## Statistical Physics, Volume 5Elementary college physics course for students majoring in science and engineering. |

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Results 1-3 of 13

Page 131

the heat given off by the system and is given by – Q. Thus we can write Q = AE

and Q = AE' (49) for the heat Q absorbed ... Two systems are said to be

energy ...

the heat given off by the system and is given by – Q. Thus we can write Q = AE

and Q = AE' (49) for the heat Q absorbed ... Two systems are said to be

**thermally****insulated**or adiabatically isolated from each other if they cannot exchangeenergy ...

Page 132

Panel (c) shows a final equilibrium situation which might result if the magnetic

field is changed from B to B1 in some arbitrary way; the work done in the

particular case shown here is W = –0.4MoR1 + 0.8poB. to be

from each ...

Panel (c) shows a final equilibrium situation which might result if the magnetic

field is changed from B to B1 in some arbitrary way; the work done in the

particular case shown here is W = –0.4MoR1 + 0.8poB. to be

**thermally insulated**from each ...

Page 200

5.3 Work, Internal Energy, and Heat The concepts of heat and work were

introduced in Sec. 3.7. ... When the system is not

absorbed by it can be determined by (13) if one makes use of the information

previously ...

5.3 Work, Internal Energy, and Heat The concepts of heat and work were

introduced in Sec. 3.7. ... When the system is not

**thermally insulated**, the heat Qabsorbed by it can be determined by (13) if one makes use of the information

previously ...

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### Contents

Characteristic Features of Macroscopic Systems | 1 |

A I | 2 |

I | 6 |

Copyright | |

26 other sections not shown

### Common terms and phrases

absolute temperature absorbed accessible approximation assume atoms average Avogadro's calculate classical collision Consider constant container corresponding cules denote discussion distribution ensemble entropy equal equilibrium situation equipartition theorem example exchange energy expression external parameters fluctuations function given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy interval isolated system kinetic energy large number left half liquid ln Q macroscopic parameters macroscopic system macrostate magnetic field magnetic moment magnitude mass mean energy mean number mean pressure mean value measured mechanics mole molecular momentum number of molecules occur oscillator particle particular partition phase space piston position possible values Prob quantity quantum numbers quasi-static random relation result simply solid specific heat spin system statistical statistical ensemble statistically independent Suppose thermal contact thermal interaction thermally insulated thermometer tion total energy total magnetic total number unit volume velocity