Top Banner
ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE SOLUTION BUT FINDS THE CONSTANTS USING BASIC CIRCUIT ANALYSIS TOOLS AND FORGOES THE DETERMINATION OF THE DIFFERENTIAL EQUATION MODEL , , 2 1 K K 0 , ) ( 2 1 t e K K t x t stat steady in circuit the analyzing determined be can and variable the of value state steady the is 1 K 2 1 , ) 0 ( K K x constants the compute to equation second the provides and condition initial the is element storing energy the across Thevenin using determined be can and constant time the is
26

ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

Dec 17, 2015

Download

Documents

Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENTCONSTANT INDEPENDENT SOURCES

A STEP-BY-STEP APPROACH

THIS APPROACH RELIES ON THE KNOWN FORM OF THE SOLUTIONBUT FINDS THE CONSTANTS USING BASIC CIRCUIT ANALYSIS TOOLS AND FORGOES THE DETERMINATION OF THE DIFFERENTIAL EQUATION MODEL

,, 21 KK

0,)( 21 teKKtx

t

statesteady incircuit the analyzing determined be

can and variablethe of valuestatesteady the is 1K

21,

)0(

KK

x

constants the compute to equation

second the provides and condition initial the is

element storingenergy the across Thevenin using

determined be can andconstant time the is

Page 2: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

Obtaining the time constant: A General Approach

Circuitw ith

resistancesand

sources

I nductororCapacitor

a

b

R epresentation of an arbitrarycircuit w ith one storage elem ent

TheveninVTH

R TH

I nductororCapacitor

a

b

VTH

R TH a

b

C

+

vc

_

Case 1.1Voltage across capacitor

VTH

R TH a

b

L

iL

Case 1.2Current through inductor

KCL@ node a

ciRi0 Rc ii

dt

dvCi C

c

TH

THCR R

vvi

0

TH

THCC

R

vv

dt

dvC

THCC

TH vvdt

dvCR

Use KVL

Rv

Lv

THLR vvv

LTHR iRv

dt

diLv L

L

THLTHL viRdt

diL

TH

THL

L

TH R

vi

dt

di

R

LSCi

CIRCUITS WITH ONE ENERGY STORING ELEMENT

TH

TH

R

L

CR

Circuit Inductive

Circuit Capacitive

Page 3: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

THE STEPS

)0();(

0,)(

211

21

xKKxK

teKKtxt

STEP 1. THE FORM OF THE SOLUTION

STEP 2: DRAW THE CIRCUIT IN STEADYSTATE PRIOR TO THE SWITCHING ANDDETERMINE CAPACITOR VOLTAGE ORINDUCTOR CURRENT

STEP 3: DRAW THE CIRCUIT AT 0+THE CAPACITOR ACTS AS A VOLTAGESOURCE. THE INDUCTOR ACTS AS ACURRENT SOURCE.DETERMINE THE VARIABLE AT t=0+

STEP 4: DRAW THE CIRCUIT IN STEADYSTATE AFTER THE SWITCHING ANDDETERMINE THE VARIABLE IN STEADYSTATE.

)0( x DETERMINE

)(x DETERMINE

STEP 5: DETERMINE THE TIME CONSTANT

inductor one withcircuit

capacitor one withcircuit

TH

TH

R

L

CR

STEP 6: DETERMINE THE CONSTANTS K1, K2

)0(),( 211 xKKxK

Page 4: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0),( tti FIND

0,)( 21 teKKti

t :1 STEP

USE CIRCUIT IN STEADY STATEPRIOR TO THE SWITCHING

mAk

Vi 212

24

][32)2)(2(36)0( VkmAVvc

)0()0( cC vv

)0( i Determine :3 STEP

USE A CIRCUIT VALID FOR t=0+.THE CAPACITOR ACTS AS SOURCE

mAk

Vi

3

16

6

32)0(

capacitor across voltageInitial :2 STEP

NOTES FOR INDUCTIVE CIRCUIT(1)DETERMINE INITIAL INDUCTOR CURRENT IN STEP 2(2)FOR THE t=0+ CIRCUIT REPLACE INDUCTOR BY A CURRENT SOURCE

