Notes 19 ECE 5317-6351 Microwave Engineering Fall 2011 Power Dividers and Couplers Part 1 Prof....
-
Upload
elliott-brinson -
Category
Documents
-
view
313 -
download
12
Transcript of Notes 19 ECE 5317-6351 Microwave Engineering Fall 2011 Power Dividers and Couplers Part 1 Prof....
1
Notes 19
ECE 5317-6351 Microwave Engineering
Fall 2011
Power Dividers and Couplers Part 1
Prof. David R. JacksonDept. of ECE
2
Power Dividers and Directional Couplers
Divider1P 2 1P P
3 11P P
1 2 3P P P 2P
3P
Coupler(Combiner)
Three-port networks
11 12 13
21 22 23
31 32 33
S S S
S S S S
S S S
General 3-port:
3
For all ports matched, reciprocal, and lossless:
12 13
12 23
13 23
0
0
0
S S
S S S
S S
13 23
12 23
12 13
0
0
0
S S
S S
S S
2 2
12 13
2 2
12 23
2 2
13 23
1
1
1
S S
S S
S S
Lossless [S] is unitary
Not physically possible
These cannot all be satisfied.
At least 2 of S13, S12, S23 must be zero.
Power Dividers and Directional Couplers (cont.)
(There are three distinct values.)
(If only one is zero (or none is zero), we cannot satisfy all three.)
(If only one is nonzero, we cannot satisfy all three.)
4
Now consider a 3-port network that is non-reciprocal, all ports matched, and lossless:
12 13
21 23
31 32
0
0
0
S S
S S S
S S
31 32
21 23
12 13
0
0
0
S S
S S
S S
2 2
21 31
2 2
12 32
2 2
13 23
1
1
1
S S
S S
S S
Lossless
These equations will be satisfied if:
“Circulator”
12 23 31
21 32 13
0
1
S S S
S S S
21 32 13
12 23 31
0
1
S S S
S S S
Power Dividers and Directional Couplers (cont.)
(There are six distinct values.)
or
1
2Note that Sij Sji.
5
21S
32S
13S
1
2
3
12S
23S
31S
2
1
3
0 0 1
1 0 0
0 1 0
S
Clockwise (LH) circulator
Circulators
Counter clockwise (RH) circulator
1
2
Circulators can be made using biased ferrite materials.
Note: We have assumed here that the phases of all the S parameters are zero.
0 1 0
0 0 1
1 0 0
S
6
Power DividersT-Junction: lossless divider
1inY
02Z
03Z3inY
01Z
1
23
1
3
02 03 02 03 02 03
01 02 02
02 03
02 0301 02 03
01 02 03
03 02 02 03 03 02
0 03 2
2 21 1
1 1
1|
1
1
|
1
1
in
in
i
n
in
n
i
Z Z Z Z Z ZY
Z Z Z Z Z Z Z Z Z
YZ
YZ Z
Z ZY Z Z Z
Z Z Z
YZ
Note,however,
Th
To mat
us ls, A o,
ch
If we match at port 1, we cannot match at the other ports!
7
02Z
03Z
01Z 1V
1
2
3
2 1
3
1
1
11
1 1
01 03
02 02 0
2
1
02
2
3
01 021
03 0
2
1
30 0
1
3 2
0
1
2
1
2
1
2
1
in iout in
i
in
ni nt
n
n iou
VP
Z
V
Z ZP P
Z Z Z
Z ZP P
ZP
ZK
K
P
P
ZP
V
Z
Z
02 0301
02 03
Z ZZ
Z Z
Assuming port 1 matched:
Power Dividers (cont.)
We can design the splitter to control the powers into the two output lines.
8
02Z
03Z
01Z 2V1V+
-
+
-
2 3
1 3 1 2
02 03 01
02 03 01
01 03 02 01 02 03
111
1 0
2 322 33
2
01 03 02 01 02 03
30 0
a a
a a a a
Z Z Z
Z Z Z
Z Z Z Z Z Z
Z
VS
V
V VS
Z Z
V
Z
SV
Z Z
zero if port 1 is matched
For each port we have:
Power Dividers (cont.)
