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  • D5-12: CORIOLIS EFFECT - WATER JET

    D5-12
    Model the Coriolis effect.
    Fill the can with water and rotate the entire can-tank assembly on its platform. The water jet exhibits a curved trajectory which is an analog to the curvature of the trajectory of a projectile on earth due to the Coriolis effect.
    OS10
  • D5-13: FOCAULT PENDULUM - MODEL

    D5-13
    Model the Foucault pendulum
    The circular base can be rotated while the pendulum oscillates in a fixed plane in the frame of reference of the laboratory, thus showing the apparent rotation of the plane of the pendulum when viewed in the frame of reference of its base.
    D5, OS10
  • D5-21: BALL ROLLING ON ROTATING DISC

    D5-21
    Show that a sphere rolling on a rotating disc will move in circles.
    The ball can be placed at the center of the rotating disc and tapped to initiate the motion or it can be loosely trapped with your fingers at about half the radius of the disc, and then released. The frequency of the circular motion does not depend on either the radius or the mass of the ball, or on the radius of the orbit, but only on the frequency of the rotating disc.
    OS12
  • D5-22: ROTATING PENDULUM

    D5-22
    Demonstrate the presence of a "critical parameter" which determines the dynamic behavior of a simple physical system.
    Attach a mounting frame to a variable speed rotator with the length of the pendulum of 10 cm. Adjust the rotation rate to less than about 1.6 revolutions per second, and the bob will remain in stable equilibrium in the vertical position. For rotational rates greater than 1.6 revolutions per second, the stable equilibrium position of the bob will be non-zero, depending on the rotation rate. For angular speeds greater than 2 or 3 revolutions per second the pendulum is erratic. For angular speeds less than about 3 revolutions per second the presence of a non-zero stable equilibrium position is readily demonstrated. Adjusting the length of the pendulum will change the critical angular speed.
    D5, D1
  • D5-23: ROTATING BEAD ON LOOP

    D5-23
    Demonstrate the presence of a "critical parameter" which determines the dynamic behavior of a simple physical system.
    Attach the mounting frame to the variable speed rotator and adjust the rotation rate to less than approximately 1.6 revolutions per second. The bead remains in equilibrium at the bottom of the loop. For rotational rates greater than 1.6 revolutions per second, the bead will be in stable equilibrium at a non-zero angle dependent on the rotation rate. Frictional effects are considerable; nevertheless the presence of a critical angular velocity can be seen.
    D5, D1
  • D5-24: ROTATING PENDULA - LENGTH VS. HEIGHT

    D5-24
    Show that pendula of different length suspended from the same point rotating at the same angular speed rise to the same vertical height.
    When the device is rotated at an angular speed w the angle a from the vertical which a pendulum of length l will assume is given by cos a = g / w^2 l, where g is the acceleration of gravity. The vertical distance of each from the support point is l cos a = g / w^2, the same value for each of the pendulum. This can be easily observed using the apparatus.

  • E1-01: CAVENDISH EXPERIMENT - MODEL

    E1-01
    Aid in describing the Cavendish experiment.
    The black (steel) balls are temporarily rigidly fixed in space. A steel barbell is mounted to a stiff wire on the axis of the barbell with a small mirror attached to the wire just above the barbell. Light reflects off the mirror, indicating the oscillations of the barbell. This models how, in the full experiment, the equilibrium position for oscillations of the barbell would show the displacement corresponding to the gravitational force between the two pairs of balls, and is observed by noting the movement of the light reflected off the mirror.
    FS2, LS1
  • E1-12: MARBLE IN GLASS BOWL

    E1-12
    Demonstrate orbits in a gravitational potential well.
    Start the marble rolling tangentially in the bowl to obtain an orbit, then observe the effects of conservation of angular momentum.
    E1, I6
  • E1-21: GRAVITATIONAL LENS OPTICAL MODEL

    E1-21
    Demonstrate optical characteristics of a gravitational lens.

    The lens shown in the top photograph above is a plano-convex lens whose focal characteristics model that of a gravitational lens. The shape of the lens, described in one of the reference articles in the reference list linked below, is seen in the photograph at the right.

    The experimental setup is shown in the second photograph. The distant "star" is formed by a hole in a piece of black paper or foil in front of a light source. The star can be moved by sliding it left-to-right along the optical rail behind the gravitational lens, in the same plane as the observer (video or other camera). Adjusting the height of the camera will put the observer slightly out of the plane of the motion of the star and axis of the gravitational lens. These cases are shown below.

    An mpeg video shows a star passing directly behind the gravitational lens, where the star is represented by a small disc of light. The camera, in the plane of the motion, records the light from the star as the star passes DIRECTLY behind the gravitational lens. The ring of light created when the distant star is EXACTLY in line with the gravitational lens and the observer is called the Einstein ring.

    Another mpeg video shows the situation where the distant star is slightly above the plane of the gravitational lens and the observer.

