a>3 *•
CM
V
CM^
Vto
o CO
CD<nc
> CMco-
CM
o"
CO TJ
CO <u3 *>
co
o"
V
CO
OV
coK on
«o
Q.CDCM
COCM
CO "Oio 3>3 *^
oCM
AoCM
A
H-
C
PM
C3
IX)
CN1
inCM
CM
8CM*
1oinCOcm" 2 i
28 September 1977^r
Mullard V
Isolators and circulators INDUSTRIAL HEATING
ISOLATORS
© ©CM NO ©
m\ ^^
n£&
V MilliardSeptember 1977 29
WAVEGUDEISOLATORS
COyjCCLUCO
CCOh-
5o<n
LU
QC3
i
r^ 00 O) o o> in CO O) ** in CO CN CO r~ r» ooo o o *- r~ CM CM CM CM «- CM CN CM CNV o o o o o o O o o o o O O o o o o-1(0 t
CO CO CO CO CO CO CO CO CO CO CO CO CO CO CO CO CO
£ 3 <N CM CM CN CN CM CM CN CN CN CN CM CN CN CN CN CNCN CM CM CN CN CM CN CM CN CN CM CM CN CM CM CM CMf^ P^ l»N P- r>» r«» r» ("« r- r>. r-. r- fx r»- r~ r» r^CM CM CM CM CN CM CM CN CM CM CM CM CN CM CM CM CM
Xv> O O o O O O o o O o o o o O O o o oO in CO CO in in in in in in CO CM o O o CO CM(0 Q. O) r>- ** CO CO Tf * <a- *t *r * CM «t * CO CO ^- CMc
CDCM
* **
o oo 88, Sic ^ *
00 o 00 00 o o o o o o *r 8 ooCCUJ
CC00 8 8
5= CL '3- ^i- ^ Tf r- i-» r> r-» r» t-» 00 -> ->> CC CC CC CC CC CC CC CC CC CC CC CC CC 4m 4
in
CC CC*-'
UJ m UJ UJ UJ UJ UJ UJ Ul UJ 00 00 00 00 003 3 3 3 3 3 3 3 3 3 3 3 3 3 3
go O s o o o o3 — CO o 00 CO O O O o O o <tf o o o O 'S-O) — ^I * ^- * r-» t^ r» 1^ r->. p". 00gj a)£ Q.
CC CC CC or CC CC CC CC CC CC CC CC CC CC CC CC CC
5 >
o o o o o o o O o o o o o o o o o3
* 00 ^> ^- r~ r» i^ px r~ r* r* r*. r-» r»«
+ + + + + + + + + + + + + + + + +? ?o o o o o o o o o o o o o O o o o oQ. <D °E
*"
*-* +• «-» «-« H +J "> •(->
o o o o o o o o o o o o o o o o oto + + + + 1 1 1 1 1 1 + 1 + 1 1 + +
ower
c.w.) w o o o o o o o o o o o o ,_ o o in oCM CM CM CN CN
Q.
—
u.in in in in in in in in m m in m in in in m
5 O o o o o o o o o o o o CN o o
> V V V V V V V V V V V V V V V V V
ertion
OSS dBCO in in 00 CO CO CO CO CO in in in CO CN oo mo o o o o o o o o o o o o ^ ^- o o
c V V V V V V V V V V V V V V V V V
ation B o o o o o o o o o o o o in m o 2 oCO CO CO CO CO CO CO CO CO CO CO CO «— in CM CO CO
o u.S2
A A A A A A A A A A A A A A A A A
in o in o o inCM in CM in in CM r»« in
> CN CM CO o ** *-,. •«f r^ r> o in CO CO CO CO «- COu ^r < ^- in CO r^ r» i^- r>. 00 00 o> en O) o>C cuI 1 | 1 1 1 1
1 |
equerang
GHzin in in in OCM CM CM CM in
00 00 CM CO en * 00 CM ^r i-» in in m in r^ in* CO CO * ^> in CO CO r» i~~ r~ r*. CO CO CO 00 O CM
It
•s °
O u.
30 September 1977 r Milliard &
Isolators and circulators WAVEGUDEISOLATORS
o1 I
0> CM
P O ^— +1 <•>"
Q o ^
1 1 1
T1—
1
i!| ~
>«-l
+1in
-+I
II
.»