LEARNING EXAMPLE

)0( i

KVL

Page 5: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

constant time Determine :5 STEPCRTH :circuit Capacitive

kkkRTH 5.16||2 FC 100

sF 15.0)10100)(105.1( 63

21,KK Determine :6 STEP

0,)( 21 teKKti

t 1) (STEP

mAi3

16)0(( 3) STEP 21 KK

mAi8

36)( 4) (STEP 1K

)(i Determine :4 STEP

USE CIRCUIT IN STEADY STATEAFTER SWITCHING

mAi8

36)( 0,

6

5

8

36)( 15.0

teti

t

WERFINAL ANS

NOTE: FOR INDUCTIVE CIRCUIT

THR

L

ORIGINAL CIRCUIT

6

5

8

36

3

162 K

Page 6: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

USING MATLAB TO DISPLAY FINAL ANSWER

0,6

5

8

36

02)(

15.0 te

tmAti t » help linspace

LINSPACE Linearly spaced vector. LINSPACE(x1, x2) generates a row vector of 100 linearly equally spaced points between x1 and x2. LINSPACE(x1, x2, N) generates N points between x1 and x2. See also LOGSPACE, :.

%example6p3.m%commands used to display funtion i(t)%this is an example of MATLAB script or M-file%must be stored in a text file with extension ".m”%the commands are executed when the name of the M-file is typed at the%MATLAB prompt (without the extension)tau=0.15; %define time constanttini=-4*tau; %select left starting pointtend=10*tau; %define right end pointtminus=linspace(tini,0,100); %use 100 points for t<=0tplus=linspace(0,tend, 250); % and 250 for t>=0iminus=2*ones(size(tminus)); %define i for t<=0iplus=36/8+5/6*exp(-tplus/tau); %define i for t>=0plot(tminus,iminus,'ro',tplus,iplus,'bd'), grid; %basic plot command specifying %color and markertitle('VARIATION OF CURRENT i(t)'), xlabel('time(s)'), ylabel('i(t)(mA)')legend('prior to switching', 'after switching')axis([-0.5,1.5,1.5,6]);%define scales for axis [xmin,xmax,ymin,ymax]

Command used to define linearly spaced arrays

Script (m-file) with commands used. Prepared with the MATLAB Editor

Page 7: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.
Page 8: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0),( ttv FIND

