rf circuit design - [ch1-2] transmission line theory
TRANSCRIPT
Chapter 1-2
Transmission Line Theory
Chien-Jung Li
Department of Electronics Engineering
National Taipei University of Technology
Department of Electronic Engineering, NTUT
Common Types of Transmission Lines
Two-wire line
Coaxial
Microstrip
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Transmission Line Theory
• At high frequencies, especially when the wavelength is not longer than the dimension of circuitry, conventional circuit theory no longer holds.
• Circuitry perspective on electromagnetic waves.
• Transmission-line effects: Standing waves generated (related to position)
Load impedance changes
Departs from max power transmission
• Transmission-line effect is obvious as frequency or line length increases.
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Theory
Conventional
Circuit Theory
Microwave
Engineering Optics
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Electrical Model for Transmission Line
Source
Source
impedance
Load
impedance
• In conventional circuit theory, you can easily find the voltage
appears at load by: L
s
s L
Zv v
Z Z
Transmission line
sv
sZLZ
l
• If the transmission line is not just an ideal interconnection?
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Distributed Circuit Model
• Assume that the transmission line is uniform and the length l is divided into many identical
sections Δx.
• R: Ω/m, L: H/m, C: F/m, G: S/m
G x
L xR x
C xsZ
svLZ
l
dx dx dx
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A Section of the Transmission Line
• The voltages and currents along the trans-mission line are functions of position and time.
• Input: ,
• Output: ,
• R: finite conductivity G: dielectric loss
,v x t
,i x tR x L x
G x C x ,v x x t
,i x x t
,v x t ,i x t
,v x x t ,i x x t
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Transmission Line Equations (I)
• Apply Kirchhoff’s voltage law (KVL)
• Apply Kirchhoff’s current law (KCL)
,, , ,
i x tv x t v x x t R x i x t L x
t
,, , ,
v x x ti x t i x x t G x v x x t C x
t
,v x t
,i x tR x L x
G x C x ,v x x t
,i x x t
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Transmission Line Equations (II)
, ,,
v x t i x tRi x t L
x t
, ,,
i x t v x tGv x t C
x t
, , ,,
v x t v x x t i x tRi x t L
x t
, , ,,
i x t i x x t v x x tGv x x t C
x t
• Rearrange Δx then we have:
• Assume that Δx is very small
The partial differential equations describe the voltages and currents along
the transmissions, called transmission line, or telegrapher equation.
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Lossless Transmission Line
, ,,
v x t i x tRi x t L
x t
, ,,
i x t v x tGv x t C
x t
, ,v x t i x tL
x t
, ,i x t v x tC
x t
,v x t
,i x t
,v x x t
,i x x tL x
C x
• Of particular interest in microwave electronics is the lossless
transmission line, i.e., R=G=0.
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Sinusoidal Steady-state Analysis
f(x) and g(x) are the real functions of position, and , describe
the positional dependence of the phase.
, cos Re Rej t x j x j tv x t f x t x f x e f x e e
, cos Re Rej t x j x j ti x t g x t x g x e g x e e
j xI x g x e
j xV x f x e , Re j tv x t V x e
, Re j ti x t I x e
• Time-domain representation
x x
• Phasor-domain representation
time-domain
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Solve for the Voltage
V x I xL j LI x
x t
I x V xC j CV x
x t
dV xj LI x
dx
dI xj CV x
dx
V x dV x
x dx
2
2
2
d V x dI xj L LCV x
dx dx
• Laplace equation
2 2
2 2
2 2
d V x d V xLCV x V x
dx dx
LC• Propagation constant
• General solution
j x j xV x Ae Be ,where A, B are complex constant
• Lossless transmission line equations
(Think that if approaches zero?)
( is also called the “phase constant” that represents the phase change per
meter for the wave traveling along the path)
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Solve for the Current
1 1 j x j xdv x
I x A j e B j ej L dt j L
• Solve for the current
LC
• Define
0
L L LZ
CLC
j x j xA e B eL L
j x j xV x Ae Be
0 0
j x j xA BI x e e
Z Z
dV xj LI x
dxWith and
,where
Z0 is the characteristics impedance of the transmission line, for the lossless
condition Z0 is real.
