Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 39
... thermometer and will be denoted by the Greek letter 0. For example , the familiar mercury or alcohol ther- mometer is a special example of a thermometer . Here the length L of the column of liquid in the glass capillary tube of the ...
... thermometer and will be denoted by the Greek letter 0. For example , the familiar mercury or alcohol ther- mometer is a special example of a thermometer . Here the length L of the column of liquid in the glass capillary tube of the ...
Page 151
... thermometer ) assumes the same value in both cases . This implies that , after M has come to equilibrium with A , it remains in equilibrium after being placed in thermal contact with B. Hence the zeroth law allows one to conclude that A ...
... thermometer ) assumes the same value in both cases . This implies that , after M has come to equilibrium with A , it remains in equilibrium after being placed in thermal contact with B. Hence the zeroth law allows one to conclude that A ...
Page 217
... thermometer reading is again 5.00 cm . The switch is closed for 3 min , and then opened . After equilibrium has been attained , the thermometer reading is L = 7.52 cm . The switch is then closed again for 3 min before being opened ...
... thermometer reading is again 5.00 cm . The switch is closed for 3 min , and then opened . After equilibrium has been attained , the thermometer reading is L = 7.52 cm . The switch is then closed again for 3 min before being opened ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
9 other sections not shown
Common terms and phrases
absolute temperature absorbed accessible approximation assume atoms average calculate classical collision Consider constant container cules definition denote discussion distribution electron ensemble entropy equal equilibrium situation equipartition theorem example expression external parameters fluctuations fluid function Gibbs free energy given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy isolated system kinetic energy large number left half liquid macroscopic system macrostate magnetic field magnetic moment magnitude mass maximum mean energy mean number mean pressure mean value measured mole molecular momentum n₁ number of molecules occur oscillator particle particular phase phase space piston plane Poisson distribution position possible values Prob probability P(n quantity quantum numbers quasi-static random relation result simply solid specific heat statistical statistical ensemble statistically independent Suppose thermal contact thermally insulated thermometer tion total energy total number unit volume velocity