0,)( 21 teKKtv

t :1 STEP

currentinductor Initial :2 STEP

Use circuit in steady stateprior to switching

kk 3||6

mAI 46

241 136

6)0( IiL

mAiL 3

8)0(

)0( v Determine :3 STEP

Use circuit at t=0+.Inductor is replaced bycurrent source

1V

03

8

1264

24 111 VVV ][

3

201 VV

][3

52][24)0( 1 VVVv

LEARNING EXAMPLE

Page 9: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

)(v DETERMINE :4 STEP

USE CIRCUIT IN STEADY STATEAFTER SWITCHING

][24)( Vv

CONSTANT TIME DETERMINE :5 STEP

12||6||4THR

2THR

THR

L :Circuit Inductive

sH

22

4

21,KK DETERMINE :6 STEP4) (step ][24)(1 VvK

3) (step 213

52)0( KKv

][3

2024

3

521 VK

0,243

20)( 2

tetv

t

:ANS

ORIGINAL CIRCUIT

Page 10: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0),( ttvO FIND

0,)( 21 teKKtv

t

o :1 STEP

VOLTAGECAPACITORINITIAL :2 STEP

)0(Cv

0t

1v 2v

2

12

12)0(

)12(3

1

vv

vv

C

V12

022

8

3

12: 1111

vvvv @KCL 6/*

][60488 11 Vvv ][10)0()0(][22 VvvVv CC

)0( Ov DETERMINE :3 STEP

0t

)0(Ov

V10

][5)10(22

2)0( VvO

LEARNING EXTENSION

Page 11: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

)(Ov DETERMINE :4 STEP

)(Ov

][5

24)12(

5

2)( VvO

CONSTANT TIME DETERMINE :5 STEPCRTH :Circuit Capacitive

THR5

44||1THR

sFC5

82

21,KK DETERMINE :6 STEP

][5

24)(1 VvK O

][5

1][5)0( 221 VKKKVvO

0];[5

1

5

24)( 5

8

tVetv

t

O :ANS

ORIGINAL CIRCUIT

Page 12: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0,)( 21 teKKtv

t

O :1 STEP

CURRENT INDUCTORINITIAL :2 STEP

)0( LiOv0

22

)4(

2

12 OOO vvv

][3

4)0()0(

][3

8

Aii

Vv

LL

O

)0( Ov DETERMINE :3 STEP

)0( Li

][3

8)0(2)0( Viv LO

)0( Ov

0),( ttvO FIND

Page 13: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

)(Ov DETERMINE :4 STEP

ORIGINAL CIRCUIT

)(Ov

][6)12(22

2)( VvO

CONSTANT TIME DETERMINE :5 STEP

THR

L

Circuit Inductive

THR

4THR

s5.04

2

21,KK DETERMINE :6 STEP

4) (step ][6)(1 VvK O

3) (step 213

8)( KKvO

][3

106

3

82 VK

0,3

106)( 5.0

tetv

t

O :ANS

Page 14: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0),( ttvO FIND0,)( 21

teKKtv

t

O :1 STEP

)0( Li DETERMINE :2 STEP

AiA 3

][6V

][18V

][3)0()0( Aii LL

)0( Ov DETERMINE :3 STEP

][18)0( VvO

LEARNING EXAMPLE

Page 15: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

)(Ov DETERMINE :4 STEP

ORIGINAL CIRCUIT

Bv

06

)2(

42

36 '

ABBB ivvv

4' BA

vi

12/*

636411 ' AB iv ][5.4],[18 ' AiVv AB

][9V

][27)( VvO

KVL

CONSTANT TIME DETERMINE :5 STEP

THR

L

circuit inductive

SC

OCTH i

vR

sourcesdependent

withCircuit

OPEN CIRCUIT VOLTAGE

AiA 6"

V12

KVL

][361224 VvOC

Page 16: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

NOTE: FOR THE INDUCTIVE CASETHE CIRCUIT USED TOCOMPUTE THE SHORT CIRCUIT CURRENT IS THE SAME USE TODETERMINE )(Ov

SHORT CIRCUIT CURRENT

ORIGINAL CIRCUIT

1i

'''221

121

26)(236

4)(236

Aiiii

iii

'''1

2

A

SC

i i

i i

][8

36AiSC

8][8/36

][36TH

SC

OC RAi

VvsHL8

33

21,KK DETERMINE :6 STEP4) (step 127)( KvO

3) (step ][918)0( 221 VKKKvO

0,927)( 83

tetv

t

O :ANS

Page 17: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

0),( ttvo FIND0,)( 21

teKKtv

t

O :1 STEP

0t AT VOLTAGECAPACITOR DETERMINE :2 STEP

][12VvA

][24V

KVL][60122424)0( VvC

)0(Cv

)0( Ov DETERMINE :3 STEP

)0()0( CC vv

][60)0( Vvvv OCO )(Ov DETERMINE :4 STEP

)(Ov0i

0Av

][24)( VvO

LEARNING EXTENSION

Page 18: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

CONSTANT TIME DETERMINE :5 STEP CRTH circuit capacitive

SC

OCTH i

vR

)(Ov][24)( Vvv OOC

OCv

ORIGINAL CIRCUIT

OPEN CIRCUIT VOLTAGE

SHORT CIRCUIT CURRENT

SCi

2

KVL

02242 ASC vi

SCA iv 2 ][4 AiSC

64

24THR

sF 1226 21,KK DETERMINE :6 STEP

4) (step 24)(1 OvK

3) (step 2160)0( KKvO ][362 VK

0,3624)( 12

tetvt

O :ANS

Page 19: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

Inductor example

STEP 1: Form of the solution

t

OeKKtv

21

)(

STEP 2: Initial inductor current

2

2 4

V6

0t

)0( Li

AiL

3)0(

STEP 3: Determine output at 0+(inductor current is constant)

