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1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II
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Page 1: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

1

EKT 441MICROWAVE COMMUNICATIONS

CHAPTER 5:

MICROWAVE FILTERS

PART II

Page 2: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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f2

Filter Realization Using Distributed Circuit Elements (1) Lumped-element filter realization using surface mounted inductors and

capacitors generally works well at lower frequency (at UHF, say < 3 GHz). At higher frequencies, the practical inductors and capacitors loses their intrinsic

characteristics. Also a limited range of component values are available from manufacturer. Therefore for microwave frequencies (> 3 GHz), passive filter is usually realized

using distributed circuit elements such as transmission line sections. Here we will focus on stripline microwave circuits.

Page 3: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Zo

Zo

Filter Realization Using Distributed Circuit Elements (2) Recall in the study of Terminated Transmission Line Circuit that a

length of terminated Tline can be used to approximate an inductor and capacitor.

This concept forms the basis of transforming the LC passive filter into distributed circuit elements.

Zo

Zo

Zc ,

l

L

Zc ,

l

C

Page 4: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Filter Realization Using Distributed Circuit Elements (3)

This approach is only approximate. There will be deviation between the actual LC filter response and those implemented with terminated Tline.

Also the frequency response of distributed circuit filter is periodic. Other issues are shown below.

How do we implement series Tlineconnection ? (only practical forcertain Tline configuration)

Connection physicallength cannot beignored atmicrowave region,comparable to

Thus some theorems are used to facilitate the transformation of LCcircuit into stripline microwave circuits.Chief among these are the Kuroda’sIdentities (See Appendix)

Thus some theorems are used to facilitate the transformation of LCcircuit into stripline microwave circuits.Chief among these are the Kuroda’sIdentities (See Appendix)

Zo

Zo

Page 5: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

5

More on Approximating L and C with Terminated Tline: Richard’s Transformation

Zc ,

l

L jLLjljZZ cin tanZin

LZ

l

c tan

(3.1.1a)

Zc ,

l

CZin jCCjljYY cin tan

CY

l

cZc

1

tan (3.1.1b)

For LPP design, a further requirment isthat:

1tan cl (3.1.1c)8

2 1tan cc

ll

Wavelength atcut-off frequency

Page 6: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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More on Approximating L and C with Terminated Tline: Richard’s Transformation

Page 7: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Kuroda’s Identities

As taken from [2].

122 1ZZ

n

Z1

l

21Z Z2/n2

l

nZ1

Z2

l

221

Znn2Z1

l

1Z

Z2

l

21

n

ZZ2/n2

l

1Z

1: n2

Z1

l

221

Znn2Z1

l

21Z

n2: 1

Note: The inductor representsshorted Tline while the capacitorrepresents open-circuit Tline.

Page 8: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 – LPF Design Using Stripline

Design a 3rd order Butterworth Low-Pass Filter. Rs = RL= 50Ohm, fc = 1.5GHz.

Step 1 & 2: LPP

Zo=1

g1 1.000H

g3 1.000H

g2 2.000F

g4

1

Length = c/8for all Tlinesat = 1 rad/s

500.0000.21

Page 9: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 – LPF Design Using Stripline

Design a 3rd order Butterworth Low-Pass Filter. Rs = RL= 50Ohm, fc = 1.5GHz.

Step 3: Convert to Tlines using Richard’s Transformation Length = c/8for all Tlinesat = 1 rad/s

500.0000.21

Z0=1 Z0=1

Z0=0.5

Page 10: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Z0=1 Z0=1

Z0=0.5

UE UE

Z0=1 Z0=1

Example 5.7 Cont…

Length = c/8for all Tlinesat = 1 rad/s

Step 4: Add extra Tline on the series connection Extra T-lines

Page 11: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 Cont…

Step 5: apply Kuroda’s 1st Identity.

Similar operation isperformed here

Z0=1 Z0=1

Z0=0.5

UE UE

Z0=1 Z0=1

Step 6: apply Kuroda’s 2nd Identity.

Page 12: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 Cont…

After applying Kuroda’s Identity.

Length = c/8for all Tlinesat = 1 rad/s

Since all Tlines have similar physicallength, this approach to stripline filterimplementation is also known as Commensurate Line Approach.

Since all Tlines have similar physicallength, this approach to stripline filterimplementation is also known as Commensurate Line Approach.

Z0=0.5

Z0=2 Z0=2

Z0=2 Z0=2

Page 13: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 Cont…

Length = c/8for all Tlines atf = fc = 1.5GHz

Zc/Ω /8 @ 1.5GHz /mm W /mm 50 13.45 2.8525 12.77 8.00100 14.23 0.61

Microstrip line using double-sided FR4 PCB (r = 4.6, H=1.57mm)

Step 5: Impedance and frequency denormalization.

Z0=25

Z0=100 Z0=100

Z0=100 Z0=100

Page 14: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.7 Cont…

Step 6: The layout (top view)

Page 15: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.8

Design a low pass filter for fabrication using microstrip lines. The specifications are: cutoff freq of 4 GHz, third order, impedance of 50 ohms and a 3dB equal ripple characteristics

g1 = 3.3487 = L1

g2 = 0.7117 = C2

g3 = 3.3487 = L3

g4 = 1.0000 = RL

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Example 5.8 (cont)

Page 17: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.8 (cont)

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Example 5.8 (cont)

Page 19: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Example 5.8 (cont)

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Kuroda’s Identities

As taken from [2].122 1ZZ

n Note: The inductor representsshorted Tline while the capacitorrepresents open-circuit Tline.

1Z

2

2

n

Z2

1

n

Z2Z

2

2Zn1Z

2Z 1

2Zn

Page 21: 1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 5: MICROWAVE FILTERS PART II.

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Kuroda’s Identities

As taken from [2].122 1ZZ

n Note: The inductor representsshorted Tline while the capacitorrepresents open-circuit Tline.

2

2

n

Z2

1

n

Z

2:1 n

1

2Zn

2

2

1

Zn

1:2n

1Z

2Z

2Z 1

Z


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