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Electro magnetic Induction ch 21

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EM Induction is where we get all this electricity stuff. ( w/out induction there would be no ipods, cell phones, video games) EM Induction ... – PowerPoint PPT presentation

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Title: Electro magnetic Induction ch 21


1
Electro magnetic Induction (ch 21)
  • Well cover ch 21.1 21.4
  • EM Induction is where we get all this electricity
    stuff. (w/out induction there would be no ipods,
    cell phones, video games)

2
EM Induction
  • Michael Faraday found that a changing magnetic
    field creates an induced current in a coil of
    wire.
  • A changing magnetic field induces an emf (emf a
    voltage and hence a current)
  • This induced emf is created when the magnetic
    field is moving relative to the conductor.

3
EM Induction
  • Magnetic Flux is the amount of magnetic field
    crossing a given area
  • F BAcosT magnetic flux
  • A area, B magnetic field, and the angle is
    measured from the line (axis) perpendicular to A
    with the B field. (Flux is a maximum when it
    crosses the area perpendicular)

4
EM Induction
  • Faradays Law for induction the amount of emf
    produced depends on the change in flux per time.
  • EMF (or voltage) -?f/?t -?BAcosT/?t
  • To create an EMF(voltage) you can change either
    the magnetic field B, the area A, or the angle
    (like rotating a magnetic inside a conductor).

5
EM Induction
  • Direction of the induced emf
  • The current induced is directed to create its own
    magnetic field which will oppose the changing
    flux which is inducing it (huh?)
  • In other words, the current induced will always
    make a magnetic field which tries to keep things
    the way they were. (oh, thats much clearer)

6
EM Induction
  • If the conductor is a coil of wire with N loops,
    then the emf-N?f/?t.

7
EM Induction
  • For a moving conductor crossing a magnetic field,
    there is one more relationship on the 50,000
    green sheet
  • It can be shown (look on page 590) that emf Blv
    where B magnetic field, l length of wire
    crossing the field, v velocity of that length
    of wire crossing the field.
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