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Prof. Ji Chen
Notes 6 Transmission Lines
(Time Domain)
ECE 3317
1
Spring 2014
Note:
Transmission lines is the subject of Chapter 6 in the Shen & Kong book. However, the subject of wave propagation in the time domain is not treated very thoroughly there. Chapter 10 of the Hayt book has a more thorough discussion.
Note about Notes 6
2
A transmission line is a two-conductor system that is used to transmit a signal from one point to another point.
Transmission Lines
Two common examples:
Coaxial cable Twin lead
r a
b
z
A transmission line is normally used in the balanced mode, meaning equal and opposite currents (and charges) on the two conductors.
3
Transmission Lines (cont.)
Coaxial cable
Here’s what they look like in real-life.
Twin lead
4
Transmission Lines (cont.)
5
CAT 5 cable(twisted pair)
Transmission Lines (cont.)
Some practical notes:
Coaxial cable is a perfectly shielded system (no interference).
Twin line is not a shielded system – more susceptible to noise and interference.
Twin line may be improved by using a form known as “twisted pair” (e.g., CAT 5 cable). This results in less interference.
l
-l
+
++
+
++
-
---
- -
E
Coax Twin lead
E
6
Another common example (for printed circuit boards):
Microstrip line
w
hr
Transmission Lines (cont.)
7
Transmission lines are commonly met on printed-circuit boards.
A microwave integrated circuit (MIC)
Microstrip line
8
Transmission Lines (cont.)
Microstrip line
Transmission Lines (cont.)
9
Microstrip
h
w
er
er
w
Stripline
h
Transmission lines commonly met on printed-circuit boards
Coplanar strips
her
w w
Coplanar waveguide (CPW)
her
w
10
Transmission Lines (cont.)
4 parameters
Symbol for transmission line:
z
Note: We use this schematic to represent a general transmission line, no matter what the actual shape of the conductors.
Transmission Lines (cont.)
11
+-
,V z t
,I z t
4 parameters
C = capacitance/length [F/m]
L = inductance/length [H/m]
R = resistance/length [/m]
G = conductance/length [S/m]
Four fundamental parameters that characterize any transmission line:
z
These are “per unit length” parameters.
Capacitance between the two wires
Inductance due to stored magnetic energy
Resistance due to the conductors
Conductance due to the filling material between the wires
Transmission Lines (cont.)
12
Circuit Model
Circuit Model:
Dz13
z
Dz
+-
,V z t
,I z t
RDz LDz
GDz CDz
z
Coaxial Cable
Example (coaxial cable)
r a
bz
0
0
2F/m
ln
ln H/m2
rCba
bL
a
2S/m
ln
1 1/m
2 2
d
a ma a mb
Gba
Ra b
2
m
(skin depth of metal)
d = conductivity of dielectric [S/m]
m = conductivity of metal [S/m]
14
,,
2a b
ma mb
ma
mb
Coaxial Cable (cont.)
Overview of derivation: capacitance per unit length
1QC
V z V
0 0
ln2 2
b b
r ra a
bV E d d
a
02
ln
rCba
15
l
-l
+
++
+
++
-
---
- -
E
a
b
Coaxial Cable (cont.)
Overview of derivation: inductance per unit length
1L
I z
0 0
0
2
ln2
b b
a a
Iz H d z d
I bz
a
0 ln2
bL
a
16
y
E
x
Js
b
a
Coaxial Cable (cont.)
Overview of derivation: conductance per unit length
2
ln
dGba
d
C G
RC Analogy:
2
lnC
ba
17
da
b
Coaxial Cable (cont.)
Relation Between L and C:
0 02F/m ln H/m
2ln
r bC L
b aa
0 0r rLC
Speed of light in dielectric medium: 1
dc
2
1
d
LCc
Hence:This is true for ALL transmission lines.
18
( A proof will be seen later.)
Telegrapher’s Equations
Apply KVL and KCL laws to a small slice of line:
+ V (z,t)-
RDz LDz
GDz CDz
I (z,t)
+ V (z+Dz,t)-
I (z+Dz,t)
z
z z+Dz
( , )KVL : ( , ) ( , ) ( , )
( , )KCL : ( , ) ( , ) ( , )
I z tV z t V z z t I z t R z L z
tV z z t
I z t I z z t V z z t G z C zt
19
Hence
( , ) ( , ) ( , )( , )
( , ) ( , ) ( , )( , )
V z z t V z t I z tRI z t L
z tI z z t I z t V z z t
GV z z t Cz t
Now let Dz 0:
V IRI L
z tI V
GV Cz t
“Telegrapher’s Equations (TEs)”
Telegrapher’s Equations (cont.)
20
To combine these, take the derivative of the first one with
respect to z:
2
2
2
2
V I IR L
z z z t
I IR L
z t z
V V VR GV C L G C
t t t
Take the derivative of the first TE with respect to z.
Substitute in from the second TE.
Telegrapher’s Equations (cont.)
21
I VGV C
z t
2 2
2 2( ) 0
V V VRG V RC LG LC
z t t
The same equation also holds for i.
Hence, we have:
2 2
2 2
V V V VR GV C L G C
z t t t
There is no exact solution to this differential equation, except for the lossless case.
Telegrapher’s Equations (cont.)
22
2 2
2 2( ) 0
V V VRG V RC LG LC
z t t
The same equation also holds for i.
Lossless case:
2 2
2 20
V VLC
z t
0R G
Note: The current satisfies the same differential equation.
Telegrapher’s Equations (cont.)
23
“wave equation”
The same equation also holds for i.
