Transmission line
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Transcript of Transmission line
EMLAB
1
Transmission line
EMLAB
2
An apparatus to convey energy or signal from one place to another place.
• Transmitter to an antenna
• connections between computers in a network
• hydroelectric generating plant and a substation several miles away
• interconnect between components of a stereo system
• CATV service provider and your TV set
• Connections between devices on a circuit board
Transmission line
EMLAB
3Example – Cable TV
EMLAB
4Example – Computer network
EMLAB
5Example – Electric power transmission line
EMLAB
6Example – Printed circuit board
EMLAB
7Example – Printed circuit board
EMLAB
8Types of transmission lines
Microstrip line
Coaxial cable
Two-wire transmission line
EMLAB
9Distribution of electric field strengths of typical TEM lines
E/H distributions vary as the structures of transmission lines change. For electromagnetic compatibility, E/H should be confined to small area.
MicrostripTwo-wireParallel plate
EMLAB
10Field representation in waveguides
EMLAB
11
Wave Solution
0 zz HE
0ˆ
0ˆ
ttztt
ttztt
Ej
Hj
HzH
EzE
)ˆ
ˆ
ztttzztztt
ztztzztt
Hjω
Hjω
zHEEE
)z(H )E(E)E(E
(
)Eqs.Maxwell(, JEHHE jj
ttttz
ttttz
jωzz
jω
jωzz
jω
E HE H
H EH E
)ˆ(
)ˆ(
0,0 22
22
2
2
tt
tt k
zk
zH
HE
E0
0,0
0
2
tt
ttt
ztt z
E
H
E
EE
)(zftt E
)(00jkzjkz
tjkzjkz
t eVeVee EEE
TEM mode (Transverse electromagnetic mode)
EMLAB
12
z
y
xParallel plate waveguide
02
2
2
2
2
22
xyxt
With a wide enough line trace, varia-tion along y-axis can be ignored.
xd
VCxC s 21
)(ˆ)(ˆ jkzjkzjkzjkzsTEM eVeVeCeC
d
V xxE
d
)(1
ˆ)(ˆ1 jkzjkzjkzjkzx
TEM eVeVeVeVk
z
H
jj
yyE
H
EMLAB
13
i (z, t)
v (z, t)+
-
z
L zC z
i (z+z, t)
v (z+ z,t)+
-
i (z, t)
z
v (z, t)+
-
Transmission line 등가 회로
tC
z
it
iL
z
),(
),(),( tzz
t
tzizLtz
),(),(
),( tzzit
tzzzCtzi
EMLAB
14Transmission line eq. solution
tC
z
i
t
iL
z
, 0,02
2
2
2
2
2
2
2
t
iLC
z
i
tLC
z
)()(),(
)()(),(
tuzItuzItzi
tuzVtuzVtz
C
LZ0)()(),()( 00 tIZtVtIZtV
LCu
1
IC
LVI
C
LV ,
)(z
z
)( tuz
z
)( tuz
z
01
)(),(
,1
2
2
2
2
2
2
22
2
2
22
2
2
2
2
2
2
dX
Vd
dX
Vd
t
V
uz
V
dX
Vdu
t
X
t
V
Xt
Vu
dX
dV
t
X
dX
dV
t
V
dX
Vd
z
X
z
V
Xz
V
dX
dV
z
X
dX
dV
z
V
tuzX
EMLAB
15Transmission line 의 특징
H
E
Direction of propagation
H
1. For a magnetic field and an electric field propagating in the same direction, the ratio of E and H (E+/H+) is kept constant.