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Time-domain Results
, Re Re
j x t j x tj tv x t V x e Ae Be
0 0
, Re Rej x t j x tj t A B
i x t I x e e eZ Z
cos cosA x t B x t
0 0
cos cosA B
x t x tZ Z
j x j xV x Ae Be
0 0
j x j xA BI x e e
Z Z
• Time-domain results can be easily drawn from the phasor.
Voltage Wave
Current Wave
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Wave Wavelength
j xV x Ae
• Consider
Take a look on the term , the phase means how many radians
change for the wave to travel through the distance of x. If distance x is
equal to a wavelength long, i.e., :
j xe x
2
xx
2
0x x
0t t T
distance
time
phase
0xx
2
xx
1 , Re cosj x j tv x t Ae e A t x
x
For simplification, assume the
wave starts from x=0 and t=0.
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Wave Velocity
In the vacuum, 7
0 4 10 Wb/A-mL
0 8.85419 F/mC
8
,
0 0
1 light speed 3 10 /p vacuumv c m s
0
0
0
377 L
ZC
,
0
p vaccumv
fis the wavelength in vacuum
2 1
2 2pv f
T LC
• Wave velocity can be found: ( the wave goes one wavelength long in a period of T)
is the intrinsic/characteristic
impedance of vacuum (or free-space)
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Wave Propagation in Material
0 0r
8
0 0
1 3 10/p
r r r
cv m s
Propagation in material with relative dielectric constant r
(non-magnetic material)
0p r
g
r
cv
f f
Take water for an example:
8
7
,
3 103.32 10 /
81.5p waterv m s
0
, 00.1181.5
g water
The propagation speed is slower than that in vacuum, and the wavelength
is also shorter than that in vacuum.
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Wave at a Certain Point
2
t Tt
2T
1 , cosv x t A x t
0x
1 0, cosv t A t
2t
00
tt
A
A
1 0, cosv t A t
0x x l
0x
x l• Consider
At position
We only pay attention to this point
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Wave at a Certain Time
2
xx
2
1 , cosv x t A x t
0t
1 ,0 cosv x A x
2 x
00
xx
A
A
1 ,0 cosv x A x
0x x l
0x
x l
• Consider
At time
We now pay attention to the whole line
at any time instant (here, t=0)
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Wave Propagation versus x and t
2 x
A
A
t
t T
2t T
x
x
t
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Wave at Point x=
2 x
A
A
t
t T
2t T
t
0x x l
We only pay attention to this point
x
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Terminated Transmission Line
LZ LZ0Z 0Z
j xAe
j xBe j xBe
j xAe
0x x l 0dd l
j x j xV x Ae Be
0 0
j x j xA BI x e e
Z Z
IN d
1 1
j d j dV d A e B e
1 1
0 0
j d j dA BI d e e
Z Z
1
jA Ae l 1
jB Be lwhere and
d xl
incident wave
reflected wave
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Reflection Coefficient
1 1
j d j dV d A e B e 1
jA Ae l 1
jB Be l
2 21 1
0
1 1
j dj d j d
IN j d
B e Bd e e
A e A
10
1
0IN
B
A
where and
• Moves from the load (at d=0) toward the source (at d=l)
where is the load reflection coefficient, which is the value
of at d=0:
0
IN d
incident wave reflected wave
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Reflection Coefficient at Load
2
1 0 1 01j d j d j d j dV d A e e A e e
21 10 0
0 0
1j d j d j d j dA AI d e e e e
Z Z
00
0
j d j d
IN j d j d
V d e eZ d Z
I d e e
00
0
10
1IN LZ Z Z
00
0
L
L
Z Z
Z Z
1 1
j d j dV d Ae B e
1 1
0 0
j d j dA BI d e e
Z Z
Input impedance of the transmission line at any position d
is defined as
Use boundary condition at load (d=0)
0 0 when 0LZ ZProperly terminated (matched line):
LZ V d
0dd l
IN d
INZ d
I d
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Input Impedance of a Terminated Line
0 0
0
0 0
j d j d
L L
IN j d j d
L L
Z Z e Z Z eZ d Z
Z Z e Z Z e
00
0
cos sin
cos sinL
L
Z d jZ dZ
Z d jZ d
00
0
tan
tanL
L
Z jZ dZ
Z jZ d
00
0
L
L
Z Z
Z Z
00
0
j d j d
IN j d j d
V d e eZ d Z
I d e e
It gives the value of the input impedance at any position d along the
transmission line
At d=0 0IN LZ Z
At d=l
00
0
tan
tanL
IN
L
Z jZZ Z
Z jZ
ll
l
A very important property of a transmission line is the ability to change
a load impedance to another value of impedance as its input.
