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Atomic Physics

  • P3-22: CATHODE RAY TUBE - CANAL RAYS

    p3-22
    Demonstrate canal rays present in a cathode ray tube.
    Perforations in the cathode of the tube permit positive ions to pass through the cathode, forming "canal rays" or "positive rays." The effect of a magnet on these rays may be compared with its effect on electrons moving in the opposite direction as in demonstration K1-12: CATHODE RAY TUBE - DEFLECTION BY MAGNET. The deflections of the beam are visible if viewed closely with very low ambient light level.
  • P3-23: CATHODE RAY TUBE - FLUORESCENCE EFFECT

    p3-23
    Demonstrate fluorescence in a cathode ray tube.
    A group of minerals which fluoresce with different colors when irradiated with electrons are in the base of the tube. It's not overwhelming, but it's nice.
  • P3-24: CATHODE RAY TUBES - MISCELLANEOUS

    p3-24
    Illustrate various types of discharge tubes.
    This demonstration includes several gas discharge tubes of various shapes. This demonstration can be used in conjunction with other gas discharge demonstrations from P3 or N1 to demonstrate the variety of forms these effects can take. The wiring is exposed for visibility, so please handle with care.
    Connect the power supply to one discharge tube at a time to see it discharge. Connect to common wire at left and run one tube at a time by choosing its connector on the right.
  • P3-25: CATHODE RAY TUBE - CONCAVE CATHODE

    p3-25
    Show what happens in a discharge tube as the pressure is changed.
    Turn the pump on and off for brief periods to vary the pressure while observing the effect on the discharge. A gauge on the pump reads the pressure.
  • P3-31: X-RAY TUBE

    p3-31
    Classic x-ray tube.

    Move detector around x-ray tube to show that x-rays come out preferentially in the forward direction. Ask for absorbers if you wish. Looking at the close-up photograph at the right above, electrons originate from the electrode at the upper right and strike the anode from its right side, producing x-rays that move preferentially to the right from the cathode.

    Note: This demonstration is rather touchy to set up to actually obtain x-rays. It is available largely so that the geometry of such a tube can be seen by the students.

    Atomic Physics

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  • P3-41: FRANCK-HERTZ EXPERIMENT

    p3-41
    Demonstrate that the bound electrons in an atom can only occupy discrete energy levels, by determining the quantum of energy such an electron can absorb.
    The oven heats the Franck-Hertz tube so that the mercury in the tube becomes a vapor and diffuses uniformly throughout the tube. The cathode filament provides a source of electrons which are accelerated through a variable potential to a perforated anode grid. While the electrons are being accelerated, they collide with the mercury atoms. Some electrons will pass through the grid, encountering a retarding potential until they reach the electrode. The current from the electrode is measured by the picoammeter and displayed using a slave meter on the overhead projector. The electron current can be plotted as a function of the accelerating voltage, indicating the energy levels of the mercury electrons. The circuit along with the accelerating voltage and anode current are displayed on the overhead projector, shown in the photograph at the right.

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  • P3-51 BALMER SERIES

    P3-51
    Observe the Balmer series in hydrogen
    The discharge tube provides an electrical discharge through low-pressure hydrogen, resulting in the characteristic hydrogen spectrum. The Balmer series of lines is visible. The spectrum can be observed using hand-held holographic diffraction gratings in small classrooms. Due to brightness limitations, the spectrum will be shown using a video camera and rear projection TV in the lecture halls, using a holographic grating taped to the lens of the TV camera.
    N2
  • P3-52: RESONANCE RADIATION

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    Show resonance radiation of iodine.
    A glass sphere containing iodine vapor is illuminated by a bright point source, and characteristic radiation can be seen as scattered light. The light scattered (absorbed and re-emitted) by the iodine vapor is desaturated yellow-green, and the light passing through the sphere is a desaturated pink, the complementary color.
  • P3-53: ATOMIC ENERGY LEVEL MODEL

    p3-53
    Model of energy levels in the atom.
    This model has four levels with the appropriate number of electrons for each level: 2, 8, 8, then 18 for the top level. The spacing between each higher level is less, as in the actual electron energy level spacing. In the photograph above, the first level is filled, the second level has three electrons, and one electron has been excited into the next level; this would represent a carbon atom in its lowest excited state.
    FS1
  • P3-54: ENERGY LEVELS - BALLS AND LADDER

    p3-54
    Model energy levels in atomic orbits.
    The steps of the ladder represent energy levels or atomic orbitals. The ball represents an electron. Electrons moving between energy levels can be modeled by balls on different steps of the ladder.

    Optionally, a light source can be provided with different coulour filters. The light source provides a photon of energy. With a red filter the ball jumps one step; with the blue filter the electron jumps two or three steps up the ladder. Radiation with the wrong light, say green light, leaves the ball in its ground state (on the floor), because that energy would leave the ball between energy levels. Invite students to make predictions about the results of different colours of light/different amounts of absorbed energy.

  • P3-61: FLUORESCENT LIQUIDS

    p3-61
    Show fluorescence of different chemicals.

    A set of liquid vials containing fluorescent materials is illuminated by an ultraviolet light source. The radiation is absorbed by the chemicals and emitted at a visible frequency, causing them to glow. Identification of the chemical is printed above each vial. The bottle at the right contains quinine water. It's almost enough to make you give up drinking quinine water.

