lecture 26: wed 18 mar - lsuphys.lsu.edu/~jdowling/phys21022sp09/lectures/26wed18mar.pdfmaglev train...
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Lecture 26: WED 18 MARLecture 26: WED 18 MARCh30Ch30..4–6
Induction and Inductance Induction and Inductance
Physics 2102Spring 2007
Jonathan Dowling
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A Changing Magnetic Field Produces a Current in a Wire Loop
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dA
FaradayFaraday’’s Laws Law• A time varying magnetic FLUX
creates an induced EMF• Definition of magnetic flux is
similar to definition of electricflux
B
�
E = !d"
B
dt
�
!B
=! B " d" A
S
#• Take note of the MINUS sign!!• The induced EMF acts in such away that it OPPOSES thechange in magnetic flux (“Lenz’sLaw”).
�
d! A
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Some ApplicationsSome ApplicationsMagLev train relies onFaraday’s Law: currentsinduced in non-magnetic railtracks repel the movingmagnets creating the induction;result: levitation!
ELECTRIC Guitar pickups also use Faraday’sLaw — a vibrating string modulates the fluxthrough a coil hence creating an electricalsignal at the same frequency.
Fender StratocasterSolenoid Pickup
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Start Your Engines: The Ignition CoilStart Your Engines: The Ignition Coil• The gap between the spark plug
in a combustion engine needs anelectric field of ~107 V/m inorder to ignite the air-fuelmixture. For a typical spark pluggap, one needs to generate apotential difference > 104 V!
• But, the typical EMF of a carbattery is 12 V. So, how does aspark plug work??
spark
12V
The “ignition coil” is a double layer solenoid:• Primary: small number of turns -- 12 V• Secondary: MANY turns -- spark plug
http://www.familycar.com/Classroom/ignition.htm
•Breaking the circuit changesthe current through “primarycoil”• Result: LARGE change in fluxthru secondary -- largeinduced EMF!
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Start Your Engines: The Ignition CoilStart Your Engines: The Ignition Coil
Transformer: P=iV
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dA
Changing B-Field Produces E-Field!Changing B-Field Produces E-Field!
• We saw that a time varyingmagnetic FLUX creates aninduced EMF in a wire,exhibited as a current.
• Recall that a current flows ina conductor because ofelectric field.
• Hence, a time varyingmagnetic flux must induce anELECTRIC FIELD!
• A Changing B-Field Producesan E-Field in Empty Space!
B
dt
dsdE
B
C
!"=#$
!!
To decide SIGN of flux, useright hand rule: curl fingersaround loop, +flux -- thumb.
�
d! A
�
E ! i
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ExampleExample• The figure shows two circular
regions R1 & R2 with radii r1 =1m & r2 = 2m. In R1, themagnetic field B1 points out ofthe page. In R2, the magneticfield B2 points into the page.
• Both fields are uniform and areDECREASING at the SAMEsteady rate = 1 T/s.
• Calculate the “Faraday”integral for the two pathsshown.
R1 R2
! "C
sdE!!
I
II
VsTrdt
dsdE
B
C
14.3)/1)((2
1 +=!!="
!=#$ %!!
Path I:
[ ] VsTrsTrsdE
C
42.9)/1)(()/1)((2
2
2
1 +=!+!!!="# $$!!
Path II:
B1
B2
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Solenoid ExampleSolenoid Example• A long solenoid has a circular cross-
section of radius R.• The magnetic field B through the solenoid
is increasing at a steady rate dB/dt.• Compute the variation of the electric field
as a function of the distance r from theaxis of the solenoid.
First, let’s look at r < R:
dt
dBrrE )()2( 2
!! =
dt
dBrE
2=
Next, let’s look at r > R:
dt
dBRrE )()2( 2
!! =
dt
dB
r
RE
2
2
=
magnetic field lines
electric field lines
B
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Solenoid Example Cont.Solenoid Example Cont.
r
E(r)
r = R
Er<R
=r
2
dB
dt
! r
Er>R
=R2
2r
dB
dt
!1 / r
Added Complication: Changing B FieldIs Produced by Changing Current i inthe Loops of Solenoid!
B = µ0ni
dB
dt= µ
0ndi
dt
i
i
E
B
Er<R =
µ0nr
2
di
dtEr>R =
µ0nR
2
2r
di
dt
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SummarySummaryTwo versions of Faradays’ law:
– A time varying magnetic flux produces an EMF:
�
E = !d"
B
dt
dt
dsdE
B
C
!"=#$
!!
–A time varying magnetic flux produces anelectric field: