Download - EECS2200 Chapter 5 part1 - York University

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Page 1: EECS2200 Chapter 5 part1 - York University

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EECS2200 Electric Circuits

Chapter 5

Capacitance, Inductance, and RC/RL circuits

Objectives (1) n  Understand how an inductor or a capacitor

behaves in the presence of a constant current or constant voltage

n  Know and being able to use the equations of current, voltage power and energy in an inductor and capacitor

n  Be able to combine inductors (capacitors) with an initial condition in series and parallel to form a single equivalent conductor (capacitor).

n  Understand the basic concept of mutual inductance and being able to write mesh-current equations for a circuit containing magnetically coupled coils using the dot convention correctly.

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Objective (2) n  Be able to determine the natural response

of RL and RC circuits. n  Be able to determine the step response of

RL and RC circuits.

EECS2200 Electric Circuits

Chapter 5 Part 1

Capacitance and RC circuits

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EECS2200 Electric Circuits

Capacitor

Capacitor

n  Parallel plates, separated by an insulator, so no charge flows between the plates. Impose a time-varying voltage drop.

n  Capacitor equation:

n  Units: v(t) is volts, i(t) is amps, and C is farads [F]

dttdvCti )()( =

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Activity 1 Look at the capacitor equation: Suppose v(t) is constant, what is the value of i(t)? A.  0 B. ∞ C. a constant

dttdvCti )()( =

Activity 2 if the voltage drop across the capacitor is constant, its current is 0, so the capacitor can be replaced by: A. A short circuit B. An open circuit C. a constant

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Capacitor n  If the voltage drop across a capacitor is constant, the

current is 0, so the capacitor can be replaced by an OPEN CIRCUIT.

n  Look at the capacitor equation again:

n  Suppose there is a discontinuity in v(t) – that is, at some value of t, the voltage jumps instantaneously. At this value of t, the derivative of the voltage is infinite. Therefore the current is infinite! NOT POSSIBLE.

n  Thus, the voltage drop across a capacitor is continuous for all time.

dttdvCti )()( =

Voltage n  The equation for voltage in terms of current:

∫∫

+=⇒

=⇒

=⇒=

t

t o

tv

tv

t

t

o

oo

tvdiC

tv

dxCdi

tCdvdttidttdvCti

)()(1)(

)(

)()()()(

)(

)(

ττ

ττ

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Power and Energy n  Power and energy

p(t) = v(t)i(t) =Cv(t) dv(t)dt

p(t) = dw(t)dt

=Cv(t) dv(t)dt

⇒ dw(τ ) =Cv(τ )dv(τ )

⇒ dx =C y(τ )dτ0

v(t )∫0

w(t )∫

⇒ w(t) = 12Cv(t)

2

Activity 3 Find the voltage, power, and energy

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Capacitor in series

Capacitor in parallel

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EECS2200 Electric Circuits

RC Natural Response

Introduction n  Natural Response: The current and

voltages that arise when the stored energy in the L of C is released.

n  Step Response: The current and voltage that arise when energy is being acquired by the L or C when a sudden application of voltage or current is applied to the circuit.

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RC Natural Response n  Switch in position A for a long time n  The capacitor charged to Vg

RC Natural Response To evaluate the voltage drop across the capacitor for t < 0, put the switch in the “a” position and replace the capacitor with an open circuit. The voltage drop across the open circuit, positive at the top, is A.  Vg

B.  -Vg

C. RVg / (R + R1)

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RC Natural Response

:0<t

0, <= tVv g

There is an open circuit here, so the current in this circuit is 0, and the voltage drop across R1 is 0. Thus,

Remember the continuity requirement for capacitors – the voltage drop across the capacitor must be continuous everywhere, so that the current through the capacitor remains finite. Thus,

gVv =)0(

RC Natural Response

:0≥tKCL at b: C dv(t)

dt+v(t)R

= 0

0,)(so)0(But1Solving,

01so0)1(g,Rearrangin0ng,Substituti

)(and)(Let

)1( ≥==

=

=−=−

=+−

−==

−−

−−

teVtvVvRCa

aCReaCRRe)aeC(

aedttdvetv

tRCgg

at

atat

atat

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Activity 4 Find Vc(t) for t>=0

EECS2200 Electric Circuits

RC Step Response

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Step Response of RC Circuits

Step Response of RC Circuit

( ) RCtss

RCt

s

s

s

s

ttv

V s

s

ss

s

eRIVRItv

eRIVRItv

tRCRIV

RItv

dtRCRIv

dv

dtRCRIv

dvRC

RIvC

IRvdtdv

IRv

dtdvC

/0

/

0

0

0

)(

)(

)()()(

1)()()(ln

1

1

/

0

−+=

=−

−=

−=

−=

+−=

+−=

=+

∫∫

( )

RCts

RCts

eRVIi

eRC

RIVCi

dtdvCi

/0

/0

1

⎟⎠

⎞⎜⎝

⎛ −=

⎟⎠

⎞⎜⎝

⎛ −−=

=

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v i

RC Step Response n  R=10 KΩ, C=1 µF n  Is=5A, V0=0

Activity 5 The switch has been in position 1 for a long time. At t=0, the switch moves to position 2. Find v0(t) for t>=0 and io(t) for t>=0+