    This device was designed and produced by physicist Sid Liebes, an expert on gravitation and relativity, and author of several of the reference works, including both the design and application of the lens.

    This additional animated video shows what one might observe when a background galaxy passes on the opposite side of a black hole from the observer.

    E1, OM1, LS1, L6

    e1-21a e1-21b

  • E2-03: CRATER FORMATION MODEL

    E2-03
    Illustrate how a crater forms as a result of an impact or a blast from below.

    Drop a steel ball onto a dish of sand. The ball becomes partially buried and a crater forms.

    Bury the end of the hose in the sand using the plastic strip attached to the end of the hose, and smooth out the sand. Using lung power, blow in a blast of air and notice the crater that forms.

    A generation ago there was a debate among geologists and astronomers as to the origin of lunar and terrestrial craters. This demonstration illustrates two ways in which craters can form.

    E2, LS2

    e2-03a

  • E2-11: SOLAR PLASMA MODEL

    E2-11
    Mass driver and ring heater show coronal holes and coronal heating.
    Hold down the ring to simulate confined plasma in a solar coronal loop; it will heat up much as does the solar plasma. Let the ring go and it will "shoot" away from the AC fields much like the plasma shoots out of coronal hole.
    K2
  • E2-23: UMBRA AND PENUMBRA - EXTENDED SOURCE

    E2-23
    Show umbra and penumbra with an extended source, as in an eclipse.
    Hold the foam ball between the extended source (an incandescent-based television lightbox) and a projection screen (In the lecture halls, use the whiteboard behind the blackboards.). The shadow will consist of three distinct regions: (1) The umbra, in which all of the source is shadowed, is the dark central part. (2) The penumbra, where part of the source is shadowed, is the intermediate band around the umbra. (3) The outer region, where none of the source is shadowed, is the brightest region.
    E2, LS1
  • E2-24: UMBRA AND PENUMBRA - COLOR FILTERS

    E2-24
    Identify the source of penumbra regions.
    Combined red and green filters project nearly white light on a screen. When the foam sphere is inserted between the sources and the screen, the penumbral regions take on the color of the filter through which the light in that region has traveled, because the other color has been blocked by the disc. The umbra, where light from both sources is blocked, is nearly black.
    E2, LS1

    e2-24a

  • E2-36: DENSITY STRATIFICATION - FORMATION OF PLANETS

    E2-36
    Demonstrates how density stratification (differentiation) in interior of planets occurs.
    Heavy balls represent dense material (e. g., iron or nickel). Light balls represent light material (e. g., silicates). Use wooden plank to vigorously mix the balls, then remove the plank and watch heavy balls settle. Mixing simulates the hot molten interior of a young planet. Settling simulates differentiation in molten interior of an older planet.
    E2, P4

    e2-36a

  • E2-43: ROTATING STAR FIELD

    E2-43
    Show the apparent motion of the night sky.
    The star field is painted onto the plate with its pivot passing through the North star.
  • E2-44: BINARY STAR MODEL

    E2-44
    Illustrate the orbital motion of a binary star system.
    This common optical device consists of a hemispherical mirror with a ball hanging at its center of curvature. When the ball is displaced and started into circular motion around the center of curvature, the real image of the ball also moves around the center of curvature on the opposite side of the center of curvature from the actual ball. This would represent the orbits of a binary star system where the masses of the two stars are approximately equal. Owing to the rather ghostly appearance of the image, this model is particularly suitable for illustrating a binary system in which one of the stars (the image) is a black hole.
    L3
  • E2-45: ECLIPSING BINARY STAR MODEL - LIGHTS

    E2-45
    Show how we view a rotating binary star.
    The two bulbs, one with less intensity than the other, are rotated about the axis of the stick. This shows the intensity variation observed for a binary star with two stars of differing brightness.
  • E2-46: ECLIPSING BINARY STAR MODEL - SPHERES

    E2-46
    Illustrate the orbits of stars in an eclipsing binary.
    The model consists of two spheres, each representing a star, which are mounted on the ends of a dowel rod. The rod can be rotated, showing how eclipses can occur and at what period the orbital velocities of the stars can be found.
    E2, FS2
  • E2-47: TWINKLING STAR

    E2-47
    Show how air currents cause the "twinkling" of a star.
    A laser beam is directed on a distant wall or screen. When the heater is positioned below the laser beam, hot air convection currents and density changes cause the beam to move continuously, or "twinkle."
    FS1, I0

    e2-47a

  • E2-48: NON-TWINKLING PLANET

    E2-48
    Illustrate why a planet does not "twinkle" like a star.
    A beam expander enlarges the laser beam to a few inches diameter on a distant wall or screen (photograph below). When a heater is placed under the beam, convection currents are readily visible in the large spot of laser light. However, because the spot is large it does not move, or "twinkle." This is contrasted with the direct light from the laser, which moves because of the convection currents from the heater. A star twinkles because it is so small, but because of the finite size of planets as viewed from the earth, planets do not twinkle.
    FS1, I0

    e2-48a