CONTROL SYSTEM UNIT - 6 UNIT - 6 Datta Meghe Institute of engineering Technology and Research Sawangi (meghe),Wardha 1 DEPARTMENT OF ELECTRONICS & TELECOMMUNICATION.

Slides:



Advertisements
Similar presentations
Lect.3 Modeling in The Time Domain Basil Hamed
Advertisements

FIRST AND SECOND-ORDER TRANSIENT CIRCUITS
Applications of Laplace Transforms Instructor: Chia-Ming Tsai Electronics Engineering National Chiao Tung University Hsinchu, Taiwan, R.O.C.
LectR2EEE 2021 Exam #2 Review Dr. Holbert March 26, 2008.
Lect15EEE 2021 Systems Concepts Dr. Holbert March 19, 2008.
The Laplace Transform in Circuit Analysis
Lecture 181 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
1 Adjoint Method in Network Analysis Dr. Janusz A. Starzyk.
Leo Lam © Signals and Systems EE235 Lecture 31.
5.7 Impulse Functions In some applications, it is necessary to deal with phenomena of an impulsive nature—for example, voltages or forces of large magnitude.
Chapter 10 Sinusoidal Steady-State Analysis
ES250: Electrical Science
APPLICATION OF THE LAPLACE TRANSFORM
FIRST ORDER TRANSIENT CIRCUITS
EENG 2610: Circuit Analysis Class 12: First-Order Circuits
Sinusoidal Steady-state Analysis Complex number reviews Phasors and ordinary differential equations Complete response and sinusoidal steady-state response.
Complex Waveforms as Input Lecture 19 1 When complex waveforms are used as inputs to the circuit (for example, as a voltage source), then we (1) must Laplace.
THE LAPLACE TRANSFORM IN CIRCUIT ANALYSIS. A Resistor in the s Domain R + v i v=Ri (Ohm’s Law). V(s)=RI(s R + V I.
Chapter 16 Applications of the Laplace Transform
The Laplace Transform in Circuit Analysis
AC STEADY-STATE ANALYSIS SINUSOIDAL AND COMPLEX FORCING FUNCTIONS Behavior of circuits with sinusoidal independent sources and modeling of sinusoids in.
EE212 Passive AC Circuits Lecture Notes 2a EE 212.
Sinusoidal Steady-State Analysis Instructor: Chia-Ming Tsai Electronics Engineering National Chiao Tung University Hsinchu, Taiwan, R.O.C.
CHAPTER 4 Laplace Transform.
CHAPTER 4 Laplace Transform.
CIRCUIT ANALYSIS USING LAPLACE TRANSFORM
Depok, October, 2009 Laplace Transform Electric Circuit Circuit Applications of Laplace Transform Electric Power & Energy Studies (EPES) Department of.
Mathematical Models and Block Diagrams of Systems Regulation And Control Engineering.
Dynamic Presentation of Key Concepts Module 8 – Part 2 AC Circuits – Phasor Analysis Filename: DPKC_Mod08_Part02.ppt.
Fundamentals of Electric Circuits Chapter 16 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Capacitors in a circuit 1. Example Let’s find the current through the following capacitor with v(t)=5 cos(2000  t)V. C = 30  F What if v(t) = 5A? =
Motivation Thus far we have dealt primarily with the input/output characteristics of linear systems. State variable, or state space, representations describe.
APPLICATION OF THE LAPLACE TRANSFORM
10. Laplace TransforM Technique
1 Alexander-Sadiku Fundamentals of Electric Circuits Chapter 16 Applications of the Laplace Transform Copyright © The McGraw-Hill Companies, Inc. Permission.
Circuit Theorems ELEC 202 Electric Circuit Analysis II.
Chapter 7 The Laplace Transform
ECE Networks & Systems Jose E. Schutt-Aine
1 ECE 3144 Lecture 32 Dr. Rose Q. Hu Electrical and Computer Engineering Department Mississippi State University.
Alexander-Sadiku Fundamentals of Electric Circuits
Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1.
Dr. Tamer Samy Gaafar Lec. 2 Transfer Functions & Block Diagrams.
1 Lecture #18 EGR 272 – Circuit Theory II Transfer Functions (Network Functions) A transfer function, H(s), can be used to describe a system or circuit.
1 Eeng 224 Chapter 10 Sinusoidal Steady State Analysis Huseyin Bilgekul Eeng224 Circuit Theory II Department of Electrical and Electronic Engineering Eastern.
Chapter 9 Sinusoids and Phasors
CSE 245: Computer Aided Circuit Simulation and Verification Instructor: Prof. Chung-Kuan Cheng Winter 2003 Lecture 2: Closed Form Solutions (Linear System)
ELECTRIC CIRCUITS EIGHTH EDITION
ELECTRIC CIRCUITS EIGHTH EDITION JAMES W. NILSSON & SUSAN A. RIEDEL.
Chapter 9 Sinusoids and Phasors
Mathematical Models of Control Systems
EE4262: Digital and Non-Linear Control
Laplace Transforms Chapter 3 Standard notation in dynamics and control
DEPT.:-ELECTRONICS AND COMMUNICATION SUB: - CIRCUIT & NETWORK
Chapter 16 Applications of the Laplace Transform
Network Analysis and Synthesis
Automatic Control Theory CSE 322
Feedback Control Systems (FCS)
Application of the Laplace Transform
Chapter 2 Interconnect Analysis
Fundamentals of Electric Circuits Chapter 16
FIRST AND SECOND-ORDER TRANSIENT CIRCUITS
Mechatronics Engineering
Signals and Systems EE235 Lecture 31 Leo Lam ©
Fundamentals of Electric Circuits Chapter 15
Control Systems (CS) Lecture-3 Introduction to Mathematical Modeling &
3/16/2015 Hafiz Zaheer Hussain.
Mathematical Models of Control Systems
Control Systems Spring 2016
Transfer Function and Stability of LTI Systems
CHAPTER 4 Laplace Transform. EMT Signal Analysis.
Presentation transcript:

