Fundamentals of statistical and thermal physics |
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Page 141
Measurements of the specific heat involve measurements of heat of the type
discussed in Sec. 4-2. In measuring heat by the comparison method (or method
of mixtures), it used to be popular to select water as the reference substance.
Hence a ...
Measurements of the specific heat involve measurements of heat of the type
discussed in Sec. 4-2. In measuring heat by the comparison method (or method
of mixtures), it used to be popular to select water as the reference substance.
Hence a ...
Page 272
Hence all molecules of this type which lie within the infinitesimal cylinder of cross
-sectional area dA and of a length v dt making an angle 6 with the e axis will
strike the wall within the time interval dt; the molecules lying outside this cylinder
will ...
Hence all molecules of this type which lie within the infinitesimal cylinder of cross
-sectional area dA and of a length v dt making an angle 6 with the e axis will
strike the wall within the time interval dt; the molecules lying outside this cylinder
will ...
Page 380
This would again lead to a nonpermissible temperature difference being
produced between these bodies. Hence we can conclude that /.(k) = /.(«), where
k = |te| 3. The number / is independent of the direction of polarization of the
radiation, i.e., ...
This would again lead to a nonpermissible temperature difference being
produced between these bodies. Hence we can conclude that /.(k) = /.(«), where
k = |te| 3. The number / is independent of the direction of polarization of the
radiation, i.e., ...
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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 | |
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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