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Voltage Standing-wave Ratio (VSWR)
2
1 01 j dV d A e
1 0max1V d A 1 0min
1V d A
0max
0min
1
1
V dVSWR
V d
The addition of the two waves traveling in opposite directions in a
transmission line produces a standing-wave pattern – that is,
a sinusoidal function of time whose amplitude is a function of position.
2
1 0 1 01j d j d j d j dV d A e e Ae e
Magnitude of the voltage along the line:
The voltage standing-wave ratio (VSWR):
Next we will discuss 4 important cases of the terminated line, which are
matched line, short-circuited line, open-circuited line, and quarter-wave line.
and
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Matched Line (Properly Terminated)
• Matched line: the characteristic impedance is equal to the
load impedance, i.e., IN LZ d Z
0LZ Z
0dd l
l 0INZ Z
0INZ d Z
0Z
There is no reflection wave, the input impedance is at any location d,
VSWR has its minimum value of 1, i.e., 0 0 1VSWRand 0Z
No matter how long the line is, there is no transmission line effects .
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Short-Circuited Line
• For , it follows that , , and the
input impedance at a distance d from the load, , is
given by 0 tanscZ d jZ d
The amplitude of the incident and reflected waves are
the same since (total reflection from the load), VSWR attains
its largest value of infinity.
0LZ
0dd l
l l 0 tanINZ jZ
0 tanscZ d jZ d
0Z
0LZ 0 1 VSWR
scZ d
When
Short-circuited load is transformed to
open-circuited.
0 1
l
4
l scZ
When
Short-circuited load is still short-
circuited seen from the input.
l
2
l 0scZ
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Open-Circuited Line
• For , it follows that , , and the
input impedance at a distance d from the load, , is
given by
The amplitude of the incident and reflected waves are
the same since (total reflection from the load), VSWR attains
its largest value of infinity.
LZ 0 1 VSWR
ocZ d
When
Open-circuited load is transformed to
short-circuited.
0 1
l
4
l 0ocZ
When
Open-circuited load is still open-
circuited seen from the input.
l
2
l ocZ
0 cotocZ d jZ d
LZ
0dd l
l l 0 cotINZ jZ
0 cotocZ d jZ d
0Z
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Quarter-wave Line
• Quarter-wave transformer:
2
04IN
L
ZZ
Z
0 4IN LZ Z Z
In order to transform a real impedance to another real impedance
given by , a quarter-wave line with real characteristic impedance
of value
can be used.
LZ
0d
4d
2
0
4IN
L
ZZ
Z
0Z
l
4
d
LZ 4INZ
Example: , how to trans-
form it to at certain frequency?
75 LZ50
0 4 50 75 61.2 IN LZ Z Z
You can simply use a transmission line
with 61.2 Ohm characteristic impedance! 4
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Half-wave Line
• Half-wave line:
2IN LZ Z
No matter what the line impedance is, when a half-wave line is used
and it does not affect the impedance seen from the input.
