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    Chapter 32Electromagnetic Waves

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    Is the assumption consistent with

    Faradays Law?

    Consistent only with Faradays Law if the

    wave speed and the magnitudes of the

    perpendicular vectors Eand B are related.!Ea =!Bac It is then valid to say that,

    (Electromagnetic wave

    in vacuum)

    During a time interval dt, the

    wave front moves a distance

    (c)dtto the right sweeping out

    an area (ac)dtof the rectangle.The thus increases

    during the time interval by,!

    B

    d!B =B(ac)dt

    The rate of change of is,!Bd!

    B

    dt=Bac

    E = cB

    !Ed

    !

    l"! = "Ea Does our wave satisfies Amperes Law?

    We move our rectangle so that it lies

    in the xz-plane.We take the vector area dAin the y-direction thus we integrate

    counterclockwise around the

    rectangle.On side ef, Bis zero.

    Only sideghcontributes to the

    integral.

    On side fgand he, Bis either zero or

    perpendicular to dl.

    There is no conduction current so,!Bd

    !

    l"! = 0!0d"

    E

    dt

    !

    Bd!

    l"! =Ba

    Does our wave satisfies Amperes Law?Only sideghcontributes to the integral.

    The left-hand side of Amperes Law is

    non-zero so the right-hand side must

    also be non-zero.Eand Bmust be mutually

    perpendicular.

    It is then valid to say that,(Electromagneticwave in

    vacuum)Obeys Amperes Law only if B, cand Eare

    related.

    !Bd

    !

    l"! =0!0d"

    E

    dt

    !

    Bd!

    l"! =Ba

    In a time interval dt, thethrough the rectangle increases by,!E

    d!E =E(ac)dt

    The rate of change of is,

    !E

    d!E

    dt=Eac

    Ba =0!0Eac

    B =0!0Ec

    Our EM wave must obey both Amperes and

    Faradays Law!

    It will only happen if,

    That is,

    MUST BE SATISFIED!!!B =

    0!0EcE = cB ; B =

    1

    cE

    1c

    =0!0c

    c =

    1

    0!0

    c =1

    8.85!10"12C

    2/ Nm

    2( ) 4!!10"7N/ A2( )= 299, 792, 458m / s

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    Our assumed wave is consistent with all

    Maxwells equations, provided that the wave

    front moves with the SPEED OF LIGHT!!!c = 3.00!10

    8m / s

    Important features of all Electromagnetic Waves:The wave is transverse; both E and B are perpendicular to the

    direction of propagation of the wave. The E and B fields are also

    perpendicular to each other. The direction of propagation is the

    direction of the vector product Ex B.There is a definite ratio between the magnitudes of Eand B: E= cB.The wave travels in vacuum with a definite and unchanging speed. Unlike mechanical waves, which need the oscillating particles of a

    medium such as water or air to transmit a wave, electromagnetic

    waves require no medium. Whats waving in an electromagnetic

    wave are the electric and magnetic fields.

    Sinusoidal Electromagnetic Waves

    Electromagnetic waves produced by an oscillating point charge is an

    example of sinusoidal waves that are not plane waves. The frequency, wavelength and speed of propagation of any periodic wave

    is,c = !f

    E0 ;*( +06;/4B0 ?=

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    A( * 5*;''12 ; B = 0!0EcE = cB

    X 6 S 0 0 + & O ? = 4 ( *

    +40C0;7/4;Y

    E = vB ; B = !Ev

    1

    v

    = !v !1

    v2 =!

    v2=

    1

    !

    ! v =1

    !

    v =

    1

    !m

    0!"

    0

    =

    1

    !m!

    1

    0"0

    =

    c

    !m!

    A( * +40C0;7/4;2

    X4(+0P &O /0O/*;@&(Y

    v =

    c

    !m!

    . & / 1 & 6 7

    +40C0;7/4;2

    !m !1

    v =

    c

    !

    ^0;*'60 46 *C2

    ! vdielectric

    < c 1

    !

    B

    8

    A( &S@;62c

    v

    = n

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