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Physics 202
Thursday, April 8, 1999
Announcements: Lab quiz next week on Lab # 8
(RC circuits)
Lecture notes:
Examples of Lenz's Law
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Current in the loop is such that it creates a B field opposite to the motion
of the magnet
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If the magnet moves towards the loop, the current in the loop is clockwise;
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If the magnet is moving away, the current is counerclockwise.
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The setup is exactly oppositeas the previous example
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If the magnet is moving towards the loop, current is counterclockwise.
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If the magnet is moving away, current is clockwise.
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At t= 0 the switch is closed; Current in the left hand loop (counterclockwise)
gives rise to a magnetic field, that points to the left and increases with
time.
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With time, the induced current in the right hand loop must be in a direction
that produces an induced magnetic field that opposes the magnetic field
due to the left hand loop.
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The direction of current in the right loop is opposite that of the left
loop.
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The switch had been closed for a long time and at t= 0 it was opened. The
magnetic field still points to the left, but it is decreasing with time.
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The induced current in the right loop is such that it must produce a magnetic
field that opposes the change in the magnetic field due to the left loop.
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The induced current in the left loop is the same as the current in the
right loop. Both are counterclockwise.
See also problem 31-5 on page 777 of the text for an additional example
Applications of Faraday's Law
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Generators: Area changes with time, but magnetic
field stays constant
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FB = B (dot
product) A = BAcosq
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If the coil is being rotated, FB
= BAcoswt
x = - dFB/dt
= + BAwcoswt
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If there are N turns;
x = +N BAwcoswt
Several in class demonstrations were performed to demonstrate Lenz's
Law and Faraday's Law
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