C '1 '
*~
in
o
WAVEGUDEISOLATORS
T
B8T>'O
CN
d
c
__ *
-1 <
-
iE3o""l
32 September 1977Y Milliard U
Isolators and circulators
y"V.
WAVEGUDEISOLATORS
LT ILL
mTJ
|yvv»M^>N
o o
o o
- -J 1
pyyyi 'V^
<"4 E
U
NNNi-" »— r-O O OsI-CMCM
1 1.
1
1oE
ir>"
1
&
^1 1
^h i
14*- EinCO
<
"* CM*
Xo »
Mullard YSeptember 1977 33
GENERAL
CONVERSION LISTS
Catalogue Number Type
2722 161 ,.
.
Number
01071 CL6201
01081 CL6240
01091 CL6202
01101 CL6203
01151 CL6210
01161 CL6214
01171 CL6215
01181 CL6217
01191 CL6206
01211 CL6222
01221 CL6221
01231 CL6231
01241 CL6241
01251 CL6251
01261 CL6261
01271 CL6271
01291 CL6291
02081 CL5281
02091 CL5291
02101 CL5101
02191 CL5219
02231 CL5232
02261 CL5263
02271 CL5227
02281 CL5283
03001 CL5050
03011 CL5051
03031 CL5053
03041 CL5054
03051 CL5055
03061 CL5056
03081 CL5081
03091 CL5091
Catalogue Number Type
2722 162 Number
01121 CL5027
01131 CL5028
01141 CL5029
01261 CL5261
01271 CL5271
01281 CL5282
01331 CL5331
01491 CL5491
01501 CL5501
01511 CL551
1
01551 CL5551
01561 CL5561
01572 CL5372
01582 CL5382
01592 CL5392
01612 CL5312
01622 CL5322
01632 CL5332
01642 CL5342
01662 CL5362
01811 CL5811
01821 CL5821
01851 CL5851
01861 CL5861
01871 CL5871
01881 CL5881
01891 CL5891
01901 CL5901
01931 CL5931
01941 CL5941
01951 CL5951
02041 CL6041
02071 CL6071
34 September 1977
Milliard T)
GENERAL
Catalogue Number Type
2722 162 Number
02091 CL6091
02101 CL6101
02111 CL6111
02121 CL6122
02221 CL6223
02231 CL6232
03171 CL51 72
03181 CL5182
03261 CL5262
03301 CL5301
03411 CL5411
03431 CL5431
03441 CL5441
03591 CL5592
04031 CL5032
04041 CL5042
Catalogue Number
2722 163 . .
Type
Number
02004
02024
CL6204
CL6224
V MilliardSeptember 1977 35
GENERAL
Type Catalogue
Number Number
CL5027 2722 162 01121
CL5028 2722 162 01131
CL5029 2722 162 01141
CL5032 2722 162 04031
CL5042 2722 162 04041
CL5050 2722 161 03001
CL5051 2722 161 03011
CL5053 2722 161 03031
CL5054 2722 161 03041
CL5055 2722 161 03051
CL5056 2722 161 03061
CL5081 2722 161 03081
CL5091 2722 161 03091
CL5101 2722 161 02101
CL5172 2722 162 03171
CL5182 2722 162 03181
CL5219 2722 161 02191
CL5227 2722 161 02271
CL5232 2722 161 02231
CL5261 2722 162 01261
CL5262 2722 162 03261
CL5263 2722 161 02261
CL5271 2722 162 01271
CL5281 2722 161 02081
CL5282 2722 162 01281
CL5283 2722 161 02281
CL5291 2722 161 02091
CL5301 2722 162 03301
CL5312 2722 162 01612
CL5322 2722 162 01622
CL5331 2722 162 01331
CL5332 2722 162 01632
CL5342 2722 162 01642
Type Catalogue
Number Number
CL5362 2722 162 01662
CL5372 2722 162 01572
CL5382 2722 162 01582
CL5392 2722 162 01592
CL5411 2722 162 03411
CL5431 2722 162 03431
CL5441 2722 162 03441
CL5491 2722 162 01491
CL5501 2722 162 01501
CL551^1 2722 162 01511
CL5551 2722 162 01551
CL5561 2722 162 01561
CL5592 2722 162 03591
