Network Analysis and Synthesis

Slides:



Advertisements
Similar presentations
Chapter 3 Matching and Tuning
Advertisements

Solving Differential Equations BIOE Solving Differential Equations Ex. Shock absorber with rigid massless tire Start with no input r(t)=0, assume.
Synthesis of one-port networks with two kinds of elements
ELCT564 Spring /13/20151ELCT564 Chapter 5: Impedance Matching and Tuning.
Lecture 6. Chapter 3 Microwave Network Analysis 3.1 Impedance and Equivalent Voltages and Currents 3.2 Impedance and Admittance Matrices 3.3 The Scattering.
Chapter 8 Root Locus <<<4.1>>>
Fundamentals of Power Electronics 1 Chapter 19: Resonant Conversion 19.4 Load-dependent properties of resonant converters Resonant inverter design objectives:
ELEC 412Lecture 51 ELEC 412 RF & Microwave Engineering Fall 2004 Lecture 5.
V–2 AC Circuits Main Topics Power in AC Circuits. R, L and C in AC Circuits. Impedance. Description using Phasors. Generalized.
Network Analysis and Synthesis
EKT 441 MICROWAVE COMMUNICATIONS
Network Analysis and Synthesis
Instructor: Engr. Zuneera Aziz Course: Microwave Engineering
VARIABLE-FREQUENCY NETWORK
Frequency Characteristics of AC Circuits
Introduction to Frequency Selective Circuits
Alternating-Current Circuits Chapter 22. Section 22.2 AC Circuit Notation.
IMPEDANCE Matching.
Chapter 5: Impedance Matching and Tuning
VARIABLE-FREQUENCY NETWORK
Sinusoidal Steady-state Analysis Complex number reviews Phasors and ordinary differential equations Complete response and sinusoidal steady-state response.
Lecture 8 Periodic Structures Image Parameter Method
5. Impedance Matching and Tuning
EMLAB 1 Chapter 5. Additional analysis techniques.
TELECOMMUNICATIONS Dr. Hugh Blanton ENTC 4307/ENTC 5307.
IMPEDANCE MATCHING IN HIGH FREQUENCY LINES UNIT - III.
Chapter 7 AC Power Analysis
Anuroop Gaddam. An ideal voltage source plots a vertical line on the VI characteristic as shown for the ideal 6.0 V source. Actual voltage sources include.
Partial-fraction Expansion
1 Inverse Laplace Transform Note that most of the transforms are written as fractions.
Lesson 3.4 – Zeros of Polynomial Functions Rational Zero Theorem
ME375 Handouts - Spring 2002 Root Locus Method.
Biomedical Control Systems (BCS) Module Leader: Dr Muhammad Arif muhammadarif Batch: 10 BM Year: 3 rd Term: 2 nd Credit Hours (Theory):
Chapter 2 Laplace Transform 2.1 Introduction The Laplace transform method can be used for solving linear differential equations. Laplace transforms can.
116/11/50 ENE 490 Applied Communication Systems Lecture 2 circuit matching on Smith chart.
Yi HUANG Department of Electrical Engineering & Electronics
Synthesis of R-L-C Networks EE484 – presentation Janghoon, Cho.
Network Analysis and Synthesis
Apply KCL to the top node ,we have We normalize the highest derivative by dividing by C , we get Since the highest derivative in the equation is.
Chapter 7 The Laplace Transform
19.4 Load-dependent properties of resonant converters
EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 3: MICROWAVE NETWORK ANALYSIS (PART II)
ENE 490 Applied Communication Systems
Variable-Frequency Response Analysis Network performance as function of frequency. Transfer function Sinusoidal Frequency Analysis Bode plots to display.
Chapter 19 Principles of Electric Circuits, Conventional Flow, 9 th ed. Floyd © 2010 Pearson Higher Education, Upper Saddle River, NJ All Rights.
Thevenin Theorem in Sinusoidal Steady Analysis Aim: To obtain a simple equivalent circuit for a 1-port circuit that consists of linear, time-invariant.
1 ECE 3301 General Electrical Engineering Section 19 Maximum Power Transfer Theorem.
Variable-Frequency Response Analysis Network performance as function of frequency. Transfer function Sinusoidal Frequency Analysis Bode plots to display.
Initial Conditions & Passive Network Synthesis. Sarvajanik College of Engineering & Technology Made by: Dhruvita Shah Khushbu Shah
Network Theorems (AC). OBJECTIVES Be able to apply the superposition theorem to ac networks with independent and dependent sources. Become proficient.
Lesson 10: Thevenin’s Theorem and Max Power Transfer
Salman Bin Abdulaziz University
Lec 4. the inverse Laplace Transform
Sinusoidal Excitation of Circuits
CHAPTER 5 Z-Transform. EKT 230.
Chapter 5 Root Locus.
Network Analysis and Synthesis
Automatic Control Theory CSE 322
topics Basic Transmission Line Equations
Fundamentals of Electric Circuits Chapter 14
What is a filter Passive filters Some common filters Lecture 23. Filters I 1.
ENE 428 Microwave Engineering
The Theorems we will look at are:
Network Analysis and Synthesis
Signals and Systems Lecture 3
Chapter 4. Time Response I may not have gone where I intended to go, but I think I have ended up where I needed to be. Pusan National University Intelligent.
Mathematical Models of Control Systems
Apply KCL to the top node ,we have We normalize the highest derivative by dividing by C , we get Since the highest derivative in the equation is.
Chapter 8.1 Chapter 8.2 PERIODIC STRUCTURES
4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

