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Today’s agenda: Review of Waves. You are expected to recall facts about waves from Physics 1135.

Today’s agenda: Review of Waves. You are expected to recall facts about waves from Physics 1135. Young’s Double Slit Experiment. You must understand how the double slit experiment produces an interference pattern. Conditions for Interference in the Double Slit Experiment.

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Today’s agenda: Review of Waves. You are expected to recall facts about waves from Physics 1135.

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  1. Today’s agenda: Review of Waves. You are expected to recall facts about waves from Physics 1135. Young’s Double Slit Experiment. You must understand how the double slit experiment produces an interference pattern. Conditions for Interference in the Double Slit Experiment. You must be able to calculate the conditions for constructive and destructive interference in the double slit experiment. Intensity in the Double Slit Experiment. You must be able to calculate intensities in the double slit experiment.

  2. Conditions for Interference Sources must be monochromatic-of a single wavelength. Sources must be coherent-- must maintain a constant phase with respect to each other. Here’s the geometry I will use in succeeding diagrams.

  3. For an infinitely distant* screen: L1 L1 y  S1 L2    d d P L2 L L= L2 –L1 = d sin S2 *so that all the angles labeled  are approximately equal R

  4. Constructive Interference: L1   d Destructive Interference: L2 L= L2 –L1 = d sin The parameter m is called the order of the interference fringe. The central bright fringe at  = 0 (m = 0) is known as the zeroth-order maximum. The first maximum on either side (m = ±1) is called the first-order maximum.

  5. For small angles: L1 Bright fringes: y  S1 L2  d P L S2 This is not a starting equation! R Do not use the small-angle approximation unless it is valid!

  6. For small angles: L1 Dark fringes: y  S1 L2  d P L S2 This is not a starting equation! R Do not use the small-angle approximation unless it is valid!

  7. L1 y  S1 L2  P L S2 R Example: a viewing screen is separated from the double-slit source by 1.2 m. The distance between the two slits is 0.030 mm. The second-order bright fringe (m = 2) is 4.5 cm from the center line. Determine the wavelength of the light. Bright fringes: d

  8. L1 y  S1 L2  P L S2 R Example: a viewing screen is separated from the double-slit source by 1.2 m. The distance between the two slits is 0.030 mm. The second-order bright fringe (m = 2) is 4.5 cm from the center line. Find the distance between adjacent bright fringes. Bright fringes: d

  9. L1 y  S1 L2  P L S2 R Example: a viewing screen is separated from the double-slit source by 1.2 m. The distance between the two slits is 0.030 mm. The second-order bright fringe (m = 2) is 4.5 cm from the center line. Find the width of the bright fringes. Define the bright fringe width to be the distance between two adjacent destructive minima. d

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