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Polarization

  • M7-33: DEPOLARIZATION BY SCATTERING - WAX PAPER

    M7-33
    Demonstrate how scattering can depolarize light.
    This demonstration uses the system of goose neck lamp and two rotating polaroids from demonstration M7-03 POLAROIDS AND GOOSENECK LAMP. Rotating the upper polaroid verifies the transverse nature of the light. A sheet of wax paper, placed between the crossed polaroids as shown above, depolarizes the light so that the field cannot be made dark by rotating either polaroid. This also demonstrates that it is not optical activity.
  • M7-34: ROTATION OF POLARIZATION - POLAROID AND WAX PAPER

    M7-34
    Demonstrate two ways to change the polarization of light.
    Light from a goose neck lamp passes through two polaroids to the observer. Crossing the polaroids stops light from reaching the observer. Inserting a third polaroid at an angle between the two crossed polaroids allows light to pass (above left). That light can be stopped by rotating one of the other polaroids, demonstrating the component of a component of the vector electric field. Inserting a sheet of wax paper between the crossed polaroids causes a large amount of random depolarization due to multiple scattering (above right). Rotating either of the originally crossed polaroids cannot stop the light, demonstrating that the depolarization by scattering is not a coherent process.

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  • M7-41: SCATTERING OF LASER BEAM

    M7-41
    Show scattering of light.
    Spritz chalk dust around to see a laser beam. Please be temperate.
  • M8-01 POLAROIDS AND KARO SYRUP

    M8-01
    Demonstration of an optical cavity
    Place a glass bottle of Karo syrup between two crossed polaroids lighted from behind, then rotate one of the polaroids. The second polarizing sheet removes a small band around one wavelength of light, to produce negative colors.
    M8, M7, LS1

  • M8-02: OPTICAL ACTIVITY - GLASS IN KARO SYRUP TANK

    M8-02
    Exotic demonstration of optical activity.

    A trapezoidal tank, lit from behind by polarized light from a rotating polarizer, contains various examples of optically active materials, including stressed glass. As the rear polaroid rotates a fixed polaroid on the front of the tank makes the patterns visible. Click your mouse on the photograph above to see a short mpeg video clip of the setup in motion.

    This is a wonderful hallway demonstration.

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  • M8-04: OPTICAL ACTIVITY IN KARO SYRUP TANK

    M8-04
    Show rotation of the plane of polarization of white light in a uniform tank of Karo syrup.
    Polarized white light enters the end of the tank of Karo syrup. The light which is scattered out in the horizontal plane so that we can see it, as in the photograph, shows a series of subtractive colors, indicating that some spectral color - the one scattered vertically - is missing. Viewed from the top, one sees a somewhat different sequence of colors which are complementary colors to those viewed in the horizontal plane. This demonstrates that the plane of polarization of the light is rotated by an amount which is dependent on wavelength. The two photographs above are close-ups of the tube with the polaroid aligned vertically and horizontally.

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  • M8-05: POLAROIDS AND KARO SYRUP - SPECTRUM

    M8-05
    Demonstrate explicitly that the angle of rotation of polarized light in an optically active medium is a function of wavelength.

    The prism spectrum part of the experiment consists of a bright point source with condenser lens and iris, a 20 cm focal length cylindrical convex lens which focuses light onto a slit, and a 20 cm focal length spherical lens which focuses the light passing through a prism onto a distant screen. After the spectrum is aligned, the optical activity arrangement, consisting of a uniform plastic cylinder of Karo syrup between two rotatable polaroids, can be positioned between the cylindrical lens and the slit, as seen in the photograph. As either polaroid is rotated a dark band moves through the spectrum, because the polaroid absorbs the color/wavelength that has rotated by that angle.

    The color of the light passing through the polaroid/Karo syrup system is a series of negative colors: white minus the color removed by the polaroids. The spectra are shown above (left to right): white light, cyan (minus red), magenta (minus green), and yellow (minus blue) respectively.

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  • M8-06: SUGAR SOLUTION IN TUBE - BARBER POLE

    M8-06
    Demonstrate rotation of the plane of polarization of light.
    White light from a bright point source is polarized and propagated along a tube containing a sugar solution somewhat less dense than Karo syrup. The color seen by observers in the horizontal plane changes much like a barber pole effect. Because more of the blue light is scattered out of the tank, the color gets more redish toward the far end of the tube.

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  • M8-11: OPTICAL ACTIVITY - ROSE AND BUTTERFLY

    M8-11
    Demonstration of classical optically active trinkets.
    Standard Cenco-Bracewell specimens of an optically active rose and butterfly are viewed between two rotatable polaroids. A lens after the second polaroid focuses the image of the optically active specimen onto a screen for visibility by the class.

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  • M8-12: POLARIZED COLOR SLIDE SET

    M8-12
    Fancy artistic demonstration of optical activity.
    Any slide containing birefringent material (such as cellophane, mylar, split iceland spar, ephidrine crystal, ammonium chloride, citric acid, and many others) can be used to show various shapes in beautiful blinking colors, even though it has no color at all when viewed in normal light. To achieve this effect, polarizing material is placed (on the slide) between the condensing lens of the projector and the birefringent material. Then a polarizing disc (analyzer) is rotated in front of the projection lens. (description from Edmund Scientific.)

