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Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n 112 [email protected] http://scholar.cu.edu.eg/refky/

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Page 1: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Network Synthesis

Part I

Dr. Mohamed Refky Amin

Electronics and Electrical Communications Engineering Department (EECE)

Cairo University

[email protected]

http://scholar.cu.edu.eg/refky/

Page 2: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

OUTLINE

• References

• Definition

• Network Functions

• Realizability Conditions

2Dr. Mohamed Refky

Page 3: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Gabor C. Temes & Jack W. Lapatra, “Introduction to Circuit

Synthesis and Design”, McGraw-Hill Book Company.

M.E. Van Valkenburg, “Introduction to Modern Network

Synthesis”, John Wiley Inc.

References

3Dr. Mohamed Refky

Page 4: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

What we have used to do so far is the calculation of the response

of a known circuit to a given excitation.

This is called analysis of circuits.

Network Synthesis

4

Definition

Dr. Mohamed Refky

Page 5: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

In network synthesis we try to find a new circuit that provides a

required response to a given input excitation

Network Synthesis

5

Definition

Dr. Mohamed Refky

Synthesis solutions are not unique

Page 6: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

In network synthesis, complex frequency

𝑠 = 𝛿 + 𝑗𝜔

is used to analyze the circuits because it simplifies algebraic work

by including the imaginary part in 𝑠.

Network Synthesis

6

Definition

Dr. Mohamed Refky

𝐼 =𝑉

𝑅 + 𝑗𝜔𝐿 +1𝑗𝜔𝐶

𝐼 =𝑉

𝑅 + 𝑠𝐿 +1𝑠𝐶

Page 7: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a single port network, synthesis may be operated on the

following functions:

Network Synthesis

7

One-Port Networks

Dr. Mohamed Refky

𝑉 𝑠

𝐼 𝑠

𝐼 𝑠

𝑉 𝑠

Driving point impedance

𝑍 𝑠 =

Driving point admittance

𝑌 𝑠 =

Page 8: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a two port network, synthesis may be operated on the

following functions:

Network Synthesis

8

Two-Port Networks

Dr. Mohamed Refky

𝑉1 𝑠

𝐼1 𝑠

𝑉2 𝑠

𝐼2 𝑠

Driving point impedance

𝑍11 𝑠 =

Driving point admittance

𝑍22 𝑠 =

Page 9: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a two port network, synthesis may be operated on the

following functions:

Network Synthesis

9

Two-Port Networks

Dr. Mohamed Refky

𝑉1 𝑠

−𝐼2 𝑠

−𝐼2 𝑠

𝑉1 𝑠

Driving point impedance

𝑍12 𝑠 =

Driving point admittance

𝑌21 𝑠 =

Page 10: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a two port network, synthesis may be operated on the

following functions:

Network Synthesis

10

Two-Port Networks

Dr. Mohamed Refky

𝑉2 𝑠

𝑉1 𝑠

−𝐼2 𝑠

𝐼1 𝑠

Driving point impedance

𝐺21 𝑠 =

Driving point admittance

𝛼21 𝑠 =

Page 11: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

We will focus on the synthesis of driving point functions for one-

port networks.

The functions used are generally in the form of ratios of

polynomials

𝑍 𝑠 or 𝑌 𝑠

Network Synthesis

11

One-Port Networks

Dr. Mohamed Refky

=𝜙 𝑠

𝜓 𝑠=𝛼𝑚𝑠

𝑚 + 𝛼𝑚−1𝑠𝑚−1 +⋯+ 𝛼0

𝛽𝑛𝑠𝑛 + 𝛽𝑛−1𝑠

𝑛−1 +⋯+ 𝛽0

=𝛾𝑚𝛾𝑛

𝑠 − 𝑧1 𝑠 − 𝑧2 … 𝑠 − 𝑧𝑚𝑠 − 𝑝1 𝑠 − 𝑝2 … 𝑠 − 𝑝𝑛

Page 12: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

𝑍 𝑠 =1

𝑠𝐶// 𝑅 + 𝑠𝐿

=

1𝑠𝐶

𝑅 + 𝑠𝐿

𝑅 + 𝑠𝐿 +1𝑠𝐶

=𝑅 + 𝑠𝐿

𝑠𝐶𝑅 + 𝑠2𝐿𝐶 + 1

Network Synthesis

12

Example (1)

Dr. Mohamed Refky

Find the impedance of the shown circuit

Page 13: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

𝑍 𝑠 or 𝑌 𝑠

𝛼’s and 𝛽’s are positive constants

𝑚 is the orders of 𝜙 𝑠 .

