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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
 
  • Current in the loop is such that it creates a B field opposite to the motion of the magnet
    • If the magnet moves towards the loop, the current in the loop is clockwise;
    • If the magnet is moving away, the current is counerclockwise.
  • The setup is exactly oppositeas the previous example
    • If the magnet is moving towards the loop, current is counterclockwise.
    • If the magnet is moving away, current is clockwise.
  • 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.
    • 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.
    • The direction of current in the right loop is opposite that of the left loop.
  • 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.
    • 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.
    • 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
  • Generators: Area changes with time, but magnetic field stays constant
    • FB = B (dot product) A = BAcosq
    • If the coil is being rotated, FB =  BAcoswt

    • x = - dFB/dt = + BAwcoswt
    • If there are N turns;
              x =  +N BAwcoswt


Several in class demonstrations were performed to demonstrate Lenz's Law and Faraday's Law
 
Information contained on this page does not represent the lecture verbatim.
These notes are not a substitute for class attendance.



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