CONTROL SYSTEM UNIT - 6 UNIT - 6 Datta Meghe Institute of engineering Technology and Research Sawangi (meghe),Wardha 1 DEPARTMENT OF ELECTRONICS & TELECOMMUNICATION ENGINEERING

Department of Electronics & Telecommunication Engineering VI SEM CONTROL SYSTEM UNIT- VI STATE VARIABLE METHOD 2

Introduction To learn how easy it is to work with circuits in the s domain To learn the concept of modeling circuits in the s domain To learn the concept of transfer function in the s domain To learn how to apply the state variable method for analyzing linear systems with multiple inputs and multiple outputs To learn how the Laplace transform can be used in stability analysis D.M.I.E.T.R.3

Circuit Element Models Steps in applying the Laplace transform: –Transform the circuit from the time domain to the s domain (a new step to be discussed later) –Solve the circuit using circuit analysis technique (nodal/mesh analysis, source transformation, etc.) –Take the inverse Laplace transform of the solution and thus obtain the solution in the time domain 4

s-Domain Models for R and L Time domain s domain 5

s-Domain Model for C Time domains domain 6

Summary For inductor:For capacitor: 7

Summary ElementZ(s)Z(s) ResistorR InductorsL Capacitor1/sC *Assuming zero initial conditions Impedance in the s domain – Z(s)=V(s)/I(s) Admittance in the s domain – Y(s)=1/Z(s)=V(s)/I(s) 8

Example 1 9

Example 2 10

Example 2 (Cont’d) 11

Example 3 12

Circuit Analysis Operators (derivatives and integrals) into simple multipliers of s and 1/s Use algebra to solve the circuit equations All of the circuit theorems and relationships developed for dc circuits are perfectly valid in the s domain 13

Example 1 14

Example 2 15

Example 3 Assume that no initial energy is stored. (a)Find V o (s) using Thevenin’s theorem. (b)Find v o (0 + ) and v o (  ) by apply the initial- and final-value theorems. (c) Determine v o (t). =10u(t) 16

Example 3: (a) 17

Example 3: (b), (c) 18

Transfer Functions The transfer function H(s) is the ratio of the output response Y(s) to the input excitation X(s), assuming all initial conditions are zero. 19

Transfer Functions (Cont’d) Two ways to find H(s) –Assume an input and find the output –Assume an output and find the input (the ladder method: Ohm’s law + KCL) Four kinds of transfer functions 20

Example 1 21

Example 2 Find H(s)=V 0 (s)/I 0 (s). 22

Example 2 (The Ladder Method) 23

Example 3 Find (a) H(s) = V o /V i, (b) the impulse response, (c) the response when v i (t) = u(t) V, (d) the response when v i (t) = 8cos2t V. 24

Example 3: (a), (b) 25

Example 3: (c), (d) 26

State Variables The state variables are those variables which, if known, allow all other system parameters to be determined by using only algebraic equations. In an electric circuit, the state variables are the inductor current and the capacitor voltage since they collectively describe the energy state of the system. 27

State Variable Method 28

State Variable Method (Cont’d) 29

How to Apply State Variable Method Steps to apply the state variable method to circuit analysis: –Select the inductor current i and capacitor voltage v as the state variables (define vector x, z) –Apply KCL and KVL to obtain a set of first-order differential equations (find matrix A, B) –Obtain the output equation and put the final result in state-space representaion (find matrix C) –H(s)=C(sI-A) -1 B 30

Network Stability A circuit is stable if its impulse response h(t) is bounded as t approaches  ; it is unstable if h(t) grows without bound as t approaches . Two requirements for stability –Degree of N(s) < Degree of D(s) –All the poles must lie in the left half of the s plane 31

Network Stability (Cont’d) A circuit is stable when all the poles of its transfer function H(s) lie in the left half of the s plane. Circuits composed of passive elements (R, L, and C) and independent sources either are stable or have poles with zero real parts. Active circuits or passive circuits with controlled sources can supply energy, and can be unstable. 32

Example 1 33

Example 2 Find k for a stable circuit. 34

Summary The methodology of circuit analysis using Laplace transform –Convert each element to its s-domain model –Obtain the s-domin solution –Apply the inverse Laplace transform to obtain the t-domain solution 35

Summary The transfer function H(s) of a network is the Laplace transform of the impulse response h(t) A circuit is stable when all the poles of its transfer function H(s) lie in the left half of the s plane. 36