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PHYS122

  • L1-24: PINHOLE TV CAMERA

    L1-24
    Demonstrate a pinhole "image" using a TV camera.
    A pinhole of either 0.032 inch or 0.020 inch is positioned on the front of a TV camera, replacing the lens. The resulting image on the videcon of the TV camera is a "pinhole image." Change pinholes to vary the resolution of the image. It can be used with other objects as long as they are well lighted.
    L1, OF4

    l1-24a

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  • L2-06 MAGIC TRICK - DISAPPEARING RABBIT

    L2-06
    Plane-mirror magic trick


    A box has been divided diagonally by a flat mirror. A hatch in the top lets a toy rabbit be dropped in to the space behind the mirror.
    Engagement Suggestion
    • • The box is first shown to the group. Then the black cloth is placed over the front of the box, the trap door on top of the box opened, and the rabbit put into the box through the trap door.
    • • Invite students to predict what they will see when the cloth is removed.
    • • When the black cloth is removed the rabbit has vanished into thin air (behind the mirror).
    • • Challenge then to analyze how this has happened
    • • Explain the positioning of the mirror, and invite them to consider what it would look like with the mirror at different angles.
    Background
    Because the mirror is mounted at a 45 degree angle, it reflects the bottom of the box to look like the rear of the box. So viewed from the front, the box appears empty. This is a common technique for creating such illusions.
    L2
  • L2-23: MIRROR BOX

    L2-23
    Use a half-silvered mirror in a weird way.

    The large box has holes in each end for people to insert their heads, and a half-silvered mirror in the middle. A special variac has been wired so that when the knob is turned lights in each end of the box change intensity with one getting brighter while the other gets dimmer, and vice versa. Each viewer will see a metamorphosis of his or her face to that of the person on the other side. This device was made by an art student as a class project and donated to the Lecture-Demonstration Facility.

    A second hole in one end allows the action to be viewed by a video camera and displayed for the entire class, as seen in the photographs below.

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  • L3-03 LARGE CONVEX MIRROR (60cm)

    L3-03
    Shows the image from a convex mirror
    Just observe your image in the mirror. Note that this type of mirror is used in stores, school buses, and other commercial applications. Because it produces an erect and small image, it can be used as the right hand rear view mirror in a car to see over several lanes of traffic. Because the image is smaller and therefore looks farther away, rear view mirrors carry the warning "Objects in this mirror are closer than they appear."
    OS8
  • L3-14 LARGE CONCAVE MIRROR (60cm)

    L3-14
    Shows types of images from a concave mirror
    Observe and describe the image of the class sitting in front of the mirror when the mirror is at a reasonably large distance away (inverted, small, real). Ask your students if they have this kind of mirror at home. After they say no, hold the mirror close to your face an let them view the image by turning your back to the class, producing an upright, large, virtual image.
    OS8

    geo

  • L3-19 PENNY AND PARABOLIC MIRRORS

    L3-19
    Classic illusion of penny levitating above a pair of parabolic concave mirrors
    This commercial apparatus forms a real image of a penny glued to the bottom mirror. Two concave parabolic mirrors with the correct focal length and spacing create an image of the penny levitating on the opening of the upper mirror. The illusion can be viewed within a limited angle, so it is most effective for individual observation. A ray drawing is included which shows how the image is produced.

    Invite students to place their hand through the image, to get a feel (or not) for what's happening. Have them consider where such images might be used.

    L3
  • L3-31 GIANT 160cm MIRROR - CONCAVE AND CONVEX

    L3-31
    Demonstrates images from concave and convex mirrors
    This five-foot diameter, 132cm (252-inch) radius of curvature parabolic mirror was originally designed as a solar collector on a satellite. Both convex and concave sides can be used with large classes or individually.

    Students can stand in front of the concave side at different distances to find the focal point. Invite students to predict the orientation of the image they see at different points, then try it out.

    FS0
  • L4-03 REFRACTION - ROD IN WATER

    L4-03
    Demonstrates refraction
    The rod, inserted into the water tank and viewed from an angle, shows a discontinuity at the surface of the water. Insert the other end of the rod at an angle into the water; the rod looks bent when viewed at an angle.

    Invite different students to view the tank from different angles and draw what the rod looks like. Have them compare their experiences and discuss.

    L4
  • L4-06 REFRACTION IN CLOUDY WATER

    L4-06
    Demonstrates a light ray bends when it enters a different medium at an oblique angle.
    The ray from the laser refracts when entering the surface of the cloudy water. The path of the laser beam in the water may be rendered more visible by adding a touch of powdered creamer to the water.
  • L4-31 DISAPPEARANCE OF GLASS IN LIQUID

    L4-31
    Demonstrates how index of refraction affects what wesee in a fluid bath
    Glass seems to disappear when immersed in a liquid with the same index of refraction. The bottles, left to right, contain air, water, and two with microscope immersion oil, a liquid with almost the same index of refraction as glass. In the immersion oil, the glass shaft is almost invisible! An air bubble moving up and down in the shaft takes on an odd appearance, as it will be constrained by the shaft but will appear to be moving in free space.

    A video camera is optionally available to make this more visible in large lecture halls.