𝑛 are the orders of 𝜓 𝑠 .

Network Synthesis

13

One-Port Networks

Dr. Mohamed Refky

=𝜙 𝑠

𝜓 𝑠=𝛼𝑚𝑠

𝑚 + 𝛼𝑚−1𝑠𝑚−1 +⋯+ 𝛼0

𝛽𝑛𝑠𝑛 + 𝛽𝑛−1𝑠

𝑛−1 +⋯+ 𝛽0

Page 14: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

𝑍 𝑠 or 𝑌 𝑠

𝑧1, 𝑧2, …, 𝑧𝑚 are the zeros of 𝑍 𝑠 or 𝑌 𝑠

𝑝1, 𝑝2, …, 𝑝𝑛 are the poles of 𝑍 𝑠 or 𝑌 𝑠

Network Synthesis

14

One-Port Networks

Dr. Mohamed Refky

=𝜙 𝑠

𝜓 𝑠=𝛼𝑚𝑠

𝑚 + 𝛼𝑚−1𝑠𝑚−1 +⋯+ 𝛼0

𝛼𝑛𝑠𝑛 + 𝛽𝑛−1𝑠

𝑛−1 +⋯+ 𝛽0

𝛾𝑚𝛾𝑛

𝑠 − 𝑧1 𝑠 − 𝑧2 … 𝑠 − 𝑧𝑚𝑠 − 𝑝1 𝑠 − 𝑝2 … 𝑠 − 𝑝𝑛

𝛾𝑚𝛾𝑛

is the scale factor

Page 15: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For series impedances

𝑍 𝑠 = 𝑍1 𝑠 + 𝑍2 𝑠

For parallel impedances

𝑍 𝑠 =1

𝑌1 𝑠 + 𝑌2 𝑠

Network Synthesis

15

Realization of a Function

Dr. Mohamed Refky

=1

1𝑍1 𝑠

+1

𝑍2 𝑠

Page 16: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For series impedances

𝑌 𝑠 =1

𝑍1 𝑠 + 𝑍2 𝑠

For parallel impedances

𝑌 𝑠 = 𝑌1 𝑠 + 𝑌2 𝑠

Network Synthesis

16

Realization of a Function

Dr. Mohamed Refky

=1

𝑍1 𝑠+

1

𝑍1 𝑠

Page 17: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a combination of series and

parallel impedances

𝑍 𝑠 = 𝑍1 𝑠 + 𝑍𝑝 𝑠

Network Synthesis

17

Realization of a Function

Dr. Mohamed Refky

= 𝑍1 𝑠 +1

1𝑍2 𝑠

+1

𝑍3 𝑠

= 𝑍1 𝑠 +1

𝑌2 𝑠 + 𝑌3 𝑠

Page 18: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a combination of series and

parallel impedances

𝑍 𝑠 =1

𝑌1 𝑠 + 𝑌2 𝑠

Network Synthesis

18

Realization of a Function

Dr. Mohamed Refky

=1

1𝑍1 𝑠

+1

𝑍2 𝑠 + 𝑍3 𝑠

Page 19: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a combination of series and