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  • M8-13: POLAGE

    M8-13
    Art using optically active materials.
    The above art work contains the following layers, from rear to front: a fluorescent light, a rotating polaroid, a diffuser, a collage of optically active materials, and a polarized sheet. The POLAGE consists of the collage and the polaroid sheet mounted together. When the rear polaroid rotates, the picture changes between a butterfly and a cocoon (as shown in the photographs above), while the caterpiller at the lower right changes color.
  • M8-14: PHOTOELASTICITY

    M8-14
    Demonstrate photoelasticity in plastic.
    The system of mounted rotating polaroids in front of a goose neck lamp is used with various stress samples for this demonstration. Rotating either polaroid shows how polaroids work. With the two polarizers crossed, a U-shaped piece of plastic is held between the two crossed polaroids (left) and squeezed at its ends to produce stress patterns (right) with varied colors and intensities. A plastic sheet (provided) can be stretched or a McDonald's plastic salad bar container stressed during manufacture (also provided) can be positioned between the polaroids to show similar patterns.

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  • M8-21: CALCITE BIREFRINGENCE

    M8-21
    Demonstrate birefringence in a calcite crystal.
    Light from a bright point source passes through an object (a letter F in a baffle), a calcite crystal, and a lens, which focusses the F onto a distant screen. The calcite crystal can be rotated in its baffle to show separation of the two polarization components. The rotatable polaroid is inserted into the beam between the calcite crystal and the lens to demonstrate that the two component images are orthogonally polarized. The sequence of photographs above shows the two polarized images and both combined with the polaroid at an angle between the ordinary and the extraordinary ray planes.

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  • M8-22: NICOL PRISM

    M8-22
    Show polarization by the classic Nicol prism.
    A Nicol prism, formed by a cut calcite crystal, uses total internal reflection of one of the two polarization components to achieve polarization of a light beam. The object (a letter F in a baffle) is focused by a lens onto a distant screen, with the Nicol prism between the object and the lens. Polarization can be verified by rotating either the Nicol prism or the polaroid, which is between the Nicol prism and the lens in the photograph.

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  • M8-31: LIQUID CRYSTALS

    M8-31
    Show various liquid crystals for individual viewing.
    Several sheets of encapsulated liquid crystal are provided, with a wide range of critical temeratures for color changes. Descriptive literature is included. Best for individual use.
  • M9-02: CIRCULAR POLARIZATION - ROTATING VECTOR MODEL

    M9-02
    Model a circularly polarized wave
    The vector moves along as it rotates, simulating the advance of a circularly polarized electromagnetic wave.
  • M9-03: CIRCULAR POLARIZATION - STICK MODEL

    m9-03
    Model of circularly polarized electromagnetic wave.
    Sticks emanating from a central rod create a model of a circularly polarized electromagnetic wave, as the wave is moved through space at the speed of light by the instructor.
    FS1
  • M9-11: MICROWAVES - ELLIPTICAL POLARIZATION

    m9-11
    Show properties of an elliptically polarized microwave beam.
    A dipole antenna with a spiral shape can produce an elliptically or circularly polarized microwave beam. Any orientation of the receiving antenna yields the same signal, as seen in the photographs below, taken at angles of 0, 45, and 90 degrees respectively with respect to the vertical. (See Demonstration M7-01: MICROWAVES - POLARIZATION for the case of a linearly polarized wave. The elliptically polarized wave will be picked up by the receiving antenna in either vertical or horizontal orientation.

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  • M9-21: QUARTER WAVE PLATE

    m9-21
    Show properties of a quarter-wave plate.

    Light from a bright point source with condenser and iris passes through a yellow filter and two crossed polaroids onto a distant screen. The quarter-wave plate is then positioned between the two crossed polaroids and rotated to any angle except 45 degrees with respect to the crossed polaroids. When the analyzer is rotated periodic minima and maxima of illumination appear on the screen, because the beam is elliptically polarized, and no position of the analyzer will produce darkness. When the polarizer and analyzer are crossed and the quarter-wave plate is set at 45 degrees, rotating the analyzer does not produce any changes in the intensity of the beam. This is the effect of circular polarization.

    Note that the yellow filter is used because the thickness of the quarter wave plate is based on the wavelength of yellow light.

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  • M9-22: HALF WAVE PLATE

    m9-22
    Show properties of a half-wave plate.

    Light from a bright point source with condenser and iris passes through a yellow filter and two crossed polaroids onto a distant screen. The half-wave plate, consisting of two identical quarter-wave plates, is then positioned between the two crossed polaroids at the angle which produces the greatest illumination on the screen. Remove the plate and cross the polaroids. The half-wave plate is then inserted set at the angle for darkness. The plate is rotated somewhat less than 45 degrees, producing some light. The analyzer must be rotated by twice the angle of the plate rotation to again produce darkness.

    The quarter wave plates have thickness chosen for yellow light.

    Polarization

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