    The second photograph was taken with normal fluorescent lighting.

    P3

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  • P3-62: FLUORESCENT CHALK

    p3-62
    Demonstrate fluorescence in different materials.
    Colored chalk is doped with various fluorescent chemicals so that when illuminated by ultraviolet light it glows brightly. Write on the blackboard with different colors, then make them come alive with a black light.
    P3
  • P3-63: WAVE LENGTH SHIFTER BAR

    p3-63
    Demonstrate how a wave length shifter bar absorbs photons and re-emits the energy at its characteristic wavelength.

    The spectrum of a carbon arc lamp, projected onto a screen, contains both visible and ultraviolet radiation. A wavelength shifter bar is a plastic material containing a fluorescent chemical, fluorescien. Insert the wave length shifter bar into the spectrum with light coming out the curved end aimed at the class for easier observation. For wavelengths greater than green, the spectral color is observed (red, orange, yellow). For shorter wavelengths, the chemical in the bar absorbs the incident light but re-emits that energy as green light, the characteristic color of the chemical in the plastic tube.

    Use the wave length shifter bar to demonstrate the existence of ultraviolet radiation in the spectrum of the carbon arc lamp.

    P3

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  • P3-64: PHOSPHORESCENCE - BLACK LIGHT AND OSCILLOSCOPE CRT

    p3-64
    Demonstrate phosphorescence.
    An ultraviolet light illuminates the face of an oscilloscope tube, causing it to glow a bright green color. When the black light is removed, the tube screen still glows, demonstrating its phosphorescence. This effect is important in avoiding flickering when an oscilloscope, TV set, or computer monitor is viewed.
    P3
    Atomic Physics

    p3-64

     

  • P3-65: WINTERGREEN MINTS

    p3-65
    To demonstrate that breaking wintergreen mints creates small flashes of light.

    Wintergreen mints are smashed IN A DARK ROOM between two glass plates, as pictured above, or by biting into one. When the mint breaks, a small flash of bluish light is produced.

    When a sugar crystal in the mint is broken, it is often separated into two sections with different charges, creating a potential difference. If enough crystals are fractured simultaneously, the potential becomes large enough to cause electrons in the structure to be repulsed from one region and attracted to another. In transit, these electrons strike other electrons in nitrogen molecules in the air, raising the atomic electrons to excited states. When the electrons decay they emit ultraviolet radiation that strikes molecules of methyl salicylate flavoring in the wintergreen mint. These molecules of methyl salicylate flavoring absorb the UV radiation and re-emit it as the blue light observed when the mint fractures.

    Instructor must provide mints.

    P3
  • P3-66: FLUORESENCE AT LN TEMPERATURE

    p3-66
    Demonstrate fluorescence of a normal material at LN temperature.
    The material does not fluoresce at room temperature. When cooled to the temperature of liquid nitrogen it will fluoresce when illuminated with ultraviolet light. The figures above show the material (a) at room temperature, (b) at LN temperature with room lights on, and (c) at LN temperature with room lights off.
    P3, I0

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                               (a)                                                       (b)                                                         (c)

  • P3-67: FLUORESCENCE OF LAUNDRY SOAP

    p3-67
    Demonstrate that laundry soap is fluorescent.
    Fluorescent chemicals are typically added to laundry soap to make white clothing appear "whiter and brighter." In the presence of even a small amount of UV, the fluorescence due to the residual chemical remaining after the clothes are rinsed is sufficient to cause white shirts, socks, or T-shirts to have a blue/white glow. Soap manufacturers would like consumers to believe that their soaps are actually making the whites "whiter."
    P3
  • P3-71: VISIBLE LASER

    P3-71
    See the inside of a laser, observe the spectrum of light
    The case has been removed from a HeNe laser and has been replaced by a clear plastic tube, so that the optical parts can be seen. A flat white tab has been installed at the end so that the light leaving the laser strikes the tab. Using hand-held diffraction gratings, the spectrum of the light inside and outside the laser tube can be seen, allowing observation of the optical effect of the lasing action. The light inside the tube can be seen through a series of slits along the tube's length. The single wavelength of light in the external beam can be seen as the red dot on the top of the spectra above.
    P3
  • P4-11 RADIOACTIVE DECAY - DICE

    P4-11
    Illustrates the radioactive decay of a sample of nuclei. Shows how a half-life is determined
    Thirty dice with holes along one axis represent radioactive nuclei. When the dice are rolled on the overhead projector, a certain number will have the hole showing, meaning that they have decayed. They are collected and placed on a transparency graph showing how the sample would decay theoretically. The remaining dice are rolled, and the decayed nuclei placed on the graph in the next horizontal location. The procedure is repeated until every die has decayed. The "half life" is the number of times the dice must be thrown until only half are left, where each throw represents a certain fixed time interval. If you want to get real fancy, you can make use of the fact that you actually expect one-third of the dice to decay in any throw.
    P4
  • P4-41: RUTHERFORD SCATTERING MODEL

    P4-41
    Show difference in scattering from the Thompson and Rutherford models of the nucleus.
    Small ball bearings representing alpha particles roll down an inclined groove to gain kinetic energy, then pass through representations of either Thompsons model (center) of the nucleus or Rutherford's model (right) of the nucleus. The angle of the track or the starting position for the balls can be adjusted to change the energy of the alpha particles.

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