2 2
2 2 2
10
d
V V
z c t
Hence we have
Solution:
,d d
V z t f z c t g z c t
where f and g are arbitrary functions.
Solution to Telegrapher's Equations
This is called the D’Alembert solution to the wave equation (the solution is in the form of traveling waves).
24
Traveling Waves
2 2
2 2 2
1
d
V V
z c t
,d d
V z t f z c t g z c t
Proof of solution
2
2
22 2
2
,
,
d d
d d d d
V z tf z c t g z c t
zV z t
c f z c t c g z c tt
It is seen that the differential equation is satisfied by the general solution.
General solution:
25
Example(square pulse):
z
t = 0 t = t1 > 0 t = t2 > t1
z0 + cd t1z0 z0 + cd t2
V(z,t)
,d
V z t f z c t
26
z
f (z)
z0
t = 0
Traveling Waves (cont.)
“snapshots of the wave”
z
t = 0t = t1 > 0t = t2 > t1
z0 - cd t1 z0z0 - cd t2
V(z,t)
,d
V z t g z c t
27
z
g (z)
z0
t = 0
Traveling Waves (cont.)
Example(square pulse):
“snapshots of the wave”
Loss causes an attenuation in the signal level, and it also causes distortion (the pulse changes shape and usually gets broader).
z
t = 0 t = t1 > 0t = t2 > t1
z0 + cd t1z0 z0 + cd t2
V(z,t)
Traveling Waves (cont.)
(These effects can be studied numerically.)
28
Current
V IRI L
z t
V I
Lz t
Lossless
,d d
V z t f z c t g z c t
,d d
V z tf z c t g z c t
z
,d d
I z t u z c t v z c t
,d d d d
I z tc u z c t c v z c t
t
(first Telegrapher’s equation)
Our goal is to now solve for the current on the line.
Assume the following forms:
The derivatives are:
29
Current (cont.)
d d d d d df z c t g z c t L c u z c t c v z c t
V IL
z t
d d df z c t L c u z c t
d d dg z c t L c v z c t
1
1
d d
d
d d
d
u z c t f z c tLc
v z c t g z c tLc
This becomes
Equating like terms, we have
Hence we have
30
Note: There may be a constant of integration, but this would correspond to a DC current, which is ignored here.
1 1d
LLc L L
CLC
Then
0
0
1
1
d d
d d
u z c t f z c tZ
v z c t g z c tZ
Define the characteristic impedance Z0 of the line:
0
LZ
C The units of Z0 are Ohms.
Current (cont.)
Observation about term:
31
General solution:
,d d
V z t f z c t g z c t
0
1, d dI z t f z c t g z c t
Z
For a forward wave, the current waveform is the same as the voltage, but reduced in amplitude by a factor of Z0.
For a backward traveling wave, there is a minus sign as well.
Current (cont.)
32
Current (cont.)
z
Picture for a forward-traveling wave:
0
,
1,
d
d
V z t f z c t
I z t f z c tZ
+
- ,V z t
,I z t
forward-traveling wave
33
0
,
,
V z tZ
I z t
z
Physical interpretation of minus sign for the backward-traveling wave:
0
,
1,
d
d
V z t g z c t
I z t g z c tZ
+
- ,V z t
,I z t
backward-traveling wave
,I z t
The minus sign arises from the reference direction for the current.
Current (cont.)
34
0
,
,
V z tZ
I z t
0
,
,
V z tZ
I z t
Coaxial Cable
Example: Find the characteristic impedance of a coax.
0
0
2F/m
ln
ln H/m2
rCba
bL
a
0
00
ln2
2
ln
r
bL a
ZC
ba
00
0
1 1ln
2r
bZ
a
r a
bz
35
Coaxial Cable (cont.)
0 0
1 1ln
2r
bZ
a
00
0
0 376.7303
-120
-70
8.8541878 10 [F/m]
= 4 10 [H/m] ( )µ
exact
(intrinsic impedance of free space)
36
r a
bz
Twin Lead
10 0
1 1cosh
2r
dZ
a
d
a = radius of wires
r
10 0
1
F/m cosh H/m2
cosh2
r dC L
d aa
0 0
1 1ln
r
dZ
a
a d
37
Twin Line (cont.)
Coaxial cable
0 300Z
Twin line
0 75Z
These are the common values used for TV.
75-300 [] transformer
300 [] twin line 75 [] coax
38
w
hr
Microstrip Line
0
0
,
,
r
wC w h
hh
L w hw
0 0
1,
r
hZ
w
w h
Parallel-plate formulas:
39
Microstrip Line (cont.)
More accurate CAD formulas:
w
hr
w
hr
0
120
/ 1.393 0.667 ln / 1.444effr
Zw h w h
1 1 11 /
2 2 4.6 /1 12 /
eff r r rr
t h
w hh w
( / 1)w h
( / 1)w h
Note: The effective relative permittivity accounts for the fact that some of the fields are outside of the substrate, in the air region. The effective width w' accounts for the strip thickness.
21 ln
t hw w
t
t = strip thickness
40
Some Comments
Transmission-line theory is valid at any frequency, and for any type of waveform (assuming an ideal straight length of transmission line).
Transmission-line theory is perfectly consistent with Maxwell's equations (although we work with voltage and current, rather than electric and magnetic fields).
Circuit theory does not view two wires as a "transmission line": it cannot predict effects such as single propagation, reflection, distortion, etc.
41
One thing that transmission-line theory ignores is the effects of discontinuities (e.g. bends). These may cause reflections and possibly also radiation at high frequencies, depending on the type of line.