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    Physics 1051

    Lecture 24

    Electromagnetic Waves

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    Recommended Problems

    Fishbane, Chapter 34, Problems 7,10,14,16,21,24,30

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    The story so far

    So far we have talked about oscillations and waves,

    electric forces and fields, and magnetic forces and

    fields.

    In the next couple of lectures we use all of this

    material to develop a description ofelectromagnetic

    waves.

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    What do we know about

    electricity and magnetism? Charged particles produce electric fields

    Moving charges produce magnetic fields

    Electric fields cause a force on a charged particle

    Magnetic fields cause a force on moving charges

    particles

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    What do we know about

    electricity and magnetism? The electric flux through a closed surface is

    proportional to the charge inside the surface

    (Gausss Law).

    This says that electric fields are due to electric

    charges. Electric field lines begin and end atcharges. We can use it to show that the electric

    field of a point charge is proportional to 1/r2.

    0

    Q E dA

    I !

    &&

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    What do we know about

    electricity and magnetism? The magnetic flux through a closed surface is zero.

    This says that there are no magnetic monopoles,

    and that magnetic field lines have no beginning or

    end.

    0B

    dA !

    &&

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    What do we know about

    electricity and magnetism? Integrating the magnetic field around a closed path gives a

    result that is proportional to the current enclosed by the

    path. (Ampres Law)

    This says that magnetic fields are caused by currents.

    There is another part to this that we have not discussed:Magnetic fields can also be caused by changing electric

    fields. Including this mathematically would give us another

    term on the rhs that included the time derivative of a surface

    integral of the electric field. I will spare you the details.

    0 encB ds IQ !& &

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    What do we know about

    electricity and magnetism? Changed in magnetic flux cause an induced emf.

    (Faradays Law).

    This says that changing magnetic fields produce an

    electric potential, or in other words changing

    magnetic fields produce an electric field.

    surface

    d

    dt

    d E ds B dA

    dt

    I *!

    ! && &&

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    What do we know about

    electricity and magnetism? These laws show that there is a strong connection

    between electricity and magnetism. In factelectricity and magnetism are two aspects of thesame phenomenon, which we can callelectromagnetism.

    The electric and magnetic fields are coupled theydepend on each other.

    In a vacuum, if we have no electric charges and noelectric currents, then the equations weve writtendown above are perfectlysymmetric with respect to

    Eand B. This means thatEand Bbehave the same.

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    Maxwells Equations

    The equations weve written down here are a form of

    Maxwells Equations.

    Maxwell saw that all of these electromagnetic

    phenomena could be described in a single

    mathematical framework.

    The solution to Maxwells equations in a vacuum

    turns out to be traveling waves

    both the electric andmagnetic field propagate through space in the form of

    waves.

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    Electromagnetic Waves

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    0

    0

    ( , ) sin

    ( , ) sin

    E r t E kx t

    B r t B kx t

    [

    [

    !

    !

    & &&

    & &&

    k!2T

    P

    [ !2T

    T

    ! 2Tf

    The plane wave solutions to Maxwells Equations have the

    following form

    where E0 and B0 are theamplitudes of the electric and

    magnetic components of the wave.

    kis the wave number of the electromagnetic waves. (Really it

    should be a vector pointing in the direction of propagation ofthe wave.)

    k! wave number

    P = wave length

    f ! frequency

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    Maxwells equations tell us several things:

    The electric and magnetic fields propagate as traveling

    waves

    These waves travel at the speed of light. The speed of the

    waves is given by

    The electric and magnetic fields are always perpendicular to

    each other.

    The amplitudes of the fields are also related:

    0 0

    1v c

    Q I! !

    0 0 0E B !

    & &

    E cB!

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    Electromagnetic Waves

    Maxwells equations, published in 1864, had far reaching

    consequences. They showed in detail how electricity and

    magnetism were connected. Maxwells equations predicted the

    existence of electromagnetic waves, which traveled with the

    speed of light. Maxwell conjectured that light was a form ofelectromagnetic radiation.

    In 1887 Heinrich Hertz

    produced radio waves and

    from the measured frequency

    and wavelength confirmed

    Maxwells conjecture.

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    Electromagnetic Spectrum

    Radio Waves

    Microwaves

    Infrared

    Visible light

    Ultraviolet

    X-rays Gamma rays

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    Example 1

    Fishbane, Chapter34, Problem 5

    If the electric field for a plane electromagnetic wave

    is given by

    what are and the direction of propagation of the

    wave?

    0

    0

    cos( )

    x

    y

    E

    E E kz t [

    !

    !

    B&

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    Example 2

    Fishbane, Chapter34, Problem 61.

    Use dimensional analysis to show that

    has the dimensions of speed.

    0 0

    1

    Q I

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    Electromagnetic Energy

    Electromagnetic waves carry energy and can transport

    energy from one place to another. The energy carried

    by an electromagnetic waves is shared equallybetween the magnetic field part of the wave and the

    electric field part of the wave. The average value of

    the total energy density in the wave is

    220 0

    0

    0

    1

    2 2

    Eu B

    I

    Q! !

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    Intensity and Energy Transport

    c

    c

    x

    R

    Since electromagnetic fields

    represent a form of energy,

    and electromagnetic waves

    propagate through space, then

    electromagnetic waves

    transport energy.

    Consider a segment of acircular beam of circular light

    of radius R. How much

    energy is transported across a

    surface in time (t?

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    Electromagnetic Energy

    The power per unit area delivered by an

    electromagentic wave to a surface perpendicular to the

    direction of propagation is

    This is called the intensity of the em wave.

    220 0 0 0

    0

    0 02 2 2

    c E EBc I cu B

    I

    Q Q! ! ! !

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    Example

    The intensity of sunlight on the

    earths surface is approximately

    1 kW/m2.

    Calculate the energy density of

    sunlight at the earths surface.

    Estimate the amplitude of the

    electric and magnetic fields of

    the sunlight striking the earth.

    u !I

    c

    !10

    3

    3v

    10

    8 J m-3

    ! 3.3v106 J m-3

    I! uc

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    u }I0E0

    2

    2

    To calculate the amplitude of

    the electric field we use the

    relation

    E}2u

    I0

    }2 v 3.3 v106

    8.85v1012V m

    -1

    } 864 V m -1

    Thus we obtain

    E0

    B0

    ! c

    To calculate the amplitude of

    the magnetic field we use the

    relation

    B0 !E0

    c

    ! 8643v108

    T

    ! 2.87 v106 T

    Thus we obtain

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    Example 3

    A typical laser pointer has a power of around 0.5 mW

    and a beam width of around 1mm.

    Calculate the intensity of the beam.

    Calculate the amplitude of the electric and magnetic

    fields of the beam.

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    Production of EM Waves

    Electromagnetic waves

    are produced by creating

    an oscillating electric or

    magnetic field.

    Charges oscillating in a

    linear antenna will produce

    an oscillating electric field.

    An oscillating electric field

    will produce an oscillating

    magnetic field.

    This produces a wave which

    travels away from the source

    with the speed of light.

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    There are other types of

    antenna. For example the loop

    antenna, uses an oscillating

    current to produce a oscillating

    magnetic field.