## Fundamentals of statistical and thermal physics |

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Page 270

Imagine that the container is a box in the form of a parallelepiped, the area of one

end- wall being A. How many molecules per unit time strike this end-wall?

Suppose that there are in this gas n molecules per

move in ...

Imagine that the container is a box in the form of a parallelepiped, the area of one

end- wall being A. How many molecules per unit time strike this end-wall?

Suppose that there are in this gas n molecules per

**unit volume**. Since they allmove in ...

Page 469

We shall give the argument in simplified fashion without being too careful about

the rigorous way of taking various averages. Consider a gas consisting of only a

single kind of molecule. Denote the mean number of molecules per

We shall give the argument in simplified fashion without being too careful about

the rigorous way of taking various averages. Consider a gas consisting of only a

single kind of molecule. Denote the mean number of molecules per

**unit volume**...Page 474

Let us now give an approximate simple calculation of the coefficient of viscosity. If

there are n molecules per

along the z direction. Half of these, or \n molecules per

Let us now give an approximate simple calculation of the coefficient of viscosity. If

there are n molecules per

**unit volume**, roughly one-third of them have velocitiesalong the z direction. Half of these, or \n molecules per

**unit volume**, have mean ...### What people are saying - Write a review

#### LibraryThing Review

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