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PHYS260

  • I1-13 THERMAL EXPANSION - BIMETAL STRIP

    I1-13
    Demonstrates differential thermal expansion

    Two strips of different metals, invar steel and brass, are welded together to form a bimetal strip. Since each metal has a different coefficient of thermal expansion, heating the bimetal strip will result in the metals expanding at different rates, causing it to bend.

    When heating, always wear goggles and handle the flame with care, ensuring that it is not pointed near students or flammable materials. Use in a well ventilated classroom.

    Engagement Suggestion
    Ask your students: • Which metal will expand more when it is heated, and why?
    • What happens when it is cooled?
    • How could you make use of this to measure or control something?
    Background

    The amount a metal expands or contracts with temperature is governed by its coefficient of thermal expansion, a property which varies between different metals depending on their molecular structure. Invar steel is an alloy designed to have an exceptionally low coefficient, about one-tenth that of most steel, while brass has a higher coefficient than even ordinary steel. So the brass expands much more rapidly than the steel does when heated.

    Bimetallic strips like this are used in some types of thermometers and thermostatic controllers (including many older window thermometers and household thermostats). Check out demonstrations I1-17 and I1-18 for examples and to see how this works.

    I1, I0
  • I1-22: WATER DENSITY VS TEMPERATURE

    I1-22
    Demonstrate the change in the density of water with temperature.

    A calibrated thin spherical metal shell with air and shot inside sinks in water at approximately 115-120 degrees F. The water is then cooled by a fan, whereupon the sphere rises to the top of the water when a temperature of about 100-110 degrees F is reached (this cooling can take up to 15 minutes depending on room temperature and humidity).

    The water can be stirred continually to keep the temperature uniform using the digital thermometer probe, which simultaneously reads the temperature, which is displayed on a large scale. If the sphere starts out floating and is sunk by heating the water, the demonstration requires more time due to surface tension.

    I0, I1
  • I2-04 WIEN'S LAW OF THERMAL RADIATION

    I2-04
    Shows that higher temperature blackbodies radiate with shorter wavelengths

    A variable transformer, or Variac, is connected to two identical incandescent light bulbs in parallel. These bulbs are viewed behind red and blue filters respectively. As the voltage is increased by the variac, the lights glow more brightly, and more light is seen through the blue filter relative to that of the red filter. Very little or no blue is seen at low voltages, whereas red is seen to be emitted even at very low voltages.

    Engagement Suggestion:
    • Ask students to compare this to other phenomena that emit light. Where else do you se this change of color with temperature?
    Background:

    Wilhelm Wien postulated in the 1890s that the power curve of blackbody radiation from an object could be computed from its temperature. His original calculations, obviously, did not take quantization into account; in modern practice, the revised calculations are still commonly referred to as Wien's Law.

    Note that this apparatus only works with incandescent lightbulbs. Fluorescent and LED bulbs do not produce their primary light through thermal excitation, and thus don't produce the same kind of blackbody spectrum.

    I2, PS1
  • I2-08 RADIATIVE HEAT TRANSFER

    I2-08
    Shows radiation from a hot object
    As more voltage is applied to the heater it glows more brightly and emits more heat
    I2, PW1
  • I2-21 THERMAL CONDUCTIVITY IN METALS

    I2-21
    Demonstrates thermal conductivity in various metals
    Heat from a gas burner at the center is conducted along rods of copper, aluminum, and brass. Wax blocks at the ends of the rods melt and drop off the rods due to the conduction of heat, in the following order: copper (3.98 Watts/cm deg C), aluminum (2.37 Watts/cm deg C), and brass (1.23 Watts/cm deg C).
    I2, I0
  • I2-24: THERMAL CONDUCTIVITY IN WATER

    I2-24
    Demonstrate that water is a poor conductor of heat.
    An immersion heater placed at the top of a dewar of water causes the water near the top of the dewar to boil. However, heat is not readily conducted through the water to the bottom, and the bottom remains at a much lower temperature even 15-20 minutes after the water on top begins to boil.
  • I2-27: THERMAL EQUILIBRIUM BETWEEN ALUMINUM AND COPPER

    I2-27
    Show process of thermal equilibrium happening between touching aluminum and copper cylinders.
    Pieces of copper and aluminum are held together by a large C-clamp. Small holes are drilled into the pieces to a allow a digital thermometer probe to be inserted to measure the temperature of each block, showing that the blocks are initially the same temperature, at equilibrium. Remove the thermometer probes and put a flame under one block to create a temperature difference. Remove the flame, reinsert the probes, and watch as the blocks come to thermal equilibrium.
    I2, I0, tools
  • I2-28: WATER BALLOON AND CANDLE

    I2-28
    To demonstrate the transfer of heat by water
    A balloon filled with water is held above a candle flame. Contrary to most students' expectations, the balloon does not burst. The water in the balloon conducts heat away from the rubber before it can melt.
    I0
  • I3-14: MAGDEBURG HEMISPHERES