9
2 3
0121 11 12
02
01 0231 13 11 32 23 22
0
1 1 11 2 2 1 2
2
0221
1
01 0
1 11
0
1 1
3 3
1 ; /
1
1 1
/ 1
a a
V V S V V V V V V V
ZS S S
Z
Z ZS S S S S S
Z Z
Z
V
S
V
S
Z
Similarly,
and
Power Dividers (cont.)
02Z
03Z
01Z 2V1V+
-
+
-
Also, we have
10
01 03 02 01 02 0311 22 33
01 03 02 01 02 03
01 0121 12 11
02 02
01 0113 31
03
02 03
0211
03 03 02 03
0222
03
0232 23 22
03
0
1
; ;
1
1
1
Z
Z Z
Z
Z Z
ZS
Z Z Z Z Z ZS S S
Z Z Z Z Z Z
Z ZS S S
Z Z
Z ZS S S
Z Z
ZS S S
Z Z
21 31
21 22 32
31 32 33
0 S S
S S S S
S S S
If port 1 is matched:
The output ports are not isolated.
Power Dividers (cont.)02 03
0102 03
Z ZZ
Z Z
11
03
02 03
02
0
222
2 03
11
2331
1
PS
P
P
Z
Z Z
Z
Z ZS
P
Powers:
Power Dividers (cont.)
1 203 02
1 1 102 0 0
33 2 03
Z ZP P P
ZP P P
Z Z Z
Check :
3 02
2 03
P Z
P ZHence
12
Summary
Power Dividers (cont.)
3 02
2 03
P Z
P Z
01 03 02 01 02 0311 22 33
01 03 02 01 02 03
0321 12
02 03
0213 31
02 03
0232 23 22
03
0 ; ;
1
Z Z Z Z Z ZS S S
Z Z Z Z Z Z
ZS S
Z Z
ZS S
Z Z
ZS S S
Z
02Z
03Z
01Z1
2
3
02 0301
02 03
Z ZZ
Z Z
The input port is matched, but not the output ports.
The output ports are not isolated.
13
Example: Microstrip T-junction power divider
Power Dividers (cont.)
01 50 [ ]Z
02 100 [ ]Z
03 100 [ ]Z
11
22 33
21 12
31 13
32 23
0
1
2
1
2
1
2
1
2
S
S S
S S
S S
S S
01 02 01 03 50 100 33.333 [ ]Z Z Z Z
14
Resistive Power Divider
0Z
0Z
0Z
1V
2V
3V
0
3
Z0
3
Z
0
3
Z
1inZ
port1
port3
port2
0 0 01
0 00
4 4
3 3 3
2
3 3
in
Z Z ZZ
Z ZZ
11 22 33 0S S S
Same for Zin1 and Zin2
All ports are matched.
15
1 1 11 1
2
1 1
00
2 10 0
0 0
1
23
23 3
1
2
3
2 3
3 4
V
V
V
V V S
Z ZV V
Z Z
V
Z Z
2 3
2
021
1
0 0a a
V
ZS
V
Z
12 321 1 13 32 23
1
2S S S SS S
By reciprocity and symmetry
Resistive Power Divider (cont.)
0Z
0Z
0Z
1V
2V
3V
0
3
Z0
3
Z
0
3
Z
1inZ
port1
port3
port2
16
221
1 10
22 2 2
2 3 2 1 21 1 21 1
0 1 11
1 0 12
1 1
1 1
2 2
4
0
1 1 1
2 2 2
in
in
VP P a
Z
PP P b a S
S
P S P
All ports are matched, but 1/2 Pin is dissipated by resistors, and the output ports are not isolated.
