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1 CHAPTER 4 Transient & Steady State Response Analysis

1 CHAPTER 4 Transient & Steady State Response Analysis

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Page 1: 1 CHAPTER 4 Transient & Steady State Response Analysis

1

CHAPTER 4

Transient & Steady State Response Analysis

Page 2: 1 CHAPTER 4 Transient & Steady State Response Analysis

2

Previous Class

In Chapter 3: Block diagram reduction Signal flow graphs (SFGs)

Transfer FunctionTransfer Function

Page 3: 1 CHAPTER 4 Transient & Steady State Response Analysis

Today’s class

Chapter 4 – Transient & Steady State Response Analysis First Order System Second Order System

3

Page 4: 1 CHAPTER 4 Transient & Steady State Response Analysis

Learning Outcomes

At the end of this lecture, students should be able to: Identify between transient response &

steady state response Obtain the transfer function for a first

order system based on graph analysis To become familiar with the wide range

of response for second order systems

4

Page 5: 1 CHAPTER 4 Transient & Steady State Response Analysis

5

In Chapter 4

What you are expected to learn :What you are expected to learn :

First order systemFirst order system

Second order systemSecond order system

Routh-Hurwitz CriterionRouth-Hurwitz Criterion

Steady-state errorSteady-state error

Chapter 4

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Introduction

The time response of a control system The time response of a control system consists of two parts:consists of two parts:

1. Transient response

- from initial state to the final

state – purpose of control

systems is to provide a desired

response.

2. Steady-state response

- the manner in which the

system output behaves as t

approaches infinity – the error

after the transient response has

decayed, leaving only the

continuous response.

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Introduction

Transient Steady-state

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Performances of Control Systems

Specifications (time domain) Max OS, settling time, rise time, peak time,

Standard input signals used in design actual signals unknown standard test signals:

step, ramp, parabola, impulse, etc. sinusoid (study freq. response later)

Transient response Steady-state response Relate to locations of poles and zeros

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First Order System

s1R(s) C(s)E(s)

Test signal is step function, R(s)=1/s

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First – order system

1

1

)(

)(

ssR

sC

A first-order system without zeros can be represented by the following transfer function

• Given a step input, i.e., R(s) = 1/s , then the system output (called step response in this case) is

1

11

)1(

1)(

1

1)(

sssssR

ssC

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11

First – order system

t

etc

1)(

Taking inverse Laplace transform, we have the step response

Time Constant: If t= , So the step response is C( ) = (1− 0.37) = 0.63

is referred to as the time constant of the response. In other words, the time constant is the time it takes for the step response to rise to 63% of its final value. Because of this, the time constant is used to measure how fast a system can respond. The time constant has a unit of seconds.

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First – order system

Plot c(t) versus time:

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The following figure gives the measurements of the step response of a first-order system, find the transfer function of the system.

First – order system

Example 1

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First – order system Transient Response Analysis

Rise Time Tr:

The rise-time (symbol Tr units s) is defined as the time taken for the step response to go from 10% to 90% of the final value.

Settling Time Ts:

Defined the settling-time (symbol Ts units s) to be the time taken for the step response to come to within 2% of the final value of the step response.

2.211.031.2 rT

4sT

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First – order systema

1

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Second – Order System

Second-order systems exhibit a wide range of responses which must be analyzed and described.

• Whereas for a first-order system, varying a single parameter changes the speed of response, changes in the parameters of a second order system can change the form of the response. For example: a second-order system can displaycharacteristics much like a first-order system or, depending on component values, display damped or pure oscillations for its transient response.

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Second – Order System

- A general second-order system is characterized by the following transfer function:

- We can re-write the above transfer function in the following form (closed loop transfer function):

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Second – Order System

- referred to as the un-damped natural frequency of the second order system, which is the frequency of oscillation of the system without damping.

- referred to as the damping ratio of the second order system, which is a measure of the degree of resistance to change in the system output.

Poles;Poles are complex if ζ< 1!

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Second – Order System

- According the value of ζ, a second-order system can be set into one of the four categories:

1. Overdamped - when the system has two real distinct poles (ζ >1).2. Underdamped - when the system has two complex conjugate poles (0 <ζ <1)3. Undamped - when the system has two imaginary poles (ζ = 0). 4. Critically damped - when the system has two real but equal poles (ζ = 1).

Page 20: 1 CHAPTER 4 Transient & Steady State Response Analysis

Time-Domain Specification

20

22

2

2)(

)()(

nn

n

sssR

sCsT

Given that the closed loop TF

The system (2nd order system) is parameterized by ς and ωn

For 0< ς <1 and ωn > 0, we like to investigate its response due to a unit step input

Transient Steady State

Two types of responses that are of interest:(A)Transient response(B)Steady state response

Page 21: 1 CHAPTER 4 Transient & Steady State Response Analysis

(A) For transient response, we have 4 specifications:

21

(a) Tr – rise time =

(b) Tp – peak time =

(c) %MP – percentage maximum overshoot =

(d) Ts – settling time (2% error) =

21

n

21 n

%10021 xe

n4

(B) Steady State Response(a) Steady State error

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Question : How are the performance related to ς and ωn ?

