Lecture15 Polarization

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    Chapter 24

    ElectromagneticWaves

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    24.6 Polarization

    A transverse wave is linearly polarized

    when its vibrations always occur along

    one direction.

    A linearly polarized wave on a rope

    canpass through a slit that is parallel

    to the direction of the rope vibrations.

    The rope wave cannotpass througha slit that is perpendicular tothe

    vibrations.

    POLARIZED ELECTROMAGNETIC WAVES

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    24.6 Polarization

    In polarized light, the electric field

    of the electromagnetic wave fluctuates

    along a single direction.

    Unpolarized lightconsists of short

    bursts of electromagnetic waves emitted

    by many different atoms. The electricfield directions of these bursts are

    perpendicular to the direction of wave

    travel, as in polarized light, but are

    distributed randomly about it.

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    24.6 Polarization

    Polarized light may be produced from unpolarized light with the aid of

    polarizing material.

    The intensity of the transmitted polarized light has 1/2 the intensity of

    the incident unpolarized light (perpendicular component blocked).

    The transmission axis of the material is the direction of polarization

    of the light that passes through the material.

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    24.6 Polarization

    MALUS

    LAW !2

    coso

    SS =

    intensity beforeanalyzer

    intensity after

    analyzer

    Consider two sheets of polarizing material, one to polarize unpolarized light

    (Polarizer) and one at an angle !to the polarized light (Analyzer). The

    intensity of the light after the analyzer is related to the intensity before the

    analyzer by Malus

    Law:

    ( Intensity ~ E2)

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    24.6 Polarization

    Example 7 Using Polarizers and Analyzers

    What value of !should be used so the average intensity of the polarized

    light reaching the photocell is one-tenththe average intensity of the

    unpolarized light?

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    24.6 Polarization

    !2

    5

    1cos=

    5

    1cos =! !

    4.63=!

    Applying MalusLaw at the Analyzer: S= S0,polarcos2!

    But S0,polar= (1/2)S0 and we want S= (1/10)S0

    So (1/10)S0= (1/2)S0cos2

    !

    S0 S0,polar S

    ! !

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    24.6 Polarization

    Conceptual Example 8 How Can a Crossed Polarizer and

    Analyzer Transmit Light?

    Suppose that a third piece of polarizing material is inserted between the

    crossed polarizer and analyzer. Does light now reach the photocell?

    S0 S1 S2 S3

    S1= S0/2

    S2= S1cos2!

    = (S0/2) cos2!

    S3= S2cos2(90 - !)

    = (S0/2) cos2!sin2!

    Clearly, S3> 0 as long as

    !!0 or 90o

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    24.6 Polarization

    Polarized light is produced by the scattering of unpolarized

    sunlight by molecules in the atmosphere.

    Molecules re-radiate sunlight.

    As you look at larger and larger

    angles with respect to the

    incident sunlight, the re-radiated

    light becomes more and more

    horizontally polarized.

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    Polaroid Sun Glasses

    Besides sunlight re-radiated from atmospheric molecules, there are

    other sources of horizontally polarizedlight that occur in nature, such

    as sunlight reflected from horizontal surfaces such as lakes.

    Polaroid sun glassestake advantage of this fact by using polarizers

    with their axes oriented vertically:

    !in addition to 1/2 of the unpolarized light which is already blocked by

    the polarizers, all of the horizontally polarized light is completely blocked,

    thus blocking out some of the reflected light which can confuse you

    during some outdoor activities (e.g. driving, piloting, fishing!!.).

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    24.6 Polarization

    IMAX movie projector Movie viewer using polarized glasses

    Another application using polarized glasses: watching 3-D movies.

    In a 3-D movie, two separate rolls of film are projected using a projectorwith two lenses, each with its own polarizer. The two polarizers are

    crossed. Viewers watch the action on-screen through glasses that have

    correspondingly crossed polarizers for each eye.

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    Example. Partially polarized and partially unpolarized light.

    A light beam passes through a polarizer whose transmission axis makes

    angle !with the vertical. The beam is partially polarized and

    partially unpolarized, and the average intensity of the incident light,

    S0, is the sum of the average intensity of the polarized light, S0,polar,

    and the average intensity of the unpolarized light, S0,unpolar.

    As the polarizer is rotated clockwise, the intensity of the transmitted light

    has a minimum value of 2.0 W/m2when != 20.0oand has a maximum

    value of 8.0 W/m2when the angle is != !max.

    !Find a) S0,unpolar, and b) S0,polar.

    Incident light

    S0= S0,polar+ S0,unpolar

    Transmitted light

    S= Spolar+ Sunpolar

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    Incident lightS0= S0,polar+ S0,unpolarTransmitted lightS= Spolar+ Sunpolar

    a) Minimum transmitted intensity S= Smin= 2.0 W/m2at != 20.0o.

    Sis minimum when Spolar= 0 since Sunpolaris not effected by !.

    Sunpolar= Smin- Spolar= 2.0 - 0 = 2.0 W/m2

    Sunpolar= (1/2)S0,unpolar ! S0,unpolar= 2Sunpolar= 2(2.0) = 4.0 W/m2

    b) Maximum transmitted intensity S= Smax= 8.0 W/m2occurs at !max.

    Sis maximum when Spolar= S0,polar(when != 20o+ 90o= 110o= !max)

    Smax= S0,polar+ Sunpolor!S0,polar= Smax- Sunpolar= 8.0 - 2.0 = 6.0 W/m2