Monday, 22 July 2013 10:51


Additional Info

  • ID Code: M1-11
  • Purpose: Demonstrates double slit interference
  • Description:
    A slide containing four sets of double slits is positioned in the laser beam using a slide holder on a cross-carriage mount. Any of the four sets of slides can easily be slid into the beam. The slits are available in two different widths with tow different separations. Challenge your students to predict how the relationship of slit width and slit spacing will affect the interference pattern created.

    Collimated light waves come from the laser and pass through a pair of narrow slits in the slide; the light passes through and then projects on the distant screen. But light travels as an electromagnetic wave, so when the light comes out of the two slits, it forms two wavefronts, just like ripples from two stones dropped in a pond. These two wavefronts can interfere with each other, as we can model with this pair of overlapping concentric circles. Where two peaks or two valleys of the wave pattern line up, they add together, interfering constructively; when a peak and a valley overlap, they cancel out, interfering destructively. The same happens with light waves; the light from the two slits overlaps, and creates a pattern of bright spots (constructive interference) and dark spots (destructive interference). The spacing between the bright and dark fringes ultimately depends on three things: the distance between the slits and the screen, the wavelength of the light, and the spacing between the two slits.

    Two simulations that can be of value in introducing this topic:
    • a ripple tank simulation here in the Physlet Physics collection at AAPT’s Use your mouse to measure the positions of the peaks relative to the double slit at the base of the image.
    • this PhET Simulation at the University of Colorado: Use the button on the right to activate the double slit barrier.
  • Availability: Available
  • Loc codes: FS1
Read 2122 times Last modified on Monday, 21 December 2020 10:18
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