2

2 4

V6

0t

_

)0(

Ov

A3

VvO

6)0(

2

2 4

V6

0t

H2

Ov

0),( ttvO FIND

Page 20: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

STEP 4: Find output in steadystate after the switching

2

2 4

V6

0t

_

)(

Ov

0)( Ov

2

2 4

H2

V6

0t

_

)(tvO

STEP 5: Find time constant afterswitch

2

2 4

V6

0t

THR

THR

L

8THR

s25.0

STEP 6: Find the solution

VvKKO

6)0(21

0)(

1

OvK

0;6)( 25.0

tetvt

O

0;6)( 4 tetv tO Step by

StepPulse Response

Page 21: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

PULSE RESPONSE

WE STUDY THE RESPONSE OF CIRCUITS TO A SPECIAL CLASS OF SINGULARITYFUNCTIONS

01

00)(

t

ttu VOLTAGE STEP

CURRENT STEP TIME SHIFTED STEP

Page 22: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

PULSE SIGNAL

PULSE AS SUM OF STEPS

))](01.0()([10)( mAtututi

LEARN BY DOING

))](2()1([10)( Vtututv

Page 23: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

NONZERO INITIAL TIME AND REPEATED SWITCHING

dxxfetxetxt

tTH

xttt

)(1

)()(0

0

0

00 )(; xtxfxdt

dxTH

021 ;)(0

tteKKtxtt

RESPONSE FOR CONSTANT SOURCES

This expression will hold on ANY interval where the sources are constant. The values of the constants may be different and must beevaluated for each interval

The values at the end of one interval will serve as initialconditions for the next interval

Page 24: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

LEARNING EXAMPLE 0);( ttvO VOLTAGEOUTPUT THE FIND

0)(0)(0 tvtvt O 0)0( Ov

sFkkCRTH 4.0100)12||6(

Vtvt 9)(0

'1)9(

810

8)( Kvo

t

o eKKtv

'2

'1)(

0)0( '2

`1 KKvo

4.014)(t

o etv

0)(3.0 tvt

'

)3.0("2

"1)(

t

O eKKtv

3.0ot )1(4)3.0( 4.03.0

evo

4.0'

00)( "1 Kvo )(11.2)3.0("

2 VvK o

3.0;11.2)( 4.03.0

tetvt

o

Page 25: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

+-

k10

F20

Ov

a

b

V12

THE SWITCH IS INITIALLYAT a. AT TIME t=0 IT MOVES TO bAND AT t=0.5 IT MOVES BACK TO a.FIND 0,)( ttvO

t

O eKKtv

'2

'1)(

'2

'1][12)0( KKVv

'10)( KvO

5.00,12)( 2.0

tetvt

O

sFk 2.0)20)(10(

985.012)5.0()5.0( 2.05.0

evv OO

')5.0(

"2

"1)(

t

O eKKtv

"985.0)5.0( 2"1 KKvO "

112)( KvO

015.1112985.0"2 K

5.0,015.1112)( 2.05.0

tetvt

O

EXAMPLE

)(st5.0

12

)(tvs

)(tvS

Piecewise constant source

Ott

O eKKtv

21)(

FORM THE OF IS OUTPUT THE CONSTANT IS

SOURCE THE WHEREINTERVAL EACH ON

The constants are determinedin the usual manner

)5.00 bt at (switch FOR 0ot

)at (switch FOR at 5.0 5.0ot

Page 26: ANALYSIS OF CIRCUITS WITH ONE ENERGY STORING ELEMENT CONSTANT INDEPENDENT SOURCES A STEP-BY-STEP APPROACH THIS APPROACH RELIES ON THE KNOWN FORM OF THE.

%pulse1.m% displays the response to a pulse responsetmin=linspace(-0.5,0,50); %negative time segmentt1=linspace(0,0.5,50); %first segmentt2=linspace(0.5, 1.5,100); %second segmentvomin=12*ones(size(tmin));vo1=12*exp(-t1/0.2); %after first switchingvo2=12-11.015*exp(-(t2-0.5)/0.2); %after second switchingplot(tmin,vomin,'bo',t1,vo1,'rx',t2,vo2,'md'),gridtitle('OUTPUT VOLTAGE'), xlabel('t(s)'),ylabel('Vo(V)')

USING MATLAB TO DISPLAY OUTPUT VOLTAGE

FirstOrder