Key concept in Magnetic Flux

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    Electromagnetic Induction

    Key Concept is Magnetic Flux

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    Faradays Law

    Key Concept is CHANGE in Magnetic Flux

    A CHANGING

    B through any closed loopinduces an EMF around the loop.

    The induced EMF equals the negative of

    the time rate of change of the total magnetic

    flux through the loop

    dt

    d B =

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    Faradays Law

    It doesnt matter why the flux changes

    dt

    d B =

    1) Constant B, Changing Area:

    2) Constant Area, Changing B:

    3) Constant Area, Constant B, Changing Cos :

    ==surface surface

    B cosBdAAdB rr

    where

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    Direction of the Induced EMFs and Currents

    In the previous problem, we found the directionof the induced current by noting that the forceresulting from the induced current had tooppose the applied force. This obbservation canbe generalized into:

    Lenzs Law

    The direction of any magnetic induction effect

    is such as to oppose the cause of the effect

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    The Alternator(see Y&F example 30-4)

    The magnetic field ,and the angular frequency , are constant

    tcosBAcosBAB ==

    By Faradays Law:

    r

    tcosABdt

    d B

    ==

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    The Generator(see Y&F example 30-5)

    The magnetic field ,and the angular frequency , are constant

    tcosBAcosBAB ==

    The split-ring commutator rectifies the EMF:

    r

    tcosABtcosAB ==

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    Direction of the Induced EMFs and Currents

    In the previous problem, we found the directionof the induced current by noting that the forceresulting from the induced current had tooppose the applied force. This obbservation canbe generalized into:

    Lenzs Law

    The direction of any magnetic induction effect

    is such as to oppose the cause of the effect

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    Induced Electric Fields

    nIABA 0B ==

    dt

    dInA

    dt

    d0

    B

    ==

    This seems very mysterious because there isNO magnetic field outside the solenoid and

    therefore there can be NO force on the chargesinside the conducting loop!

    The EMF will induce a current that will be

    indicated by the Galvanometer.

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    Induced Electric Fields

    Faradays Law hold even if there is

    no Motion and no Magnetic Field

    nIABA 0B ==

    dt

    dInA

    dt

    d0

    B

    ==

    Faradays Law implies that there is an

    Induced Electric Field

    = ldErr

    =dt

    dldE B

    rr

    This Induced Electric Field is a

    non-electrostatic field that arises,

    not from static charges, but from a

    changing B field alone.

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    Maxwells Equations

    The equations below summarize all of the

    underlying physics of Electricity and Magnetism

    =0

    enclosedQAdE

    rr

    = 0AdBrr

    += dt

    dildB E0C0

    rr

    = dtd

    ldE Brr

    Gausss Law

    Gausss Law for

    magnetism

    Amperes Law

    Faradays Law

    ( )BvEqFr

    v

    vv

    += Lorentz Force Law

    AND

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    Maxwells Equations in Free Space

    If there are no charges and no currents,

    Maxwells Equations have a very simple andvery symmetric form:

    = 0AdErr

    = 0AdBrr

    dt

    dldB E00

    =

    rr

    = dtd

    ldE Brr

    Note that a changing B will induce an E and

    a changing E will induce a B. This B can in turn induce

    an E, which will induce a B, and so on

    It can be shown that these equations predict the

    existence of a self-sustaining wave that propagates

    with a velocity of:

    00

    1v=

    Experimentally this velocity is found to be exactlyequal to the speed of light.

    All visible light, as well as radio wave,

    microwaves, x-rays, gamma rays, ultraviolet andinfrared radiation are all electromagnetic in origin!

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    Inductance

    Mutual

    Inductance

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    Inductance

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    Inductance

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    How Big is a Henry

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    SELF-INDUCTANCE

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    Circuit Elements