Network Analysis and Synthesis Chapter 6 Synthesis of two port networks

5.1 Introduction In this chapter we will discuss 2 of the most widely used two port synthesis methods Coefficient matching and Darlington method (insertion loss method)

5.2 Coefficient matching It is one of the most simple and effective method for two port synthesis. In this method, We compare the transfer function we want to synthesize with the transfer function of a circuit we already know. If they have the same form, we try to match the coefficients of the two functions. (Remember that the coefficients of the second transfer function is a function of the circuit elements.) Once we match the coefficients, we know the values of the elements in the circuit.

Example 1 The voltage transfer function of the following circuit is R1-source impedance R2-load impedance

If we are required to synthesize the following voltage transfer function. Comparing the two equations and assuming equal termination and normalizing the resistors to 1Ω, R1=R2=1Ω

Example 2 Consider the following network The voltage transfer function is

If we were to synthesize the following voltage transfer function assuming equal termination with 1Ω resistor.

Pros and Cons of Coefficient matching Simple Effective Cons When the order of the transfer function increases, the number of simultaneous equations we have to solve for increases. Doesn’t demonstrate sophisticated network design methods.

5.3 Insertion Loss (Darlington Method) A low pass characteristics can be obtained by using RC, RL or LC networks. Low cost, low sensitivity to component variations and simplicity of design make LC two port networks the most widely used filter networks. Here the network is assumed to be doubly terminated. (A valid assumption in almost all cases.)

A powerful method for designing doubly terminated LC two port networks is the Darlington method. It is one of the most effective method of realizing a two port network: Insertion loss method (Darlington method).

In Darlington method of filter design, The specifications of the insertion loss of the filter is converted to the reflection coefficients (related to the maximum power that can be delivered by the source vs. the actual delivered power to the load) of the filter. From the reflection coefficients the driving point impedance of the terminated networks is obtained. Then this driving-point impedance is developed into resistively terminated LC ladder network.

Procedures of Darlington synthesis The derivation of Darlington method is complicated, hence, we will just discuss the procedure for using the Darlington method. Procedure From F(s) obtain the reflection coefficient p(s)

From ρ(s) determine the normalized Z(s). The zeros of q1(s) are the left plane zeroes of q(s). The zeros of p(s) are equally distributed between the zeros of ρ (s) and ρ (-s), with restrictions that conjugate zeros must be together. From ρ(s) determine the normalized Z(s). Expand Z(s) into continued fraction expansion about infinity and obtain the ladder. The two impedances defined above lead to 2 (dual) ladders, one terminated with R2 and the other 1/R2.

Example 3 Synthesize the following voltage transfer function using Insertion loss method Solution: To find the reflection coefficient The zeros of q(s) are z1=1, z2=-1, z3=-0.5+j0.866, z4=-0.5-j0.866, z5=0.5+j0.866, z6=0.5-j0.866 Hence, poles of ρ(s) are z2=-1, z3=-0.5+j0.866, z4=-0.5-j0.866

The zeros of p(s) are 6 multiple poles at s=0. Hence, the zeros of ρ(s) are 3 multiple poles at s=0. Hence The driving point impedance is

Using continued fraction expansion

Example 4 Synthesize the following voltage transfer function using Insertion loss method with R1=R2=1Ω Solution: To find the reflection coefficient The zeros of p(s) are 8 multiple poles at s=0, hence the zeros of ρ(s) are 4 multiple poles at s=0.

The angle between the two zeros is (Refer at the end for a more detailed explanation on how to get roots of polynomials of the form sn+a) The zeros of q(s) are evenly distributed on the unit circle on the s plane. The angle between the two zeros is Since no zero on real axis or jw plane and because the zeros of q(s) have to be conjugate complex, the angle of one of the roots from the real axis should be equal for two conjugate roots.

The zeros of q(s) are then The roots of ρ(s) are the left hand zeros of q(s)

ρ(s) becomes The driving point impedance becomes:

Taking the continuous fraction expansion Hence, the network becomes

Finding roots of polynomials of the form sn+a The roots will be located on the circle with radius of a1/n on the s plane. Separation between them is Check if the polynomial has root at s=a1/n or s=-a1/n or s=ja1/n or s=-ja1/n. Case 1: root at one of these Start at that root and plot the roots with separation of θ.

Case 2: no root at those locations Because the roots have to be conjugate complex, the angle one of the roots makes with the real axis will be equal to the negative angle of the conjugate root. Hence, one of them will be Start from this root and plot the rest with separation angle of θ.

Example What are the roots of s8+1 Separation between the roots is Root on one of the axis? No Hence one of the root is Plot the rest starting from this one.

Example s6-1 The separation angle is Root at one of the axis? Yes at r1=1. Hence, plot the rest with separation of 600 starting from r1=1. The roots are then