electricity & magnetism lecture 18 - sfu.ca lecture 18 - induction.pdf · electricity &...

Electricity & MagnetismLecture 18

Today’sConcepts: A)Induc4on

B)RLCircuits

Electricity&Magne/smLecture18,Slide1

ExtendeddeadlinefornextfewFlipItPhysicshomework:! 80%extendedbyoneweek.

SomeupcomingFlipItcheckpointsincludeques4onsonLabMaterials

ClassschedulenowincludesTiplerchapterreferences

Tipler ConcordancePhysics 141 Spring 2017

Date Unit # Topics FlipItPhysics Unit Due Date

Wed, Jan 4 19 Electrostatics 01/11/2017 21-1,21-2

Fri, Jan 6 19 Coulomb's Law Coulomb's Law 21-3

Mon, Jan 9 19 Electric Fields Electric Fields

Wed, Jan 11 20 Electric Field Lines and Flux Electric Flux and Field Lines 01/18/2017 21-4,21-5

Fri, Jan 13 20 Gauss' Law Gauss' Law 22-1,22-2

Mon, Jan 16 20 Gauss' Law Calculations

Wed, Jan 18 21Electric Potential Energy 01/23/2017 22-3,

Fri, Jan 20 21 Electric Potential Electric Potential 23-1,23-2,23-3

Mon, Jan 23 22 Current and Resistance Electric Current 01/29/2016 23-4.23-5,23-6

Wed, Jan 25 22 Series and Parallel Circuits 24-1,24-2,24-3

Fri, Jan 27 23Kirchhoff's Rules 02/01/2017 25-1,25-2,25-3

Mon, Jan 30 23 Kirchhoff's Laws Conductors and Capacitors 25-4,25-4

Wed, Feb 1 24 Capacitance Capacitors 24-3

Fri, Feb 3 Midterm 1 25-6

Mon, Feb 6 24 RC Circuits RC Circuits 26-1,26-2

Wed, Feb 8 25 Magnetic Forces and Fields Magnetism 02/20/2017

Fri, Feb 10 25 Forces and Torques on Currents 26-3, (26-4)

Mon, Feb 13 Break 27-1,27-2

Wed, Feb 15 Break 27-4

Fri, Feb 17 Break 28-1,28-2,28-3,28-4

Mon, Feb 20 26s1 Magnetism from Electricity Ampere's Law, Biot-Savart Law 03/10/2017

Wed, Feb 22 26s2 Faraday's Law Motional EMF 28-6.28-7,28-8

Fri, Feb 24 27s1 Faraday's Law 03/10/2017 29-1,29-2

Mon, Feb 27 26s3 Induction and RL Circuits

Wed, Mar 1 27s2 AC Circuits LRC Circuits 29-3,29-4

Fri, Mar 3 Practice AC Circuits 29-5.29-6

Mon, Mar 6 Practice AC Circuits: Resonance and Power

Wed, Mar 8 practical exam 30-1,30-2

Fri, Mar 10 practical exam 30-3,30-4

Mon, Mar 13 28 Electromagnetic Waves Displacement Current and E-M Wa 03/20/2017 31-4,

Wed, Mar 15 28 Properties of Electromagnetic Waves

Fri, Mar 17 28 Polarization Polarization 31-1,31-2,31-3,31-5

Mon, Mar 20 29 Reflection and Images Reflection and Refraction 03/22/2017 32-1,32-2

Wed, Mar 22 30 Lenses, Mirrors 04/03/2017 32-4

Fri, Mar 24 Midterm 2

Mon, Mar 27 30 Optical Instruments

Wed, Mar 29 31 Interference 04/03/2017 33-1,33-2

Fri, Mar 31 31 Interference & Diffraction 33-3.33-4.33-8

Mon, Apr 3 32 Intro to Quantum Mechanics 04/07/2017

Wed, Apr 5 32 More Quantum 36-1,36-2

Fri, Apr 7 32 Review 36-3.36-4

Mon, Apr 10 Final Exam 8:30=11:30

Tipler 6th

Electric & Gravitational

Forces

Error Propagation, Digital

Meters

Magnetic Forces and Electric

Current

AC Circuits and the

OscilloscopeVerification of Faraday's Law

and Maxwell's Equations

Energy Transport and

Polarization

Refraction, Prisms and

Lenses

Lenses and Mirrors

Combination

Stuff you said..

Willtherebemorelabac4vi4esinvolvingoscilloscopes?Unlikelabac4vi4esinvolvingmagnets,theoscilloscopesareforeign,new,andcuriouslyinteres4ngtoplay/learnwithduetotheabove?

WhataretheexactdifferencesbetweentheCapacitorandInductor.Inwhichsitua4onwouldIusetheCapacitorinsteadoftheInductororviceversa?

http://www.sfu.ca/phys/141/1154/Schedule141.pdf

Capacitors are yin — Inductors are yang



Comments

what'sthedifferencebetweenintegralbdotdaandintegralbdotds.Whendoweuseeachone! B•DAisforGauss’law! B•dsisforAmpere’slaw

Howisenergystoredinamagne4cfield,similartocapacitorsstoringenergyasanelectricfield?! Itjustis.Bothelectricfieldsandmagne4cfieldsstoreenergylikeaspringstoresenergywhencompressed

E = ��B

dt= �NA

dBdt

Today’s Experiment


Loop area A

E = ��B

dt= �A

dBdt

If there are more turns N in the loop,

Wrapawireintoacoiltomakean“inductor”…

dIdt

ε = −L

From the Prelecture: Self Inductance


currentI

L

dIdt

εL = −L

emfinducedacrossLtriestokeepIconstant.