    I3-14
    Demonstrate force arising from the atmospheric pressure of air.
    A mechanical pump is used to evacuate the air from inside a pair of sealed hemispheres. Ropes on the two hemispheres allow two groups of students to attempt to pull the hemispheres apart against the force produced by the atmospheric air pressure. The hemispheres have a diameter of about 5 inches, thus requiring a force of over 250 pounds to separate them when fully evacuated. A safety restraint holds the two hemispheres so that if the pressure releases they will not separate entirely. Three students pulling on each rope may be able to separate the hemispheres.
    FS1
  • I3-20: COLLAPSE OF CAN - LARGE CAN WITH MALLET

    I3-20
    Demonstrate collapse of a can by atmospheric pressure.
    The air is removed from a large coffee can by a vacuum pump, as seen in the photograph above. The can is then given a strong smack with a large hard rubber mallet, causing it to unseat from the vacuum seal and to collapse with a rather large bang. The resultant coffee can is shown in the photograph at the right.
    FS1, OS9, tools

    i3-20a

  • I3-33 HELIUM BALLOON ON LIQUID NITROGEN

    I3-33
    Demonstrates how a gas contracts when cooled
    A helium balloon which is cooled by resting on a liquid nitrogen bath becomes becomes more dense -- by about a factor of 4. When the balloon is removed from the liquid nitrogen it warms up, expands, and floats away, unless it is tethered
    I0, FS1

    I3-33A

  • I3-41: BOYLE'S LAW - PROJECTION

    I3-41
    Demonstrate Boyle's law.
    Connect the piston tube to the pressure gauge. Read off several values of pressure and volume for different piston positions to show that PV=constant.
    I3

    i3-41ai3-41b

  • I3-51 CHARLES' LAW - PROJECTION

    I3-51
    Demonstrates Charles' law
    A hollow sphere filled with air is connected by a tube to a pressure gauge on an overhead projector. Place the sphere in ice water (T=273K) and in boiling water (T=373K), and read the pressure for each as well as at room temperature.
    I3, I0
  • I4-03: LATENT HEAT - ICE TO WATER TO STEAM

    I4-03
    Show latent heat as ice is transformed to water and then to steam.
    A flask is filled to within one inch of the brim with a mixture of water and ice cubes at the freezing temperature of water. The flask is then heated for about 15 to 20 minutes with the burner on high, with the temperature measured by the dial thermometer. If you were to create a plot of temperature as a function of time, it would clearly show that extra heat is required to produce the ice-water and water-steam phase transitions.
    I0
  • I4-11: BOILING AT REDUCED PRESSURE

    I4-11
    Demonstrate that water boils at a lower temperature under reduced pressure.
    Water is boiled in the flask, then heat is removed and the flask is sealed after boiling ceases. Dry ice is packed around the flask, reducing the pressure inside the flask. The boiling immediately resumes.
    I4, I0
  • I4-15 CONDENSATION OF STEAM - GALLON CAN COLLAPSE

    I4-15
    Illustrates forces produced by the pressure drop when steam condenses into water
    A small amount of water in the can is heated with the lid off, filling the can with steam. The can is then removed from the hot plate and the lid quickly screwed tightly thereon. Within a few seconds the steam begins to condense, creating a low pressure inside the can. The greater atmospheric pressure outside crushes the can.
    I0, SU14
  • I4-17: AIR BALLOON ON LIQUID NITROGEN

    I4-17
    Demonstrate dramatically that the volume of vapor is greater than the volume of the same amount of liquid.
    An air balloon is held on top of a liquid nitrogen bath. The volume of the air balloon decreases for two reasons: first, the volume of the gas shrinks according to Charles' law, and second, some of the air changes to liquid and shrinks considerably. Liquid nitrogen will readily cause oxygen to liquify, and even liquify some of the nitrogen in the balloon.
    I0

    i4-17a

  • I4-19: CONDENSATION OF STEAM - SODA CAN COLLAPSE

    I4-19
    Surprising demonstration using condensation of steam.
    A soda can with a small amount of water in the bottom is heated until the water boils, filling the can with steam. Very quickly the can is removed from the heater and inserted upside down into a container of cold water. The steam condenses so quickly that the can collapses, as seen in the photograph. This is quite a dramatic demonstration, and gets a good reaction from students.
    I4, I0, SU15
  • I4-32: FREEZING WATER BY PUMPING

    I4-32
    Freeze water by reducing the ambient pressure.
    Place about four drops of water onto a cellophane "watchglass" in the vacuum chamber as in the photograph at the left. Evacuate the chamber with the vacuum pump. Almost immediately the water will begin to bubble (boil), as seen in the middle photograph below, and within about one minute the boiling will subside and the water will freeze. When the water freezes it is clearly seen to become opaque on the overhead projector screen, as seen in the photograph on the right below. This is a very dramatic demonstration.
    I4, I0

    i4-32ai4-32bi4-32c

  • I5-01 MECHANICAL EQUIVALENT OF HEAT - SHOT BAG

    I5-01
    Demonstrates that heat can be produced from mechanical work
    The temperature of lead shot in a shot bag is measured with the digital thermometer. The shot bag is then beat on the floor about ten times, and the temperature measured once again. The work done in beating the shot bag on the floor has been converted to heat. Not very much heat though: use the tenth degree scale for quicker results!
    I5, I0, tools