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Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic...

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Physics 202, Lecture 18 Today’s Topics Reminder RL Circuits RC Circuits LC (RLC) Circuits and Electromagnetic Oscillations AC Circuits with AC Source Phasors
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Page 1: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Physics 202, Lecture 18Today’s Topics

Reminder RL Circuits RC Circuits LC (RLC) Circuits and Electromagnetic Oscillations

AC Circuits with AC Source Phasors

Page 2: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Physics 202, Lecture 18Today’s Topics

Reminder RL Circuits RC Circuits LC (RLC) Circuits and Electromagnetic Oscillations

AC Circuits with AC Source Phasors

Phaser

Page 3: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Turn on RL Circuit (reminder)

Note: the time constant is τ=L/R

I = V0R(1− e

− tL /R )

Page 4: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Turn off RL Circuit (reminder)

Note: the time constant is τ=L/R

I = I0e− tL /R

Page 5: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Charging a Capacitor in RC Circuit

Charging

)1()( /RCteCtq −−= ε RCteR

tI /)( −= ε

Note: τ≡RC is called time constant

0)(/)( =−−dttdqRCtqε

Page 6: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Discharging a Capacitor in RC Circuit

discharging

RCtQetq /)( −=

I(t) = − QRC

e−t /RC

Note the time constant τ=RC

q(t) /C + R dq(t)dt

= 0

Page 7: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Demo: RC Circuit

Light Bulb

r

Page 8: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

LC Circuit and Oscillation Exercise: Find the oscillation frequency of a LC circuit

0)(/)( =−−dttdILctq

)sin()cos(

1

0)(1)(

max

max

2

2

2

φωωφω

ω

ω

+−=+=

=

=+

tQItQq

LC

dttqdtq

0)(/)( 2

2

=+dttqdLCtq

eq. of Harmonic Oscillation

Total Energy is conserved

I

Page 9: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

AC Power Source ΔV = ΔVmax Sin(ωt+φ0) = ΔVmax Sin(ωt)

Initial phase, usually set φ0=0

T=2π/ω

ω: angular frequencyω=2πf

t=0

Page 10: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

AC Circuit Find out current i and voltage difference ΔVR, ΔVL, ΔVC.

Notes: • Kirchhoff’s rules still apply !• A technique called phasor analysis is convenient.

i

ΔVmax Sin(ωt)

Page 11: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Phasor A sinusoidal function y= Asinφ can be represented

graphically as a phasor vector with length A andangle φ (w.r.t. to horizontal)

φ

A

Asi

Page 12: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Resistors in an AC Circuit

Ohm’s Law: ΔV=IR at any time

i

iR=ΔV/R=Imax sinωt, Imax=ΔVmax/R

The current through an resistor is in phase with the voltage across it Phasor view

Function view

Page 13: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Inductors in an AC Circuit ΔV - Ldi/dt =0

iL=Imax sin(ωt-π/2)Imax=ΔVmax/XL, XL= ωL inductive reactanceThe current through an inductor is 90o behind the voltage across it.

Phasor view

Function viewi

Page 14: Physics 202, Lecture 18...Physics 202, Lecture 18 Today’s Topics ... qtCL eq. of Harmonic Oscillation Total Energy is conserved I. AC Power Source ...

Capacitors in an AC Circuit

ΔV - q/C=0, dq/dt =i

i

iL=Imax sin(ωt+π/2)Imax=ΔVmax/XC, XC= 1/(ωC) capacitive reactanceThe current through a capacitor is 90o ahead of the voltage across it. Phasor view

Function view


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