LZ
0d
2d
2IN LZ Z
0Z
2IN LZ Z
l
2
d
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Voltage on the Shorted-circuited Line
1 12 sinj d j dV d A e e j A d
2
1, Re Re 2 sinj t
j tv d t V d e A d e
When
1 14 2 sin 2 2V j A j A
12 2 sin 0V j A
4d
When
2
d
• Voltage on the short-circuited line:
incident wave reflected wave
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Standing-wave Pattern
1, 2 sin cos2
v d t A d t
2
3
2
2
max
min
V dVSWR
V d
V d
1 max2A V d
min
0 V dd
d
2
4
3
4
In order to proceed we need to know the value of the complex constant A1.
For simplicity let us assume that A1 is real. Hence we obtain
2
3
2
2
,v d t
12A
min
0 V dd
d
2
4
3
4
12A
32
t 54
t
3,4 4
t 2
t
0,t
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Example(I)
100 50sZ j 50 50LZ j
10 0sv
50 5010 0 3.92 11.31
50 50 100 50L
L s
L s
jZV V
Z Z j j
Consider the circuit shown below that there is no transmission line
between the source and load, find the voltage at the terminal of the
load.
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Example(II)
Find the load reflection coefficient, the input impedance, and the
VSWR in the transmission line shown, the length of the
transmission line is and its characteristic impedance is 50
Ohm.
10 0sv
100 50sZ j 50 50LZ j
l
00
0
50 50 500.447 63.44
50 50 50L
L
jZ Z
Z Z j
50 50 50 tan458 50 100 50
50 50 50 tan45IN
j jZ j
j j
0
0
1 1 0.4472.62
1 1 0.447VSWR
8
0 50Z
8
8INZ
LV
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Example(III)
8 100 508 10 0 5.59 26.57
8 100 50 100 50
IN
s
IN s
Z jV V
Z Z j j
2
1 01j d j dV d A e e
4 218 5.59 26.57 1 0.447 63.44
j j
V A e e 1 3.95 63.44A
0 3.95 63.44 1.77 5 45LV V
100 50sZ j
10 0sv
8 100 50INZ j
Equivalent circuit
Transmission-line effect makes things different! It is not always bad, since it
cab be used for matching and makes maximum power transfer possible.
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V x
I xR x j L x
G x j C x
V x x
I x x
Lossy Transmission Line
dV xR j L I x
dx
dI xG j C V x
dx
2
2
2
d V xV x
dx
j R j L G j C
Complex propagation constant
is the attenuation constant in
nepers/m and propagation constant
is in rads/m
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Reflection Coefficient and Input Impedance
, Re Rej x t j x tj t x xv x t V x e Ae e Be e
0 0
, Re Rej x t j x tj t x xA B
i x t I x e e e e eZ Z
With x=l - d
1 1
d dV d A e B e
1 1
0 0
d dA BI d e e
Z Z
l1A Ae l1B Be
The reflection coefficient of the terminated lossy line
21
0
1
dd
IN d
B ed e
A ewhere
010
1 0
0 LIN
L
Z ZB
A Z Z
00
0
tanh
tanhL
IN
L
Z Z dZ d Z
Z Z d
where and
The impedance of the terminated lossy line
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Summary (I)
00
0
tanh
tanhL
IN
L
Z Z dZ d Z
Z Z d
2
0
d
IN d e
00
0
L
L
Z Z
Z Z
0
0
1
1VSWR
00
0
tan
tanL
IN
L
Z jZ dZ d Z
Z jZ d
2
0
j d
IN d e
pv
2
LC• Propagation constant
• Reflection coefficient at load
• Reflection coefficient at any position lossless
• Input impedance
lossless
j where
• Phase velocity
• Wavelength
• Voltage standing wave ratio
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Summary (II)
• Transmission line affects the input impedance, and you
may not get the voltage you want at the load. On the other
hand, this property is useful when you need impedance
matching to get maximum power transfer.
• Both the wave velocity and wavelength decreases when the
wave travels from vacuum into the material that has a
relative dielectric constant greater than 1.
• Generally speaking, when the circuit dimension is
under , the transmission effects can be considered
negligible.
20
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