## Fundamentals of statistical and thermal physics |

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Page 157

But, by definition, " > \dT)T Using (5-2-7), this becomes ▻ cp = cv + R (5-2-8)

Thus c, > cy, in general agreement with (4 -4 -7), and these molar specific heats

of an ideal

heats ...

But, by definition, " > \dT)T Using (5-2-7), this becomes ▻ cp = cv + R (5-2-8)

Thus c, > cy, in general agreement with (4 -4 -7), and these molar specific heats

of an ideal

**gas**differ precisely by the**gas**constant R. The ratio y of the specificheats ...

Page 182

For an ideal

mentioned previously, no temperature change results from a throttling process.

More generally, n > 0 if a > T~l, and conversely p < 0 if a < T~l. The locus of points

in the pT ...

For an ideal

**gas**we found in (5 • 7 • 15) that a = T~K Then n = 0 and, asmentioned previously, no temperature change results from a throttling process.

More generally, n > 0 if a > T~l, and conversely p < 0 if a < T~l. The locus of points

in the pT ...

Page 282

R. D. Present: "Kinetic Theory of

Company, New York, 1958. PROBLEMS 7.1 Consider a homogeneous mixture of

inert monatomic ideal

.

R. D. Present: "Kinetic Theory of

**Gases**," chaps. 2 and 5, McGraw-Hill BookCompany, New York, 1958. PROBLEMS 7.1 Consider a homogeneous mixture of

inert monatomic ideal

**gases**at absolute temperature T in a container of volume V.

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Reif: fundamental of statistical thermal physics

### Contents

Introduction to statistical methods | 1 |

GENERAL DISCUSSION OF THE RANDOM WALK | 24 |

Statistical description of systems of particles | 47 |

Copyright | |

24 other sections not shown

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### Common terms and phrases

absolute temperature approximation assume atoms becomes Boltzmann equation calculate canonical distribution chemical potential classical coefficient collision condition Consider constant container corresponding curve denote density depends derivatives discussion electrons ensemble entropy equal equation equilibrium situation equipartition theorem evaluated example expression external parameters fluctuations frequency gases given heat capacity heat reservoir Hence ideal gas independent infinitesimal integral integrand interaction internal energy isolated system kinetic liquid macroscopic macrostate magnetic field mass maximum mean energy mean number mean pressure mean value measured metal molar mole molecular momentum number of molecules number of particles obtains partition function perature phase space photons physical piston position probability problem quantity quantum quantum mechanics quasi-static radiation range relation result simply solid specific heat spin statistical mechanics Suppose theorem thermal contact thermally insulated Thermodynamics tion total energy total number unit volume variables velocity yields