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Properties of Matter

  • F2-41: DENSITY - SLOPE OF MASS VS VOLUME GRAPH

    F2-41
    Determine the density of water.
    Starting with the container empty, pour in water a small amount at a time and plot the total mass vs. the volume of water in the container. The slope of the graph is the mass density of water.
  • F3-21: SURFACE TENSION - ALCOHOL AND WATER IN SAND

    F3-21
    Illustrate the difference between the surface tension in water and in alcohol.
    One jar contains sand with water. The bottle has been tamped so that the sand grains have become aligned with very small cracks between them. The surface tension of the water will not allow the water to flow into these very small volumes. When the jar is squeezed, the cracks open up sufficiently to allow the water to flow into them, thus causing the water in the tube to fall.

    A second jar contains sand with alcohol. Because alcohol has a much smaller surface tension than water, the alcohol will flow into the small cracks between sand grains, filling the space. When the alcohol bottle is squeezed, the volume is already filled with sand and liquid, so the alcohol level in the tube must rise.

  • G1-31: HOOKE'S LAW AND SHM

    G1-31
    Quantitatively demonstrate how the spring constant affects the period of a mass on a spring.
    Determine the spring constant from the relationship F=kx using various numbers of 200 gram weights hanging from the spring. Hang groups of 200 gram weights from the spring and create vertical oscillations, obtaining the period using the manual timer. Compare with the period calculated from the relation T = 2 pi SQRT (m/k), where k was obtained above. This can be compared with actual integration of the equations of motion using a computer if desired.
    FS1, ME1
  • H1-23: SPEED OF SOUND IN ALUMINUM

    H1-23
    Compare the measured and the theoretical values of the speed of sound in aluminum.
    An aluminum rod is stroked (See Demonstration H3-71: STROKED ALUMINUM ROD.), setting up longitudinal standing waves in the rod. The frequency f is determined using a frequency meter, with or without the aid of an audio oscillator. The length L of the rod, one-half wavelength for the fundamental, is measured using a two-meter rule. The speed of sound in aluminum is then S = 2fL. The theoretical value is obtained by using the Young's modulus Y and the mass density d: S = SQRT(Y/d), where the Young's modulus Y=7.0x10^+10 Pa and density of aluminum d=2.699x10^+3 kg/m^3. Putting in numbers, S = SQRT(Y/d) = 5,093 m/s. For the first mode of the stroked rod, the wavelength is twice the length of the rod, so measuring the length of the rod L = 1.83m, and the frequency of the first mode f = 1370 Hz, the speed of sound in aluminum is S = 2fL = 5,014 m/s.
  • H6-04: HELIUM VOICE

    H6-04
    Demonstrate the rise in frequency of vocal formants due to the increase in the speed of sound in a light gas.
    Inhale a small quantity of helium and talk and sing normally. Your voice takes on a squeaky "Donald Duck" character due to the increase in frequency of your vocal formants.

    This demonstration has the potential to be dangerous if misused, and must only be used after instruction by Lecture-Demonstration personnel. The purpose of this demonstration is to illustrate the effect of vocal formants, not as entertainment for groups where the physics content is not discussed. Take a couple of big breaths of air first to get plenty of oxygen, then breath out completely before inhaling the helium. Videos of this effect may be more useful in many classes.

    H6, FS1
  • I1-32: RUBBER BAND CONTRACTION DURING HEATING

    I1-32
    Demonstrate that rubber contracts when heated.
    A 200 gram mass hangs from a rubber band which is connected to a rigid support. Using the heat gun, apply heat to the entire length of the rubber band by aiming the heat gun up the tube, causing the rubber band to contract and pull up the weight.
    I1, I0, FS2

    i1-32a

  • I3-12: WATER BAROMETER - CAN CRUSHER

    I3-12
    Illustrate a result of atmospheric pressure.
    A rectangular can, connected to a long rubber hose, is filled with water from a large reservoir. The can is then raised about 15 feet, keeping the end of the hose in the water reservoir. The pressure differential between the inside and the outside of the can crushes the can as the water runs out in about 30 seconds. NOTE: Requires a high ceiling!

    i3-12a

  • I3-42: BOYLED MARSHMALLOWS

    I3-42
    Amusing demonstration of Boyle's Law.

    A marshmallow is placed in a bell jar. As the air is pumped out of the jar the pressure inside becomes smaller and the little bubbles of air in the marshmallow increase in size, inflating the marshmallow. Eventually much of the air originally in the marshmallow is pumped away. When the air is let back in, atmospheric pressure compresses the marshmallow to a small fraction of its original size.

    An alternative demonstration uses a balloon with a small amount of air in it in place of the marshmallow. The photographs above show the marshmallow: before pumping, after pumping, and after the air is let back into the bell jar, and the balloon: before pumping and after pumping.

    Please bring own marshmallow.

    I3, FS1

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