Induction Physics 102 Professor Lee Carkner Lecture 19.

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Induction Physics 102 Professor Lee Carkner Lecture 19
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Transcript of Induction Physics 102 Professor Lee Carkner Lecture 19.

Page 1: Induction Physics 102 Professor Lee Carkner Lecture 19.

Induction

Physics 102Professor Lee

CarknerLecture 19

Page 2: Induction Physics 102 Professor Lee Carkner Lecture 19.

Rail Gun

For each rail B = 0I/2r B = (4X10-7)(100000) /

2(0.005) B = 4 T so sum of B = 8 T

Force on conductor: F = BIL sin F = (8)(100000)(0.01) sin 90 F = 8000 N

II

X

B field from each rail

F

Page 3: Induction Physics 102 Professor Lee Carkner Lecture 19.

Magnetic Fields and Current

We have already seen that:

There should be a parallel effect where magnetic fields can produce currents

Constant magnetic fields do not produce currents

For the area of interest there must either more or less magnetic field with time

Page 4: Induction Physics 102 Professor Lee Carkner Lecture 19.

Magnetic Flux Consider a region with a magnetic field

We will define the magnetic flux as the component of the B field that passes through a region times the area of the region, or:

= BA cos Unit of flux is the Weber (Wb), 1 Wb = 1 T m2

= 0 means face on = 90 means edge on

Page 5: Induction Physics 102 Professor Lee Carkner Lecture 19.

Magnetic Flux

Page 6: Induction Physics 102 Professor Lee Carkner Lecture 19.

Flux Through a Loop

What is force on particle?

aligned with B, F= 0

Same is true for flux if = 0, = BA =

maximum flux if = 90, = 0

=BA cos 0 =BA

= BA cos 90 = 0

Page 7: Induction Physics 102 Professor Lee Carkner Lecture 19.

Induction What happens if you change the flux through a loop of wire?

Connect a loop to an ammeter and move a magnet through it

Current stops when the movement stops

Usually means something (either the loop or the magnet) must be moving

Page 8: Induction Physics 102 Professor Lee Carkner Lecture 19.

Faraday’s Law We can find the emf from Faraday’s Law:

= -N(/t)

To find the emf, we don’t want , but rather how fast changes

Can write as:/t = (f-i)/(tf-ti)

/t is also the slope of a line on a -t diagram

Page 9: Induction Physics 102 Professor Lee Carkner Lecture 19.

Lenz’s Law The induced current produces a magnetic

field of its own

Lenz’s Law: The induced current will be in a

direction such that the magnetic field it produces will counteract the changes in the original B

Page 10: Induction Physics 102 Professor Lee Carkner Lecture 19.

Induced Current

Page 11: Induction Physics 102 Professor Lee Carkner Lecture 19.

Changing B Consider a loop in a B field

The induced current flows such that the induced B is in the same direction as the original field

If you increase the flux: The induced current flows such

that the induced B is opposite the original field

Page 12: Induction Physics 102 Professor Lee Carkner Lecture 19.

Applied Induction

Induction is useful because it links physical motion to electric currents The moving magnet produces a changing

flux

The current thus preserves a record of the motion

Many applications in music

Page 13: Induction Physics 102 Professor Lee Carkner Lecture 19.

Microphone

Page 14: Induction Physics 102 Professor Lee Carkner Lecture 19.

Electric Guitar

Page 15: Induction Physics 102 Professor Lee Carkner Lecture 19.

Induction Devices Microphone

Speaker

Electric guitar Pickup magnet magnetizes string, the motion of

which induces current

Tape recorders and players The tape is magnetized such that when it passes the

tape heads it induces a current

Page 16: Induction Physics 102 Professor Lee Carkner Lecture 19.

How Does Induction Work? If we move the wire through a B field

the electrons now have a velocity

This deflection produces an imbalance of charge

Page 17: Induction Physics 102 Professor Lee Carkner Lecture 19.

Next Time

Read 21.3-21.6 Homework, Ch 21, P 7, 9, 11, 13

Page 18: Induction Physics 102 Professor Lee Carkner Lecture 19.

A wire is carrying a current straight towards you. What is the direction of the magnetic field of the wire?

A) straight towards you B) downC) upD) circling the wire in a clockwise

directionE) circling the wire in a

counterclockwise direction

Page 19: Induction Physics 102 Professor Lee Carkner Lecture 19.

A horizontal wire is carrying a current straight north. What is the direction of the magnetic field directly above the wire and directly below the wire?

A) east, west B) up, downC) north, southD) up, westE) It depends on the magnitude of

the current

Page 20: Induction Physics 102 Professor Lee Carkner Lecture 19.

A horizontal wire is carrying a current to your right. What direction would a proton be deflected in if it traveling exactly below the wire also to the right?

A) leftB) rightC) upD) downE) right at you