parallel impedances

𝑌 𝑠 =1

𝑍1 𝑠 + 𝑍𝑝 𝑠

Network Synthesis

19

Realization of a Function

Dr. Mohamed Refky

=1

𝑍1 𝑠 +1

𝑌2 𝑠 + 𝑌3 𝑠

=1

𝑍1 𝑠 +1

1𝑍2 𝑠

+1

𝑍3 𝑠

Page 20: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

For a combination of series and

parallel impedances

𝑌 𝑠 = 𝑌1 𝑠 + 𝑌𝑠 𝑠

Network Synthesis

20

Realization of a Function

Dr. Mohamed Refky

=1

𝑍1 𝑠+

1

𝑍2 𝑠 + 𝑍3 𝑠

Page 21: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

𝑍 𝑠 = 𝑍1 𝑠 +1

𝑌2 𝑠 +1

𝑍3 𝑠 +1

𝑌4 𝑠 +1

𝑍5 𝑠 + ⋯

𝑌 𝑠 = 𝑌1 𝑠 +1

𝑍2 𝑠 +1

𝑌3 𝑠 +1

𝑍4 𝑠 +1

𝑌5 𝑠 + ⋯

Network Synthesis

21

Realization of a Function

Dr. Mohamed Refky

Page 22: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Network Synthesis

22

Realization of a Function

Dr. Mohamed Refky

𝑍 𝑠 =1

𝑠𝐶 +1

𝑅 + 𝑠𝐿

𝑍 𝑠 =𝑠𝐿 + 𝑅

𝑠2𝐿𝐶 + 𝑠𝑅𝐶 + 1

Page 23: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Network Synthesis

23

Realization of a Function

Dr. Mohamed Refky

𝑍 𝑠 =1

𝑠𝐶 +1

𝑅 + 𝑠𝐿

𝑍 𝑠 =𝑠𝐿 + 𝑅

𝑠2𝐿𝐶 + 𝑠𝑅𝐶 + 1

In network synthesis, we try to find a way to convert the function

(𝑍 𝑠 or 𝑌 𝑠 ) into a form that is easier to be realized into a

circuit.

Page 24: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

1) The function must be a Positive Real (PR)

𝑅𝑒𝑎𝑙 𝑍 𝑠 or 𝑌 𝑠 ≥ 0 for 𝑅𝑒𝑎𝑙 𝑠 ≥ 0

This condition means that the power flows from the source to the

circuit

Network Synthesis

24

Realizability Conditions

Dr. Mohamed Refky

𝑍1 𝑠 = 𝑅 + 𝑠𝑋 𝑍2 𝑠 = −𝑅 + 𝑠𝑋

𝑌1 𝑠 = 𝐺 +1

𝑠𝑋𝑌2 𝑠 = −𝐺 +

1

𝑠𝑋

Page 25: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

1) The function must be a Positive Real (PR)

𝑅𝑒𝑎𝑙 𝑍 𝑠 or 𝑌 𝑠 ≥ 0 for 𝑅𝑒𝑎𝑙 𝑠 ≥ 0

This condition means that the power flows from the source to the

circuit

The poles of the function are negative or, if complex, they have

a negative real part. This condition makes the circuit stable.

The poles on the 𝑗𝜔 axis must be simple poles.

𝑍 𝑠 or 𝑌 𝑠 must not have multiple zeros or poles at the

origin.

Network Synthesis

25

Realizability Conditions

Dr. Mohamed Refky

Page 26: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

2) For the function

𝑍 𝑠 or 𝑌 𝑠

The power of the numerator and denominator in 𝑠 must differ at

most by ±1.

This is because the function must be reduced to one of the

elements

Network Synthesis

26

Realizability Conditions

Dr. Mohamed Refky

=𝜙 𝑠

𝜓 𝑠=𝛼𝑚𝑠

𝑚 + 𝛼𝑚−1𝑠𝑚−1 +⋯+ 𝛼0

𝛽𝑛𝑠𝑛 + 𝛽𝑛−1𝑠

𝑛−1 +⋯+ 𝛽0

𝑅, 𝑠𝐿,1

𝑠𝐶𝐺,

1

𝑠𝐿, 𝑠𝐶or

Page 27: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

In first foster form, partial fraction is used to factorized 𝑍 𝑠

Network Synthesis

27

First Foster Form

Dr. Mohamed Refky

𝑍 𝑠 =𝑘1

𝑎1𝑠 + 𝑏1+

𝑘2𝑎2𝑠 + 𝑏2

𝑍 𝑠 =𝛼1𝑠 + 𝛼0

𝛽2𝑠2 + 𝛽2𝑠 + 𝛽0

Page 28: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Use the first foster form to synthesize the function

𝑍 𝑠 =𝑠2 + 4𝑠 + 3

𝑠2 + 2𝑠

Network Synthesis

28

Example (1)

Dr. Mohamed Refky

Page 29: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

In second foster form, partial fraction is used to factorized 𝑌 𝑠

Network Synthesis

29

Second Foster Form

Dr. Mohamed Refky

𝑌 𝑠 =𝑘1

𝑎1𝑠 + 𝑏1+

𝑘2𝑎2𝑠 + 𝑏2

𝑌 𝑠 =𝛼1𝑠 + 𝛼0

𝛽2𝑠2 + 𝛽2𝑠 + 𝛽0

Page 30: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Use the second foster form to synthesize the function

𝑌 𝑠 =4𝑠4 + 7𝑠2 + 1

𝑠 2𝑠2 + 3

Network Synthesis

30

Example (2)

