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Induced emf and Magnetic Flux F

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Faraday found that induced emf is produced by a changing magnetic field ... coil, E = -L(D I/ Dt) where L is self-inductance or simply inductance, or choke ... – PowerPoint PPT presentation

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Title: Induced emf and Magnetic Flux F


1
Induced emf and Magnetic Flux F
  • Faraday found that induced emf is produced by a
    changing magnetic field
  • Constant magnetic field, B, induced NO emf
  • Magnetic flux in weber, FB BA cos q
  • 1 Wb 1 T-m2
  • Faradays Law of Induction E -N(D FB/ Dt)
  • Lenzs Law An induced emf always gives rise to a
    current whose magnetic field opposes the original
    change in flux

2
emf Induced in a Moving Conductor
  • Faradays law E -D FB/ Dt B DA/ Dt Blv
  • A changing magnetic flux produces an electric
    field
  • E F/q qvB/q vB
  • AC generator is based on Faradays law. It is
    also called a dynamo or an electric generator
  • E Blv NBAw sin wt where w 2pf
  • A DC generator is like an ac generator except the
    slip rings are replaced by split-ring commutators
  • Cars use ac generators or alternators
  • Counter emf or back emf is a result of Lenz law
  • Opposing the change in B, eddy currents are
    produced

3
Transformers and power transmission
  • A transformer consists of two coils primary and
    secondary
  • Transformer equation I Vs / Vp Ns / Np
  • Ns gt Np produces a step-up transformer
  • Ns lt Np produces a step-down transformer
  • Transformer equation II Is / Ip Np / Ns
  • Transformers help power transmission
  • Microphones use the principle of induction
  • During recording, the audio or video signal
    voltage is sent to the recording head, acting
    like an electromagnet. Playback is opposite to
    recording

4
Mutual Inductance and LR Circuit
  • E1 -M(D I2/ Dt) and E2 -M(D I1/ Dt) where M
    is mutual inductance
  • The unit for M is henry, H. 1 H 1 W-s
  • For a single coil, E -L(D I/ Dt) where L is
    self-inductance or simply inductance, or choke
  • The energy stored in a magnetic field U ½ LI2
  • The energy density in a magnetic field, u ½
    B2/mo
  • In a LR circuit, I (V/R) (1- e-t/t) where t
    L/R is the time constant
  • Imax V/R and I Imax e-t/t

5
AC Circuits and Impedance
  • I Io cos 2pft Irms Io/sqrt 2 and Vrms
    Vo/sqrt 2
  • For a resistor, both current and voltage are in
    phase
  • In an inductor, the current lags the voltage by
    90o
  • V IXL and XL 2pfL is the inductive reactance
  • In a capacitor, the current leads the voltage by
    90o
  • V IXC and XC 1/2pfC is the capacitive
    reactance
  • Only R (not C or L) dissipates energy
  • LRC series ac circuit V Vo cos(2pft f)
    voltage out of phase with current by f cos f is
    the power factor
  • Vrms IrmsZ or Vo IoZ and tan f (XL-XC)/R
  • Z sqrt R2 (XL XC)2 sqrt R2 (2pfL -
    1/2pfC)2

6
Resonance and Oscillators
  • Resonant freq of the circuit, fo 1/(2p) sqrt
    (1/LC)
  • An LC circuit oscillates and is used as an
    oscillator
  • Maximum power is transmitted when the output
    impedance of one device equals the input
    impedance of the secondimpedance matching
  • Sometimes, a transformer is used to alter an
    impedance
  • Zp/Zs VpIs/VsIp (Np/Ns)2
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