2. For a voltage and a current current propagating in the same di-rection, V+/I+ ratio is equal to Z0 .
3. When the ratio is disturbed, reflected waves are generated.
0ZI
V
I
V
0ZI
V
I
V)(tV
SZLZ
EMLAB
16
LZ+V-
SZI
V
I
V
VVVL
IIIL
LLL IZV
)tcoefficien reflection;(, VV
0Z
II
VV
L
L
)1(
)1(
0
0
01
1
1
1
ZZ
ZZ
ZZI
V
I
V
L
L
LL
L
Reflection coefficient
}Re{)1(2
1)1()1(Re
2
1}Re{
2
102
0
2
2
*0
*** Z
Z
V
Z
VVIVP LLL
EMLAB
17
LZ+V-
SZ
20 40 60 800 100
0
1
-1
2
time, nsecV
in, V
Vou
t, V
20 40 60 800 100
0
1
-1
2
time, nsec
Vin
, VV
out,
V
LZ+V-
SZ
LZ+V-
SZ
LZ+V-
SZ
LZ+V-
SZ
Zs = 20
Z0= 50
ZL= 1k
0.5m
Influence of line length on load voltage
rc
LT
/delay
[ns]250 T
[ns]6d T
[ns]3d T
[ns]5.1
[ns]375.0
[ns]75.0
Impedance mismatched
Vin VoutRR2R=1k Ohm
MLINRR1R=20 Ohm
VtPulseSRC1
t
Z0= 50
20 40 60 800 100
0
1
-1
2
time, nsec
Vin
, VV
out,
V
20 40 60 800 100
0
1
-1
2
time, nsec
Vin
, VV
out,
V
20 40 60 800 100
0
1
-1
2
time, nsec
Vin
, VV
out,
V
EMLAB
18
EMLAB
19Ringing : Time domain
EMLAB
20
1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.91.0 2.0
-1
0
1
2
-2
3
time, usec
Vin
, V
Vout, V
Vs Vin Vout
RR1R=10 Ohm
VtPulseSRC1
Period=50 nsecWidth=25 nsecFall=1 nsecRise=1 nsecEdge=cosineDelay=0 nsecVhigh=1 VVlow=0 V
t
RR2R=1000 Ohm
MLINTL1
L=5 meterW=0.242 mmSubst="MSub1"
Signal source
Load
~ 10SZ
1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.91.0 2.0
-0.0
0.2
0.4
0.6
0.8
-0.2
1.0
time, usec
Vin
, V
Vout, V
kZL 1500Z
Mismatched load
Ringing
EMLAB
21Impedance matching – Digital logic
~
10SZ
kZL 1500Z
R1
1k
0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50 0.55 0.60 0.65 0.70 0.75 0.80 0.85 0.90 0.950.00 1.00
0.0
0.5
-0.5
1.0
time, usec
Vin
, V
Vout, V
40
~ 10SZ
kZL 1
500Z 53
0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50 0.55 0.60 0.65 0.70 0.75 0.80 0.85 0.90 0.950.00 1.00
-0.0
0.2
0.4
0.6
0.8
-0.2
1.0
time, usec
Vin
, V
Vout, V
Source matching
Load matching
EMLAB
22Impedance matching topologies
EMLAB
23
0,02
2
2
2
2
2
2
2
t
iLC
z
i
tLC
z
Frequency domain solution
0,0 22
22
2
2
LCIz
ILCV
z
V
dezItzi
dezVtz
tj
tj
),(2
1),(
),(2
1),(
zjzj
zjzj
eIeIzI
eVeVzV
),(
),(
VCjz
IILj
z
V
,
)()(),()( IC
LVI
C
LV
LCLC p
p
1,
β : propagation constant, vp : speed of light
dezVLC
dz
zVd
tLC
ztj),(
),(
2
1 22
2
2
2
2
2
EMLAB
24
]}[Re{
}Re{
)()(),(
zjzjtj
zjtjzjtj
eVeVe
eeVeeV
tzVtzVtz
Phasor representation
zjzj eVeVzV ),(
LZ+V-
SZI
V
I
V
0Z
tjSS eVtlz ),(
}),(Re{),( tjezVtz lz 0z
)cos(}Re{),( ztVeeVtzV zjtj
)cos(}Re{),( ztVeeVtzV zjtj
EMLAB
25Transmission line terminated with short, open
Zs = Zo
VreflV inc
For reflection, a transmission line terminated in a short or open reflects all power back to source
In phase (0 ) for openo
Out of phase (180 ) for short
Vrefl
o
EMLAB
26Transmission Line Terminated with 25 Ω
Zs = Zo
ZL = 25 W
VreflV inc
Standing wave pattern does not go to zero as with short or open
3
1
5025
5025
EMLAB
27
)(][1
),(
)(),(
00
ljljljlj
ljljljlj
eeZ
VeVeV
ZlI
eeVeVeVlV
0
0
ZZ
ZZ
L
L
ljZZ
ljZZZ
ee
eeZ
lI
lVZ
L
Lljlj
ljlj
in
tan
tan
),(
),(
0
000
Equivalent input impedance
EMLAB
28Input impedance of short
ljZZ in tan0
EMLAB
29Input impedance of open
ljZZ in cot0
EMLAB
30Some transmission line examples
300
][513.2105.2
101002 18
6
m
rad][6.1288180)/(28.0 l
300tan
tan
0
000 ljZZ
ljZZZ
ee
eeZZ
L
Lljlj
ljlj
in
]W[5.1}1.030Re{2
1}Re{
2
1 6.16.1* eeVIPL
300
V][)6.1102cos(30}30Re{ 86.1102 8
teeV tL
A][)6.1102cos(1.0}1.0Re{ 86.1102 8
teeI tL
case 1) matched load
EMLAB
31
150
206466288tan150300
288tan3001500 j
j
jZZin
300
][150756.0206466300
60A
jI in
]W[333.1466)0756.0(2
1}Re{
2
1 22 inL ZIP
case 2) unmatched load
EMLAB
32Ringing : Time/frequency domain