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WAVE OPTICS AND OPTICAL INSTRUMENTS

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Title: WAVE OPTICS AND OPTICAL INSTRUMENTS


1
WAVE OPTICS AND OPTICAL INSTRUMENTS
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  • Understanding how these rainbows are made and how
    certain scientific intruments can determine
    wavelength is the domain of wave optics.
  • Light can able viewed as either a particle or a
    wave.
  • The three primary topics we examine are
    interference, diffraction and polarization.

4
The Interference of Light
  • Two waves could add together either
    constructively or destructively
  • In constructive interference- the amplitude of
    the resultant wave is greater than that of
    independent waves
  • In destructive interference- the resultant
    amplitude is less than that of either individual
    waves
  • Conditions for interference
  • 1. The sources must be coherent, which means the
    waves they emit must maintain a constant phase
    with respect to each other
  • 2. The waves must have identical wavelengths
    (monochromatic)

5
Youngs Double-Slit Experiment
  • The light from the two slits produces a visible
    pattern on screen consisting of a series of
    bright and dark parallel bands called fringes

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  • The light intensity on the screen at P is the
    result of light from both slits
  • A light from the lower slit, travels further then
    the light from the upper slit, the path
    difference
  • d(s) r2-r1 d sin ?

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  • Condition for constructive interference (for
    bright fringes) dd sin ?bright m?
  • Condition for destructive interference (for dark
    fringes) dd sin ?dark (m ½)?
  • m0, 1, 2. . . order number

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  • m 0, the first bright fringe at ?bright0 is
    called zeroth-order maximum
  • m1 is called first-order maximum
  • m0, the path difference d?/2 condition of
    location of the first dark fringe on either side
    of the central (bright maximum)
  • m1 , d3?/2 condition for the second dark
    fringe on either side
  • Position of the bright fringes
  • ybright(?L /d) m
  • Position of the dark fringes
  • ydark(?L /d)(m½)
  • m 0, 1, 2,

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Interference in thin films
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  • 1. An electromagnetic wave traveling from a
    medium of index of refraction n1 toward a medium
    of refraction n2 undergoes a 180o phase change on
    reflection when n2gtn1, there is no phase change
    in the reflected wave if n2ltn1
  • The wavelength of light ?n in a medium with index
    of refraction n is ?n ?/n
  • where ? is the wavelength of light in vacuum

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  • If 2t ?n /2, then rays 1 and 2 recombine in
    phase and constructive interference results
  • Condition for constructive interference in thin
    films
  • 2t(m½) ?n
  • m 0, 1, 2,
  • 2nt(m½) ? (1)

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  • The general equation for destructoive
    interference in thin films is
  • 2 n t m ? (2)
  • m 0, 1, 2,

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  • Equation (1) and (2) for constructive and
    destructive interference are valid when there is
    only one phase reversal (when the media above and
    below the thin film both have indices of
    refraction greater (respectively less) than the
    film
  • If the film is placed between two different
    media, one of lower refractive index than the
    film and one of higher refractive index, equation
    (1) and (2) are reversed
  • 2nt(m½) ? destructive
  • 2 n t m ? - constructive

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Diffraction
  • Diffraction the spreading out of light from its
    initial line of travel

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Single Slit Diffraction
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  • sin ? darkm ?/d
  • m 1, 2, 3,
  • This equation gives the values of ? for which the
    diffraction pattern has zero intensity, where a
    dark fringe form

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The Diffraction Grating
  • The condition of maxima in the interference
    pattern at the angle ? is
  • d sin ?bright m?
  • m0, 1, 2,
  • Diffraction grating is use in CD tracking

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Polarization of Light Waves
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Polarizing by Reflection
  • ?p90o?2180o
  • ?290o-?p sin?2sin(90o-?p)cos?p
  • nsin?1/sin?2sin?p/sin?2sin?p/cos?ptan?p
    -Brewsters Law
  • ?p?B- Brewsters angle

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Optical instruments
  • The Eye
  • The Power P of a lens in diopters is
  • P1/f
  • Ex
  • f20cm, P5
  • f-40cm, P -2.5

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  • The simple magnifier
  • Angular magnification mß/a
  • tanah/25 tanßh/p
  • mmaxß/a(h/p)/(h/25)125/f
  • If q8, than pf, m25/f

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  • The Compound Microscope
  • The overall magnification of the compound
    microscope mM1 me-L/fo(25cm/fe)
  • M1 lateral magnification (-q1/p1-L/fo)
  • me- angular magnification(25cm/fe)of the
    eyepiece for an object (corresponding to the
    image at q1)placed at the focal point

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  • The Telescope
  • m a/ß (h/fe)/(h/fo)fo/fe

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