서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2...
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![Page 1: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/1.jpg)
서강대학교 전자공학과윤상원 교수
2. Smith Chart
![Page 2: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/2.jpg)
Microwave & Millimeter-wave Lab. 2
차 례
1. Smith chart ; introduction --------------------------------2. Reflection coeff. and impedance ----------------------3. Normalized impedance equation ----------------------4. Impedance Transformation ------------------------------5. Some transmission line example -------------------6. Admittance transformation ------------------------------7. Parallel and series connections ------------------------8. Single stub matching ----------------------------------------
3 4 61020222632
![Page 3: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/3.jpg)
Microwave & Millimeter-wave Lab. 3
1. Smith chart ; introduction
Distributed nature of the transmission line Impedance is repeated periodically
One-to-one correspondence between the impedance and the reflection coeff. Impedances of the passive circuits are mapped into unit circle of the reflection coefficient plane. Impedance is treated as a reflection coefficient.
Smith chart ; a unit circle which contains all the impedance of the passive circuits
![Page 4: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/4.jpg)
Microwave & Millimeter-wave Lab. 4
2. Reflection coeff. and impedance
Reflection coefficient in phasor form
example
riLj
irL
L LejZZ
ZZ00
1000
0
00 /tan where
1 0 0 LZ
0 50 0 LZ1 0 LZ
o0 34 83.0 )15050( jZL
![Page 5: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/5.jpg)
Microwave & Millimeter-wave Lab. 5
Reflection coefficient and impedance(2)
0
30
60120
150
180
210
240 300
330
0=+10=- 1
0=0
0=0.83<34o0.8
0.4
![Page 6: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/6.jpg)
Microwave & Millimeter-wave Lab. 6
3. Normalized impedance equation
Input impedance ; reflection coefficient
z=- d z=0
Z0 Z L
Z in 0d
irdjj
d ee L 20
ir
irin j
jZdZ
1
10
Normalize the impedance as
ir
irinin j
j
d
djxrzZdZ
1
1
1
1/)( 0
A mapping from zin-plane to -plane
![Page 7: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/7.jpg)
Microwave & Millimeter-wave Lab.
Reflection Coeff. Plane
7
![Page 8: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/8.jpg)
Microwave & Millimeter-wave Lab. 8
Normalized impedance equation(2)
Normalized impedance vs. reflection coeff.
22
22
)1(
21
ir
iirin
jjxrz
Real and imaginary terms ;
, )1(
122
22
ir
irr
22)1(
2
ir
ix
Normalized impedance is represented in terms of the reflection coefficient. impedance can be plotted in the reflection coefficient plane.
![Page 9: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/9.jpg)
Microwave & Millimeter-wave Lab.
Smith Chart
9
, 1
1
1
22
2
rr
rir
22
2 111
xxir
Normalized impedance is transformed to ;
Real Part(resistance)
Imaginary Part(reactance)
![Page 10: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/10.jpg)
Microwave & Millimeter-wave Lab.
Real Part(resistance)
10
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Microwave & Millimeter-wave Lab.
Imaginary Part(reactance)
11
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Microwave & Millimeter-wave Lab.
Smith Chart(1)
12
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Microwave & Millimeter-wave Lab. 13
Smith Chart(2)
Normalized impedance is transformed to ;
, 1
1
1
22
2
rr
rir
222 11
1
xxir
![Page 14: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/14.jpg)
Microwave & Millimeter-wave Lab. 14
The Smith Chart(3)
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Microwave & Millimeter-wave Lab. 15
4. Impedance Transformation
For general load ; reflection coefficient
z=- d z=0
Z0 Z L
Z in 0d djjd ee L 2
0
Only phase changes as d increases or decreases for lossless transmission line.But, impedance changes its magnitude and phase
Calculation of input impedance using reflection coefficient on the Smith Chart ; “ 6 steps in the textbook “
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Microwave & Millimeter-wave Lab. 16
Impedance Transformation(2)