Dr. Mohamed Refky

𝑌 𝑠 =4𝑠4 + 7𝑠2 + 1

2𝑠3 + 3𝑠

= 2𝑠 +𝑠2 + 1

𝑠 2𝑠2 + 3

Page 31: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

First Cauer Form of 𝑍 𝑠 starts with

𝑍 𝑠 =𝛼𝑚𝑠

𝑚 + 𝛼𝑚−1𝑠𝑚−1 +⋯+ 𝛼0

𝛽𝑛𝑠𝑛 + 𝛽𝑛−1𝑠

𝑛−1 +⋯+ 𝛽0

then Continued Fraction Expansion (CFE) is applied to 𝑍 𝑠 to

put it in the form

Network Synthesis

31

Cauer Form (Continued Fraction

Expansion)

Dr. Mohamed Refky

𝑍 𝑠 = 𝑍1 𝑠 +1

𝑌2 𝑠 +1

𝑍3 𝑠 +1

𝑌4 𝑠 +1

𝑍5 𝑠 + ⋯

Page 32: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Realize the following function in the first Cauer form

𝑍 𝑠 =𝑠4 + 4𝑠2 + 3

𝑠3 + 2𝑠

Network Synthesis

32

Example (3)

Dr. Mohamed Refky

Page 33: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

First Cauer Form of 𝑌 𝑠 starts with

𝑌 𝑠 =𝛽𝑛𝑠

𝑛 + 𝛽𝑛−1𝑠𝑛−1 +⋯+ 𝛽0

𝛼𝑚𝑠𝑚 + 𝛼𝑚−1𝑠

𝑚−1 +⋯+ 𝛼0

then Continued Fraction Expansion (CFE) is applied to 𝑌 𝑠 to

put it in the form

Network Synthesis

33

Cauer Form (Continued Fraction

Expansion)

Dr. Mohamed Refky

𝑌 𝑠 = 𝑌1 𝑠 +1

𝑍2 𝑠 +1

𝑌3 𝑠 +1

𝑍4 𝑠 +1

𝑌5 𝑠 + ⋯

Page 34: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Realize the following admittance function in the first Cauer Form

𝑌 𝑠 =𝑠2 + 4𝑠 + 3

𝑠2 + 2𝑠

Network Synthesis

34

Example (4)

Dr. Mohamed Refky

Page 35: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Secound Cauer Form of 𝑍 𝑠 starts with

𝑍 𝑠 =𝛼0 +⋯+ 𝛼𝑚−1𝑠

𝑚−1 + 𝛼𝑚𝑠𝑚

𝛽0 +⋯+ 𝛽𝑛−1𝑠𝑛−1 + 𝛽𝑛𝑠

𝑛

then Continued Fraction Expansion (CFE) is applied to 𝑍 𝑠 to

put it in the form

Network Synthesis

35

Cauer Form (Continued Fraction

Expansion)

Dr. Mohamed Refky

𝑍 𝑠 = 𝑍1 𝑠 +1

𝑌2 𝑠 +1

𝑍3 𝑠 +1

𝑌4 𝑠 +1

𝑍5 𝑠 + ⋯

Page 36: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Realize the following admittance function in the second Cauer

Form

𝑍 𝑠 =𝑠4 + 4𝑠2 + 3

𝑠3 + 2𝑠

Network Synthesis

36

Example (5)

Dr. Mohamed Refky

Page 37: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Secound Cauer Form of 𝑌 𝑠 starts with

𝑌 𝑠 =𝛽0 +⋯+ 𝛽𝑛−1𝑠

𝑛−1 + 𝛽𝑛𝑠𝑛

𝛼0 +⋯+ 𝛼𝑚−1𝑠𝑚−1 + 𝛼𝑚𝑠

𝑚

then Continued Fraction Expansion (CFE) is applied to 𝑌 𝑠 to

put it in the form

Network Synthesis

37

Cauer Form (Continued Fraction

Expansion)

Dr. Mohamed Refky

𝑌 𝑠 = 𝑌1 𝑠 +1

𝑍2 𝑠 +1

𝑌3 𝑠 +1

𝑍4 𝑠 +1

𝑌5 𝑠 + ⋯

Page 38: Network Synthesis Part I - Cairo Universityscholar.cu.edu.eg/.../files/lecture_8-_network_synthesis_-_part_i.pdf · Network Synthesis Part I Dr. Mohamed Refky Amin Electronics and

Realize the following admittance function in the second Cauer

Form

𝑌 𝑠 =𝑠2 + 4𝑠 + 3

𝑠2 + 2𝑠

Network Synthesis

38

Example (6)

Dr. Mohamed Refky