Inductorspreventdiscon4nuouscurrentchanges!

It’slikeiner4a!

What this really means:


Twosolenoidsaremadewiththesamecrosssec/onalareaandtotalnumberofturns.InductorBistwiceaslongasinductorA

ComparetheinductanceofthetwosolenoidsA)LA = 4 LB B)LA = 2 LB C)LA = LB D)LA = (1/2) LB E)LA = (1/4) LB

(1/2)2 2

CheckPoint 2


RL

At t = 0:I = 0VL = VBATTVR = 0(L islikeagiantresistor)

VBATT

I = 0

At t >> L/R:VL = 0 VR = VBATTI = VBATT/R(Lislikeashortcircuit)

R

I = V/R

L

VBATT

Whennocurrentisflowingini4ally:

How to think about RL circuits Episode 1:

VL


WhatisthecurrentIthroughthever/calresistorimmediatelyaRertheswitchisclosed?

(+isinthedirec/onofthearrow)

A)I = V/R B)I = V/2R C)I = 0 D)I = −V/2R E)I = −V/R

Inthecircuit,theswitchhasbeenopenforalong/me,andthecurrentiszeroeverywhere.

At/met=0theswitchisclosed.

IL = 0

CheckPoint 4


WhatisthecurrentIthroughthever/calresistoraRertheswitchhasbeenclosedforalong/me?


A)I=V/R B) I =V/2RC)I= 0D)I=−V/2R E)I= −V/R

RL Circuit (Long Time)


RL

VBATT

I = V/R

At t >> L/R:I = 0VL = 0VR = 0

R

I = 0

LR

I = VBATT/RVR = IR VL = VR

At t = 0:

When steady current is flowing initially:

How to Think about RL Circuits Episode 2:

VL


WhatisthecurrentIthroughthever/calresistorimmediatelyaRertheswitchisopened?


A)I=V/RB)I=V/2RC)I=0 D)I= −V/2RE)I= −V/R

AReralong/me,theswitchisopened,abruptlydisconnec/ngthebaXeryfromthecircuit.

CheckPoint 6


R

I

V = IRdIdtV = L L

+

−

−

+

Why is there Exponential Behavior?

VL


where

Prelecture:

RL

I

Lecture:

VLVBATT

Didwemessup?

No:Theresistanceissimplytwiceasbiginonecase.


ARerlong/meat0,movedto1 ARerlong/meat0,movedto2

A]erswitchmoved,whichcasehaslarger4meconstant?

A)Case1B)Case2C)Thesame

CheckPoint 8



CheckPoint 10ARerlong/meat0,movedto1 ARerlong/meat0,movedto2

Immediatelya]erswitchmoved,inwhichcaseisthevoltageacrosstheinductorlarger?


I0 is V/R in both casesA) VL(0) = I0*2RB) VL(0) = I0*3R


CheckPoint 12ARerlong/meat0,movedto1 ARerlong/meat0,movedto2

A]erswitchmovedforfinite4me,inwhichcaseisthe

currentthroughtheinductorlarger?


A) τ1 = L/2RB) τ2 = L/3R

VL

τ1τ2

ConceptualAnalysisOnceswitchisclosed,currentswillflowthroughthis2-loopcircuit.KVRandKCRcanbeusedtodeterminecurrentsasafunc4onof4me.

StrategicAnalysisDeterminecurrentsimmediatelya]erswitchisclosed.Determinevoltageacrossinductorimmediatelya]erswitchisclosed.DeterminedIL/dtimmediatelya]erswitchisclosed.

R1

LV

R2

R3

Calculation

Theswitchinthecircuitshownhasbeenopenforalong4me.Att = 0,theswitchisclosed.

WhatisdIL/dt,the4merateofchangeofthecurrentthroughtheinductorimmediatelya]erswitchisclosed


WhatisIL,thecurrentintheinductor,immediatelyaRertheswitchisclosed?

A)IL = V/R1 up B)IL = V/R1 down C)IL = 0

IL = 0

Calculation


R1

LV

R2

R3


A)B)C)D)

Calculation

IL(t = 0 +) = 0


R1

LV

R2

R3

WhatisthemagnitudeofI2,thecurrentinR2,immediatelya]ertheswitchisclosed?


IL(t = 0 +) = 0 I2(t = 0 +) = V/(R1+ R2+ R3)

Calculation


R1

LV

R2

R3

I2

A)B)C)D)E)

WhatisthemagnitudeofVL,thevoltageacrosstheinductor,immediatelya]ertheswitchisclosed?


A)B)C)D)

VL(t = 0 +) = V(R2+ R3)/(R1+ R2+ R3)

Calculation


WhatisdIL/dt,the4merateofchangeofthecurrentthroughtheinductorimmediatelya]erswitchisclosed

R1

LV

R2

R3


Follow Up

Theswitchinthecircuitshownhasbeenclosedforalong4me.

WhatisI2,thecurrentthroughR2?

(Posi4vevaluesindicatecurrentflowstotheright)

R1

LV

R2

R3

A)B)C)D)


Theswitchinthecircuitshownhasbeenclosedforalong4meatwhichpoint,theswitchisopened.

WhatisI2,thecurrentthroughR2immediatelya]er

switchisopened?(Posi4vevaluesindicatecurrentflowstotheright)

Follow Up 2R1

LV

R2

R3

I2


A)B)C)D)E)

electricity & magnetism lecture 18 - sfu.ca lecture 18 - induction.pdf · electricity &...

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