CL5811 2722 162 01811
CL5821 2722 162 01821
CL5851 2722 162 01851
CL5861 2722 162 01861
CL5871 2722 162 01871
CL5881 2722 162 01881
CL5891 2722 162 01891
CL5901 2722 162 01901
CL5931 2722 162 01931
CL5941 2722 162 01941
CL5951 2722 162 01951
CL6041 2722 162 02041
CL6071 2722 162 02071
CL6091 2722 162 02091
CL6101 2722 162 02101
CL6111 2722 162 02111
CL6122 2722 162 02121
CL6201 2722 161 01071
CL6202 2722 161 01091
CL6203 2722 16101101
36 September 1977Mullard n
GENERAL
Type Catalogue
Number Number
CL6204 2722 163 02004
CL6206 2722 161 01191
CL6210 2722 161 01151
CL6214 2722 161 01161
CL6215 2722 161 01171
CL6217 2722 161 01181
CL6221 2722 161 01221
CL6222 2722 161 01211
CL6223 2722 162 02221
CL6224 2722 163 02024
CL6231 2722 161 01231
CL6232 2722 162 02231
CL6240 2722 161 01081
CL6241 2722 161 01241
CL6251 2722 161 01251
CL6261 2722 161 01261
CL6271 2722 161 01271
CL6291 2722 161 01291
V MilliardSeptember 1977 37
INDEX
INDEX TO BOOK 1 , PART 8
Type number Section Type number Section
ACX-01
A
H BAW95D CAEY17 D BAW95E CAEY29 D BAW95F CAEY29R D BAW95G CAEY31 D BAY96 E
AEY31A D BXY27 E
AEY32 D BXY28 E
BAT10 C BXY29 E
BAT 11 C BXY32 E
BAT31 B BXY35 E
BAT38 C BXY36 E
BAT39 C BXY37 E
BAT39A C BXY38 E
BAT50 C BXY39 E
BAT50R C BXY40 E
BAT51 C BXY41 E
BAT51
R
C BXY50 B
BAT52 C BXY51 B
BAT52R C BXY52 B
BAT59 C BXY53 E
BAV22 C BXY54 E
BAV22R C BXY55 E
BAV46 C BXY56 E
BAV72 C BXY57 E
BAV75 C BXY60 B
BAV96A C CAY 10 E
BAV96B C CL7500 HBAV96A C CL7520 H
BAV96D C CL8310 F
BAV97 C CL8630 F
Type Ntfmber Section Type number Section
CL8630S F CXY23B E
CL8631 F CXY23C E
CL8631S F CXY23D E
CL8632 F CXY24A B
CL8632S F CXY24B B
CL8633 F SIM2 see BAV22, R
CL8633S F SIM5 see BAV22, R
CL8640R F 1N23D see BAW95DCL8640T F 1N23DR see BAW95DCL8690 F 1N23E see BAW95E
CL8880BN G 1N23ER see BAW95ECL8880BNC G 1N23F see BAW95FCL8960 G 1N23G see BAW95GCL8961 G 1N23GR see BAW95GCL8962 G 1N23WE see BAW95E
CL8963 G 1N78D see BAT52CL8964 G 1N78DR see BAT52RCL8965 G 1N78E see BAT51CL8967 G 1N78ER see BAT51
R
CL9022 \
CXY10
H 1N415D see BAW95D
E 1N415E see BAW95ECXY11A B 1N415F see BAW95FCXY11B B 1N415G see BAW95GCXY11C B 1N5152 ECXY12 E 1N5153 E
CXY14A B 1N5155 ECXY14B B 1N5157 ECXY14C B
'
CXY19 B
CXY19A B
CXY19B BCXY21 B
CXY22A E
CXY22B E
CXY23A E
MICROWAVE SEMICONDUCTORSAND COMPONENTS
CONTENTS
4 SELECTION GUIDE (see coloured pages)
EA GENERAL SECTION
\ B GUNN, IMPATT AND NOISE DIODES
E C M IXER AND DETECTOR DIODES
E D BACKWARD DIODES
! EVARACTOR DIODES (Multiplier, specialpurpose and tuning types)
jF GUNN OSCILLATORS
!G DOPPLER AND TRAFFIC RADARS
j H MISCELLANEOUS
jJ ISOLATORS AND CIRCULATORS
4 INDEX
Mullard Limited
Mullard House, Torrington Place, London, WC1E 7HD
3 0)73 <O 4)
2 »CD (D
ST Io
55a
c
CD
t£
CD
Printed in England
TP 1818 (3