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Transient Analysis of RC circuits Nano107 Chapter 7

07NANO107 Transient Analysis of RC-RL Circuits

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Page 1: 07NANO107 Transient Analysis of RC-RL Circuits

Transient Analysis of RC circuits

Nano107

Chapter 7

Page 2: 07NANO107 Transient Analysis of RC-RL Circuits

Why there is a transient response?

• The voltage across a capacitor cannot be changed instantaneously.

)0()0( CC VV

• The current across an inductor cannot be changed instantaneously.

)0()0( LL II

Page 3: 07NANO107 Transient Analysis of RC-RL Circuits

Figure 5.9,

5.10

(a) Circuit at t = 0

(b) Same circuit a long time after the switch is closed

The capacitor acts as open circuit for the steady state condition

(a long time after the switch is closed).

Page 4: 07NANO107 Transient Analysis of RC-RL Circuits

(a) Circuit for t = 0

(b) Same circuit a long time before the switch is opened

The inductor acts as short circuit for the steady state condition

(a long time after the switch is closed).

Page 5: 07NANO107 Transient Analysis of RC-RL Circuits

)1(

t

C eEv

/tc eE

dt

dv

0

0

tc

tc

dt

dv

EE

dt

dv

RCTime Constant

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

C

2

K

E

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10ms

V(2)

0V

5V

10V

SEL>>

RC

R=2k

C=0.1F

Transient Response of RC Circuits

vc

Page 6: 07NANO107 Transient Analysis of RC-RL Circuits

WHAT IS TRANSIENT RESPONSE

Figure 5.1

Page 7: 07NANO107 Transient Analysis of RC-RL Circuits

Solution to First Order Differential Equation

)()()(

tfKtxdt

tdxs

Consider the general Equation

Let the initial condition be x(t = 0) = x( 0 ), then we solve the

differential equation:

)()()(

tfKtxdt

tdxs

The complete solution consists of two parts:

• the homogeneous solution (natural solution)

• the particular solution (forced solution)

Page 8: 07NANO107 Transient Analysis of RC-RL Circuits

The Natural Response

/)(,)(

)(

)(

)(,

)()(0)(

)(

t

N

N

N

N

NNNN

N

etxdt

tx

tdx

dt

tx

tdxtx

dt

tdxortx

dt

tdx

Consider the general Equation

Setting the excitation f (t) equal to zero,

)()()(

tfKtxdt

tdxs

It is called the natural response.

Page 9: 07NANO107 Transient Analysis of RC-RL Circuits

The Forced Response

0)(

)()(

tforFKtx

FKtxdt

tdx

SF

SFF

Consider the general Equation

Setting the excitation f (t) equal to F, a constant for t 0

)()()(

tfKtxdt

tdxs

It is called the forced response.

Page 10: 07NANO107 Transient Analysis of RC-RL Circuits

The Complete Response

)(

)()(

/

/

xe

FKe

txtxx

t

St

FN

Consider the general Equation

The complete response is:

• the natural response +

• the forced response

)()()(

tfKtxdt

tdxs

Solve for ,

)()0(

)()0()0(

0

xx

xxtx

tfor

The Complete solution:

)()]()0([)( / xexxtx t

/)]()0([ texx called transient response

)(x called steady state response

Page 11: 07NANO107 Transient Analysis of RC-RL Circuits

KVL around the loop: EvRi Cc

EvRdt

dvC c

c

EAev RC

t

C

Initial condition 0)0()0( CC vv

)1()1(

t

RC

t

C eEeEv

dt

dvCi c

c

t

eR

E

Switch is thrown to 1

RCCalled time constant

Transient Response of RC Circuits

EA

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

C

2

K

E

cc

dvi C

dt

Page 12: 07NANO107 Transient Analysis of RC-RL Circuits

)1(

t

C eEv

/tc eE

dt

dv

0

0

tc

tc

dt

dv

EE

dt

dv

RCTime Constant

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

C

2

K

E

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10ms

V(2)

