## Fundamentals of statistical and thermal physics |

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Page 308

We see immediately that the stability condition dp/dv < 0 is violated in the region

V\ < v < v2 where the

certainly excluded since they would lead to an intrinsically unstable situation.

We see immediately that the stability condition dp/dv < 0 is violated in the region

V\ < v < v2 where the

**curve**has positive slope. Thus values of v in this range arecertainly excluded since they would lead to an intrinsically unstable situation.

Page 309

M. Hence a

the appearance shown in Fig. 8-6-3. (The points on this

correspond to those of Fig. 8-6-2.) From this diagram one can readily see what ...

M. Hence a

**curve**of g(T,p) versus p along the constant-temperature**curve**hasthe appearance shown in Fig. 8-6-3. (The points on this

**curve**are labeled tocorrespond to those of Fig. 8-6-2.) From this diagram one can readily see what ...

Page 454

I _

One can repeat this kind of adiabatic process starting always at d = but from a

variety of initial fields H. Thus one can reach a variety of final temperatures d in

the ...

I _

**curve**showing Std.H,,) aa a function of i> for the I » given value H — H0. 0 6One can repeat this kind of adiabatic process starting always at d = but from a

variety of initial fields H. Thus one can reach a variety of final temperatures d in

the ...

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User Review - JJMAlmeida - LibraryThingNever mind that this book was published in the mid '60s (before I was even born); if you must choose one book to learn from, choose this one. It is so concise, so well thought out that I have yet to ... Read full review

### Contents

Introduction to statistical methods | 1 |

GENERAL DISCUSSION OF THE RANDOM WALK | 24 |

Statistical description of systems of particles | 47 |

Copyright | |

26 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 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 satisfy simply solid specific heat spin statistical mechanics Suppose theorem thermal contact thermally insulated Thermodynamics tion total energy total number unit volume variables velocity