    L4
  • L5-13: PLEXIGLASS SPIRAL WITH LASER

    L5-13
    Demonstrate total internal reflection with laser light.
    Due to total internal reflection the light from the laser remains mostly confined within the spiral plexiglass rod, and only exits at the end, where the angle between the surface and the incoming light exceeds the critical angle. Actually, some light escapes at scratches along the spiral, as can be seen in the photograph.
    L5, OM1
  • L5-14: LASER AND PLEXIGLASS TUBE

    L5-14
    Demonstrates total internal reflection
    The laser beam enters the plastic tube at a cutout along the top edge, and follows around the tube while spiralling downward
  • L6-08: REAL IMAGE OF CONVERGING LENS - LIGHT BULB

    L6-08
    Show the real image of a converging lens.
    An incandescent bulb with printing on the top is used as an object to be imaged with lenses of different focal lengths. Hold the lens above the light bulb at a distance slightly greater than the focal length of the lens to cast an image of the trademark onto the ceiling. Change lenses to change the magnification. (10cm and 20cm focal length lenses tend to work best in most rooms, but 5cm, 30cm, and possibly others can also be available upon request.)
    OM1, LS1
  • L6-12 MAGNIFYING LENS IN WATER

    L6-12
    Shows that focal properties of a lens depend on the medium in which the lens is located
    A small fuse box is mounted on a holder at a distance less than the focal length behind a convex lens, so the lens acts as a magnifying glass. Note, in the photo at the left, the magnification of the fuse box when the system is in air. Then dip the entire lens-object system into water. Because there is much less bending of the light at the water-glass interfaces than at the air-glass interfaces, the magnification is much less
    L6, L4

    geo

  • M1-11 LASER DIFFRACTION - FIXED DOUBLE SLITS

    M1-11
    Demonstrates double slit interference

    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.
    Background

    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 compadre.org: https://www.compadre.org/Physlets/optics/prob37_7.cfm 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: https://phet.colorado.edu/sims/cheerpj/quantum-wave-interference/latest/quantum-wave-interference.html Use the button on the right to activate the double slit barrier.
    FS1
  • M1-41: PEACOCK FEATHER

    M1-41
    Demonstrate a type of iridescence.
    Iridescence is created by the interference of light, here due to scattering of the light off a series of equally-spaced steps in the structure of the feather. The color can be seen to result from interference by observing that the hue (wavelength) changes as you view the feather from slightly different angles, as can be seen in the close-up views below.

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  • M1-42: IRIDESCENT GREEN JUNE BEETLE

    M1-42
    Demonstrate a type of iridescence.
    Iridescence is created by the interference of light, here due to scattering of the light off a series of equally-spaced steps in the structure of the beetle shell. The color can be seen to result from interference by observing that the hue (wavelength) changes as you view the beetle from slightly different angles.
  • M2-03: LASER DIFFRACTION - POISSON'S BRIGHT SPOT

    M2-03
    Demonstrate the Poisson (or Arago) bright spot.

    This is one of the keystone experiments in establishing light as a wave (rather than particles). The laser beam is expanded to around 4 cm diameter and passed around a 1 inch ball bearing which is suspended between two pointed rods. The diffraction pattern with its central bright spot is viewed on a distant screen. In the photograph at the left above the alignment of the ball in the expanded laser beam can be seen on the screen. In the photograph at the right the Poisson bright spot is seen on a ground glass screen about twenty feet from the laser, looking back toward the laser beam. This picture can be displayed on a video monitor or using a video projector.

    There is a fascinating story about the origin of this experiment, referenced from Eugene Hecht, Optics (Second Edition) and a the web site Fresnel Diffraction, written by Dean Dauger:

    In 1818, Augustin Fresnel submitted a paper on the theory of diffraction for a competition sponsored by the French Academy. His theory represented light as a wave, as opposed to a bombardment of hard little particles, which was the subject of a debate that lasted since Newton's day. Siméon Poisson, a member of the judging committee for the competition, was very critical of the wave theory of light. Using Fresnel's theory, Poisson deduced the seemingly absurd prediction that a bright spot should appear behind a circular obstruction, a prediction he felt was the last nail in the coffin for Fresnel's theory. However, Dominique Arago, another member of the judging committee, almost immediately verified the spot experimentally. Fresnel won the competition, and, although it may be more appropriate to call it "the Spot of Arago," the spot goes down in history with the name "Poisson's bright spot" like a curse.

    Note that the alignment of this system can be delicate and time-consuming; it is not recommended to combine with with other demonstrations using the same laser in a single 50-minute lecture.

    m2-03a

     

  • M3-01 MICHELSON INTERFEROMETER - LASER LIGHT

    M3-01
    Shows laser light fringes using a Michelson interferometer
    This experiment uses the laser and white light combination Michelson interferometer setup. The laser light is expanded by a 2 cm focal length convex lens and reflected into the interferometer by a front surface plane mirror. Either circular or straight line fringes can be displayed by adjusting the tilting mirror. The light exiting the interferometer is focused onto a distant screen, providing a field about one foot in diameter, clearly visible over the entire lecture hall.
    FS1
  • M6-01: HOLOGRAM - LASER LIGHT - VOLKSWAGEN

    M6-01
    View a laser light hologram.
    The hologram, in the form of a slowly rotating cylinder, is illuminated from inside as illustrated by either a white light with a red plastic filter (photograph in center) or a laser light scattered by a piece of wax paper (photograph at right). The laser light renders better resolution of the hologram details, but this is obscured in the photograph by the laser speckle.
    M6, LS1

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