0Z
0Z
0Z
1V
2V
3V
0
3
Z0
3
Z
0
3
Z
1inZ
port1
port3
port2
1P
2P
3P
Resistive Power Divider (cont.)
Hence we have
17
Even-Odd Mode Analysis1
2 1 3S
S
VV V
2 2
2 SV V
Plane of symmetry 2 2 2 2
2 eSV
oSV 0V
eV
POS POS
2 eSV
oSV
1
2e o
S S SV V V Let
e oV V V
Obviously,
Example: We want to solve for V.
using even/odd mode analysis
“odd” problem“even” problem
(This is needed for analyzing the Wilkenson.)
18
“Even” problem
2 2 2 2
2 eV
eV
2SV
2SV
4 4
0I
eSV
POS POS
eSV
Open circuit (OC) plane of symmetry
2
4 2SV eV
4
2 2 4 3e S SV V
V
Even-Odd Mode Analysis (cont.)
19
“Odd” problem
oSV
2 2 2 2
2 oSV 0oV
oV
2SV
2SV
4 4
POS POS
0oV
2
4 2SV
oV
short circuit (SC) plane of symmetry
Even-Odd Mode Analysis (cont.)
20
2 2
2 SV V
2 2 2 2
2 2SV oV
eV
2SV
2SV
2SV 2
03
3
Se
S
oVV
VV
V V
“even” problem “odd” problem
By superposition:
Even-Odd Mode Analysis (cont.)
21
0Z
0Z
0Z0
2Z
02Z
02Z
g/ 4
g / 4
3
2
1
0 1 1
1 0 02
1 0 0
jS
Wilkenson Power DividerEqual-split (3 dB) power divider
All ports matched (S11 = S22 = S33 = 0)
Output ports are isolated (S23 = S32 = 0)
Obviously not unitary
Note: No power is lost in going from port 1 to ports 2 and 3.
2 2
21 31
1
2S S
22
Example: Microstrip Wilkenson power divider
Wilkenson Power Divider (cont.)
01 50 [ ]Z 0 70.7 [ ]TZ
03 50 [ ]Z
02 50 [ ]Z
0 70.7 [ ]TZ
100 [ ]R
23
22 32,S S
11 21,S S
• Even and odd analysis is required to analyze structure when port 2 is excited.
• Only even analysis is needed to analyze structure when port 1 is excited.
To determine
To determine
Wilkenson Power Divider (cont.)
The other components can be found by using symmetry and reciprocity.
24
Top view
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
1V
1V 2V
2V
3V
3V
Plane of symmetry
Split structure along plane of symmetry (POS)
Even voltage even about POS place OC along POS Odd voltage odd about POS place SC along POS
Wilkenson Power Divider (cont.)
A microstrip realization is shown.
25
0 022
h VZ Z
I
0Z/ 2I
POS
/ 2I
Z0 microstrip line
How do you split a transmission line? (This is needed for the even case.)
top view
Voltage is the same for each half of line (V)Current is halved for each half of line (I/2)
For each half
Wilkenson Power Divider (cont.)
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
1V
1V 2V
2V
3V
3V
Plane of symmetry
(magnetic wall)
26
“Even” Problem
Wilkenson Power Divider (cont.)
02Z
0Z
0Z
0
2 Z
02Z
OC
/ 4g
/ 4g
V
eV
V
eV
02Z
1eV
1eV
3eV
0Z
0Z
OC
2eV
Ports 2 and 3 are excited in phase.
Note: The 2Z0 resistor has been split into two Z0 resistors in series.
3 2e eV VNote :
271 3 20,o o oV V V Note :
Wilkenson Power Divider (cont.)
“Odd” problem
02Z
0Z
0Z
0
0
g
g
V
oV
V
oV
02Z
1oV
1oV
3oV
0Z
0Z
2oV
Ports 2 and 3 are excited 180o out of phase.
Note: The 2Z0 resistor has been split into two Z0 resistors in series.