0V

5V

10V

SEL>>

RC

R=2k

C=0.1F

Transient Response of RC Circuits

vc

Page 13: 07NANO107 Transient Analysis of RC-RL Circuits

Switch to 2

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

C

2

K

E RC

t

c Aev

Initial condition

Evv CC )0()0(

0 Riv cc

0dt

dvRCv c

c

// tRCt

c EeEev

/t

c eR

Ei

Transient Response of RC Circuits

cc

dvi C

dt

Page 14: 07NANO107 Transient Analysis of RC-RL Circuits

RCTime Constant

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

C

2

K

E

R=2k

C=0.1F

Time

0s 1.0ms 2.0ms 3.0ms 4.0ms 5.0ms 6.0ms 7.0ms 8.0ms

V(2)

0V

5V

10V

SEL>>

t

RC

t

C EeEetv

)(

E

dt

dv

t

C 0

0

t

C

dt

dv

E

Transient Response of RC Circuits

vc

Page 15: 07NANO107 Transient Analysis of RC-RL Circuits

Response to square wave input

Time

0s 0.5ms 1.0ms 1.5ms 2.0ms 2.5ms 3.0ms 3.5ms 4.0ms 4.5ms 5.0ms 5.5ms 6.0ms

V(2) V(1)

0V

2.0V

4.0V

6.0V

vR

Page 16: 07NANO107 Transient Analysis of RC-RL Circuits

Transient Response of RL Circuits Switch to 1

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

L

2

K

E

dt

diLvL

KVL around the loop: EviR L

iRdt

diLE

Initial condition 0)0()0(,0 iit

Called time constant RL /

/

/

/

(1 ) (1 )

(1 )

1

Rt

tL

t

R

R Rt t

L LL

t

L

E Ei e e

R R

v iR E e

di d E E Rv L L e L e

dt dt R R L

v Ee

Page 17: 07NANO107 Transient Analysis of RC-RL Circuits

Transient Response of RL Circuits

Switch to 2

tL

R

Aei

dtL

R

i

di

iRdt

diL

0

Initial condition R

EIt 0,0

/tt

L

R

eR

Ee

R

Ei

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

L

2

K

E

0

0

0

0

0

: 0

:

1

ln

i t t

I

i t t

I

t t

i I i t

Rdi dt

i L

Ri t

L

tL

R

I

ti

0

)(ln

tL

R

eIti

0)(

Page 18: 07NANO107 Transient Analysis of RC-RL Circuits

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

L

2

K

E

Transient Response of RL Circuits

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10ms

I(L1)

0A

2.0mA

4.0mA

SEL>>

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10ms

I(L1)

0A

2.0mA

4.0mA

SEL>>

Input energy to L

Switch to 2

_ US I1

I1

I1

I1

I1 I1 I1 I1

R

R1

R1 R1

5

5

5 5 +

+

_

US

IS

E

U1

+

- 1 U

L

2

K

E

Switch to 1

iL

iL

Page 19: 07NANO107 Transient Analysis of RC-RL Circuits

Basic RL and RC Circuits: Summary The Time Constant

• For an RC circuit, = RC

• For an RL circuit, = L/R

• -1/ is the initial slope of an exponential with an initial value of 1

• Also, is the amount of time necessary for an exponential to decay

to 36.7% of its initial value

• When a sudden change occurs, only two types of quantities will remain the same as before the change.

– IL(t), inductor current

– Vc(t), capacitor voltage

• Find these two types of the values before the change and use them as the initial conditions of the circuit after change.

How to determine initial conditions for a transient circuit?

Page 20: 07NANO107 Transient Analysis of RC-RL Circuits

Summary

Initial Value

(t = 0)

Steady Value

(t )

time

constant

RL

Circuits

Source

(0 state)

Source-

free (0 input)

RC

Circuits

Source

(0 state)

Source-

free (0 input)

00 iR

EiL

R

Ei 0

0i

00 v Ev

Ev 0 0v

RL /

RL /

RC

RC