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1 st Order Circuits

RC and RL Circuits

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RC and RL Circuits. 1 st Order Circuits. Objective of the Lecture. Explain the transient response of a RC circuit As the capacitor stores energy when there is: a transition in a unit step function source, u(t-t o ) or a voltage or current source is switched into the circuit. - PowerPoint PPT Presentation

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Page 1: RC and RL Circuits

1st Order Circuits

Page 2: RC and RL Circuits

Objective of the LectureExplain the transient response of a RC circuit

As the capacitor stores energy when there is: a transition in a unit step function source, u(t-to) or a voltage or current source is switched into the

circuit.

Explain the transient response of a RL circuitAs the inductor stores energy when there is:

a transition in a unit step function source, u(t-to) or a voltage or current source is switched into the

circuit.Also known as a forced response to an independent source

Page 3: RC and RL Circuits

RC Circuit

IC = 0A when t < to

VC = 0V when t < to

Because I1 = 0A (replace it with an open circuit).

Page 4: RC and RL Circuits

RC CircuitFind the final conditionof the voltage across the capacitor.

Replace C with an opencircuit and determine the voltage across the terminal.

IC = 0A when t ~ ∞ s VC = VR = I1R when t ~ ∞ s

Page 5: RC and RL Circuits

RC CircuitIn the time between to and t = ∞ s, the capacitor stores energy and currents flow through R and C.

RCeRItV

Idt

dVC

R

V

IIIR

VI

dt

dVCI

VV

tt

C

CC

CR

RR

CC

RC

1)(

0

0

0

1

1

1

Page 6: RC and RL Circuits

RL Circuit

Page 7: RC and RL Circuits

RL Circuit (con’t)Initial condition is not important as the

magnitude of the voltage source in the circuit is equal to 0V when t ≤ to. Since the voltage source has only been turned

on at t = to, the circuit at t ≤ to is as shown below. As the inductor has not stored any energy because

no power source has been connected to the circuit as of yet, all voltages and currents are equal to zero.

Page 8: RC and RL Circuits

RL CircuitSo, the final condition of the inductor current

needs to be calculated after the voltage source has switched on.Replace L with a short circuit and calculate

IL(∞).

Page 9: RC and RL Circuits

Final Condition

R

VI

II

VV

R

RL

L

1

)(

0)(

Page 10: RC and RL Circuits

RL Circuit

/)(1

1

1

1)(

0

0

ottL

LL

RL

eR

VtI

L

VI

L

R

dt

dI

VRIdt

dI

R

L

dt

dILV

RVII

VVV

LL

RRL

RL

/

01

Page 11: RC and RL Circuits

Electronic ResponseTypically, we say that the currents and

voltages in a circuit have reached steady-state once 5 have passed after a change has been made to the value of a current or voltage source in the circuit.In a circuit with a forced response, percentage-

wise how close is the value of the voltage across a capacitor in an RC circuit to its final value at 5?

Page 12: RC and RL Circuits

Complete ResponseIs equal to the natural response of the circuit

plus the forced responseUse superposition to determine the final

equations for voltage across components and the currents flowing through them.

Page 13: RC and RL Circuits

Example #1Suppose there were two unit step function

sources in the circuit.

Page 14: RC and RL Circuits

Example #1 (con’t)The solution for Vc would be the result of

superposition where:I2 = 0A, I1 is left on

The solution is a forced response since I1 turns on at t = t1

I1 = 0A, I2 is left on The solution is a natural response since I2 turns off

at t = t2

Page 15: RC and RL Circuits

Example #1 (con’t)

1

)t-(t-

1

1

when e-1 )(

when 0)(

1

ttRItV

ttVtV

RCC

C

Page 16: RC and RL Circuits

Example #1 (con’t)

2

)t-(t-

2

22

when e)(

when )(2

ttRItV

ttRItV

RCC

C

Page 17: RC and RL Circuits

Example #1 (con’t)If t1 < t2

2

)t-(t-

2

)t-(t-

1

212

)t-(t-

1

12

when e e-1 )(

when e1)(

hen w 0)(

21

1

ttRIRItV

tttRIRItV

ttRIVtV

RCRCC

RCC

C

Page 18: RC and RL Circuits

General Equations

RL

eIIL

tV

eIIItI

RC

eVVC

tI

eVVVtV

tLLL

tLLLL

tCCC

tCCCC

/

)0()()(

)()0()()(

)0()()(

)()0()()(

/

/

/

/

When a voltage or

current source

changes its magnitude

at t= 0s in a simple RC or RL circuit.Equations for a simple RC circuit

Equations for a simple RL circuit

Page 19: RC and RL Circuits

Needed to Complete HW # 21

Page 20: RC and RL Circuits

How to renew your MatLAB licensehttp://swat.eng.vt.edu/Matlabtutorial.html

If you would like to contact them directly, SWAT is located at:2080 Torgersen HallOffice Hours: 12:00pm to 4:00pm Monday - FridayPhone: (540) 231-7815E-mail: [email protected]

Page 21: RC and RL Circuits

Introductory TutorialsMathWorks (www.mathworks.com) has

On-line tutorials including A Very Elementary MATLAB Tutorial

http://www.mathworks.com/academia/student_center/tutorials/intropage.html

Videos (look at the ones below Getting Started)http://www.mathworks.com/products/matlab/demos.html

Worked examples (further down the demos page)http://www.mathworks.com/products/matlab/demos.html

Textbook has a MatLAB tutorial in Appendix E.

Page 22: RC and RL Circuits

SummaryThe final condition for:

the capacitor voltage (Vo) is determined by replacing the capacitor with an open circuit and then calculating the voltage across the terminals.

The inductor current (Io) is determined by replacing the inductor with a short circuit and then calculating the current flowing through the short.

The time constant for:an RC circuit is RC and an RL circuit is L/R

The general equations for the forced response of:the voltage across a capacitor is the current through an inductor is

o

ttoL

ott

oC

tteItI

tteVtVo

o

when 1)(

when 1)(/)(

/)(

Page 23: RC and RL Circuits

SummaryGeneral equations when the magnitude of a

voltage or current source in the circuit changes at t = 0s for the:voltage across a capacitor iscurrent through an inductor is

Superposition should be used if there are multiple voltage and/or current sources that change the magnitude of their output as a function of time.

/

/

)()0()()(

)()0()()(t

LLLL

tCCCC

eIIItI

eVVVtV