**P260 Demos T.L.
Einstein Spring 2015**

Chap. 15

**I3-16: COLLAPSE OF CAN - LARGE PUMP**

I3-14
MAGDEBURG HEMISPHERES

Chap. 16

**I1-01: THERMOMETERS **

**I3-52: CONSTANT VOLUME GAS THERMOMETER - ABSOLUTE ZERO **

With a constant volume of air in the chamber, measure the pressure P(B) at the boiling point and the pressure P(F) at the freezing point of water. If the pressure P is read at some arbitrary temperature T, then that temperature in degrees celsius is:

T=100 [P-P(F)] / [P(B)-P(F)]

For an ideal gas, the pressure should go to zero at the temperature of absolute zero. Setting P=0, the value of absolute zero in degrees celcius can be calculated.

Another way to do this is to plot a graph of pressure as a function of temperature. Draw the best line through the three points determined at boiling, freezing, and room temperature, and extend it so that it intersects the pressure axis, which is T=0 in celsius degrees.

I4-01: PVT PHASE DIAGRAMS FOR CO2 AND H2O

I3-31: IDEAL GAS LAW - VOLUME OF ONE MOLE

I3-04: GALILEAN THERMOMETER

Chap. 17

I2-22 THERMODYNAMICS BY TOUCH

I2-44: CONVECTION - CANDLE IN CYLINDER

P2-21 BLACK BODY MODEL

Chap. 18

I6-03 EQUIPARTITION OF ENERGY

I6-33: MOLECULAR MOTION DEMO - GAS PRESSURE

I6-34: MOLECULAR MOTION DEMO - TEMPERATURE OF A GAS