1. Normalize the load impedance ZL with Z0 ;
2. Locate zL in the Smith Chart ;
3. Identify the load reflection coefficient in the Smith Chart in terms of its magnitude and phase.
4. Rotate 0 by its electrical length 2d to obtain in(d).
5. Record the normalized input impedance at this spatial location d ;
6. Convert into the actual impedance ;
inz
inz inZ
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Microwave & Millimeter-wave Lab. 17
Impedance Transformation(3)
Example 3-3 ;
z=- d z=0
Z0 Z L
Z in 0d 6030 jZL
GHzcmdZ 2at 2 , 500
odm 99.1912 , 77.832 1
1. Normalize the load impedance ZL with Z0 ;
2. Locate zL in the Smith Chart ;
2.16.050/6030 jjzL
![Page 18: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/18.jpg)
Microwave & Millimeter-wave Lab. 18
Impedance Transformation(4)
3. Identify the load reflection coefficient in the Smith Chart in terms of its magnitude and phase.
4. Rotate 0 by its electrical length 2d to obtain in(d) ;
5. Record the normalized input impedance at this spatial location d ;
6. Convert into the actual impedance ;
* exact calculation leads to
od 99.1912
53.03.0 jzin
inz
5.2615 jZin 7.267.14 jZin
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Microwave & Millimeter-wave Lab. 19
Impedance Transformation(5)
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Microwave & Millimeter-wave Lab.
Example 10.10
The use of the transmission line chart is best shown by example . Let us again consider a load impedance, ZL=25+j50 , terminating a 50- line. The line length is 60cm and the operating frequency is such that the wavelength on theline is 2m. We desire the input impedance.
Solution. We have , and we readBy drawing a straight line from the origin through A to the circumference, we note a reading of 0.135On the wtg scale. We have And it is, therefore, 0.3 from the load to the inputWe therefore find on the circle oppositeWtg reading of 0.135+0.300=0.435. And the pointlocating the input impedance is marked B. TheNormalized input impedance is read as 0.28-j0.40,and thus . A more accurate analyticalCalculation gives .
20
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Microwave & Millimeter-wave Lab.
D10.6
A load is located at z=0 on a lossless 50- line. The operating frequency is 200MHz and the wavelength on the line is2m.(a)If the line is 0.8m in length, use the Smith chart to find the input Impedance.
Therefore 0.4 from the load to theinput. Using smith chart tool, the pointlocating the input impedance ismarked B.The input impedance is read 79+j99
21
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Microwave & Millimeter-wave Lab. 22
D10.6
(b)What is s?
![Page 23: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/23.jpg)
Microwave & Millimeter-wave Lab. 23
2-6. Admittance transformation
Parametric admittance equation Normalized admittance equation
The conventional Smith Chart(Z-Smith Chart) gives
on the Smith Chart admittance located at 180o
away from the impedance point.
)(1
)(11
0 d
d
zY
Yy
in
inin
)(1
)(1
)(1
)(1
de
de
d
dj
j
![Page 24: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/24.jpg)
Microwave & Millimeter-wave Lab. 24
Admittance transformation(2)
Example 3-6 ; convert the normalized input impedance given as
to normalized admittance.<solution> by direct inversion
4211
j
in ejz
2
1
2
1
2
1 4 jeyj
in
![Page 25: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/25.jpg)
Microwave & Millimeter-wave Lab. 25
Admittance transformation(3)
Admittance Smith Chart(Y-Smith Chart)
![Page 26: 서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction -------------------------------- 2.](https://reader036.fdocuments.net/reader036/viewer/2022062314/56649e3b5503460f94b2d093/html5/thumbnails/26.jpg)
Microwave & Millimeter-wave Lab. 26
Admittance transformation(4)
ZY-Smith Chart
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Microwave & Millimeter-wave Lab. 27
2-7. Parallel and series connections
Parallel connection of R and L elements
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Microwave & Millimeter-wave Lab. 28
Parallel and series connections(2)
Parallel connection of R and C elements
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Microwave & Millimeter-wave Lab. 29
Parallel and series connections(3)
Series connection of R and L elements
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Microwave & Millimeter-wave Lab. 30
Parallel and series connections(4)
Series connection of R and C elements
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Microwave & Millimeter-wave Lab. 31
Parallel and series connections(5)
Example of a T-network
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Microwave & Millimeter-wave Lab. 32
Parallel and series connections(6)
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Microwave & Millimeter-wave Lab. 33
2-8. Single stub matching
Impedance matching using distributed element
d1
yL
y in y'in
y0 =1
jby in 1'
Input admittance at d1 ;
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Microwave & Millimeter-wave Lab. 34
Single stub matching(2)
Stub length
d
yL
y in y'in
y stub
y0 =1
jbystub
Stub length l1 ;