28
02Z
0Z
0
OC
gV
eV
2eV
1eV
2 22,e einZ S
33
2
0
2 00
2 022
2 0
2
2
0
0
ein
ee in
ein
e
ZZ Z
Z
Z ZS
S
Z Z
Also, by symmetry,
Wilkenson Power Divider (cont.)
Even ProblemPort 2 excitation
Port 2
29
02Z
0Z
02Z
/ 4g V
oV
0Z
2oV
1oV
2 22,o oinZ S
short
2 0 0
2 022
2 0
33 0
0
oin
oo in
oin
o
Z Z Z
S
Z ZS
Z Z
Also, by symmetry,
1 0oV
Wilkenson Power Divider (cont.)
Port 2
Odd Problem
Port 2 excitation
30
1 3
1 3
222
2 0
33
332
22 22
2 0
2
22
32 22 22
3
1 10 0 0
2 2 2
1 10 0 0
2 2 2
0
0
e o e oe o
a a
a
e o e oo
a
e
V V V VS S S
V V V
V V V VS S S
V V V
VS
V
S
VS
V
S
(by symmetry)
(by reciprocity)
Wilkenson Power Divider (cont.)
22
33
32 23
0
0
0
S
S
S S
In summary,
We add the results from the even and odd cases together:
Note: Since all ports have the same Z0, we ignore the normalizing factor Z0 in the S parameter definition.
31
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
1V
1V 2V
3V
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
1V
1V
02 Z
0Z0
2Z
OC
/ 4g
1V
1V
O.C. symmetry
plane
When port 1 is excited, the response, by symmetry, is even. (Hence, the total fields are the same as the even fields.)
Even Problem
Wilkenson Power Divider (cont.)
Port 1
Port 1 excitation
32
02Z
0Z0
2Z
OC
/ 4g
1eV
1eV
1
2
1 11,e einZ S
2 3 2
1 011
1 0
1 111 11
2
0
0 0
1
1
0
1
0
20
2
0
22
ee in
ei
ein
n
ee
e
a a a
Z
Z ZS
Z Z
V VS S
V V
Z ZZ
Wilkenson Power Divider (cont.)
11 0S
Hence
Even Problem
Port 1 excitation
33
02Z
0Z0
2Z
OC
/ 4g
1V
1V 2V
z
1 1 11 1
2 2 2
1V V S V
V V V
2 3
221
1 0a a
VS
V
(reciprocal)
2 221
1 1
1 2
1 2 2
V VS j j
V V
Wilkenson Power Divider (cont.)
21 122
jS S
20
2 0
1 0
1
0 1
/ 4 1
j z j z
g
V z V e e
V V V
V V
z
V j
distance from port 2
0 0
0 0
2 1 2
2 1 2
Z Z
Z Z
Along g/4 wave transformer:
Even Problem
Port 1 excitation
34
31 21 2jS S By symmetry:
Wilkenson Power Divider (cont.)
13 31 2jS S By reciprocity:
For the other components:
35
0 1 1
1 0 02
1 0 0
jS
Wilkenson Power Divider (cont.)
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
All three ports are matched, and the output ports are isolated.
11 22 33 0S S S
32 23 0S S
36
0 1 1
1 0 02
1 0 0
jS
Wilkenson Power Divider (cont.)
When a wave is incident from port 1, half of the total incident power gets transmitted to each output port (no loss of power).
When a wave is incident from port 2 or port 3, half of the power gets transmitted to port 1 and half gets absorbed by the resistor, but nothing gets through to the other output port.
21 312
jS S
12 132
jS S
0Z
0Z
0Z
0
2 Z
02 Z
02Z
/ 4g
/ 4g
37
Wilkenson Power Divider (cont.)
Figure 7.15 of PozarPhotograph of a four-way corporate power divider network using three
microstrip Wilkinson power dividers. Note the isolation chip resistors.
Courtesy of M.D. Abouzahra, MIT Lincoln Laboratory.