- Given a step input, i.e., R(s) =1/s, then the system output (or step response) is;

- Taking inverse Laplace transform, we have the step response;

Where; or )(cos 1

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Second – Order System

Mapping the poles into s-plane

22

2

2)(

)()(

nn

n

sssR

sCsT

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Lets re-write the equation for c(t):

Let: 21

21 nd

and

Damped natural frequency

dn

Thus:

tetc dtn sin

11)(

)(cos 1 where

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Transient Response Analysis

1) Rise time, Tr. Time the response takes to rise from 0 to 100%

21

n

rT

1sin1

1)(

tetc dt

rTtn

0 0

)0(sin

0)sin(1

rd

rd

T

T

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Transient Response Analysis

2) Peak time, Tp - The peak time is the time required for the response to reach the first peak, which is given by;

0)(

pTt

tc

01)cos()sin()(1

)( 21

nd

td

tn

pTt

tetetc nn

)cos()sin(21

pdT

pdTn TeTe pn

npn

21)tan( pdT

1

tan

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We know that )tan()tan(

So, )tan()tan( pdT

From this expression:

pd

pd

T

T

21

ndpT

Page 28: 1 CHAPTER 4 Transient & Steady State Response Analysis

3) Percent overshoot, %OS - The percent overshoot is defined as the amount that the waveform at the peak time overshoots the steady-state value, which is expressed as a percentage of the steady-state value.

Transient Response Analysis

%100)(

)()(% x

C

CTCMP p

100max

% xCfinal

CfinalCOS

OR

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2929

%100%100)sin(

%100sin1

%100sin1

22

2

2

11

1

1

xexe

xe

xed

dn

n

%100sin1

%1001

1)(xtex

TCd

tp n

21sin

21

From slide 24

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- For given %OS, the damping ratio can be solved from the above equation;

Therefore, %100%

21 xeMP

100/%ln

100/%ln22 MP

MP

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Transient Response Analysis

4) Setting time, Ts - The settling time is the time required for the amplitude of the sinusoid to decay to 2% of the steady-state value.

To find Ts, we must find the time for which c(t) reaches & stays within +2% of the steady state value, cfinal. The settling time is the time it takes for the amplitude of the decaying sinusoid in c(t) to reach 0.02, or

02.01

12

snTe

Thus,

nsT

4

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32

UNDERDAMPED

Example 2: Find the natural frequencynatural frequency and damping damping ratioratio for the system with transfer function

Solution: 362.4

36)(

2

sssG

Compare with general TF

•ωn= 6

•ξ =0.35

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Example 3Example 3:: Given the transfer function

UNDERDAMPED

sTOSsT ps 475.0%,838.2%,533.0

ps TOSTfind ,%,

Solution:

75.010 n

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UNDERDAMPED

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a = 9

s= 0; s = -7.854; s = -1.146 s= 0; s = -7.854; s = -1.146 ( two real poles)( two real poles)

)146.1)(854.7(

9

)99(

9)(

2

sssssssC

1

Overdamped ResponseOverdamped Response

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tt eKeKKtc 146.13

854.721)(

OVERDAMPEDOVERDAMPED RESPONSE !!!RESPONSE !!!

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Underdamped ResponseUnderdamped Response

)598.2sin598.2cos()( 325.1

1 tKtKeKtc t

s = 0; s = -1.5 ± j2.598 s = 0; s = -1.5 ± j2.598 ( two complex poles)( two complex poles)

a = 3

10

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UNDERDAMPEDUNDERDAMPED RESPONSE !!!RESPONSE !!!

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Undamped ResponseUndamped Response

a = 0

tKKtc 3cos)( 21 s = 0; s = ± j3 s = 0; s = ± j3 ( two imaginary poles)( two imaginary poles)

0

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UNDAMPEDUNDAMPED RESPONSE !!!RESPONSE !!!

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a = 6

Critically Damped SystemCritically Damped System

tt teKeKKtc 33

321)(

S = 0; s = -3,-3 S = 0; s = -3,-3 ( two real and equal poles)( two real and equal poles)

1

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CRITICALLY DAMPEDCRITICALLY DAMPED RESPONSE !!!RESPONSE !!!

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Second – Order System

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Effect of different damping ratio, ξ

Increasing ξ

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Example 4: Describe the nature of the second-order system response via the value of the damping ratio for the systems with transfer function

Second – Order System

128

12)(.1

2

sssG

168

16)(.2

2

sssG

208

20)(.3

2

sssG

Do them as your Do them as your own revisionown revision