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

### From inside the book

Results 1-3 of 37

Page 48

|—Water vapor —

vapor, are here shown coexisting in equilibrium at some specified temperature.

The pressure exerted by the vapor then has a unique value which depends only

on ...

|—Water vapor —

**Liquid**water Fig. 1.38**Liquid**water and its gas form, watervapor, are here shown coexisting in equilibrium at some specified temperature.

The pressure exerted by the vapor then has a unique value which depends only

on ...

Page 297

Phase transformations of a simple substance As already mentioned, simple

substances are capable of existing in phases of three types: solid,

. (There may also be several solid phases with different crystal structures.) ...

Phase transformations of a simple substance As already mentioned, simple

substances are capable of existing in phases of three types: solid,

**liquid**, and gas. (There may also be several solid phases with different crystal structures.) ...

Page 311

7.11 Attainment of low temperatures by pumping on a

at a temperature To (4.2°K) when its vapor pressure is equal topo, where po = 1

atmosphere or 760 mm of mercury. The latent heat of vaporization per mole of the

...

7.11 Attainment of low temperatures by pumping on a

**liquid Liquid**helium boilsat a temperature To (4.2°K) when its vapor pressure is equal topo, where po = 1

atmosphere or 760 mm of mercury. The latent heat of vaporization per mole of the

...

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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