Thermal Physics |
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Page 31
... properties of the system to damp out . The value of the relax- ation time may depend on the particular property ... properties that do not become random over any practical time interval . Common sense will exclude these properties from a ...
... properties of the system to damp out . The value of the relax- ation time may depend on the particular property ... properties that do not become random over any practical time interval . Common sense will exclude these properties from a ...
Page 144
... properties than systems of fermions . Atoms of He1 are bosons ; atoms of He3 are fermions . For example , the remarkable superfluid properties of the low temperature ( T < 2.17 K ) phase of liquid helium can be attributed to the properties ...
... properties than systems of fermions . Atoms of He1 are bosons ; atoms of He3 are fermions . For example , the remarkable superfluid properties of the low temperature ( T < 2.17 K ) phase of liquid helium can be attributed to the properties ...
Page 285
... properties are exhibited . The region of nega- tive slope on the phase boundary implies that here the solid is more ... properties of the liquids . ( After B. Bertram and R. A. Guyer . ) The phase diagram of He3 is shown in Fig . 6 ...
... properties are exhibited . The region of nega- tive slope on the phase boundary implies that here the solid is more ... properties of the liquids . ( After B. Bertram and R. A. Guyer . ) The phase diagram of He3 is shown in Fig . 6 ...
Contents
QUANTUM STATES | 1 |
AN ELEMENTARY SOLUBLE SYSTEM | 9 |
THE FUNDAMENTAL ASSUMPTION | 27 |
Copyright | |
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absolute zero Boltzmann bosons calculated Carnot cycle chemical potential cm³ combined system concentration curve defined definition denote density derivative diffusive contact dipole distribution function electric field electron energy levels ensemble entropy equal equation ergs example expansion experimental Fermi energy Fermi gas Fermi-Dirac fermions Figure fluctuations fractional free energy free particle frequency given grand sum ground orbital He¹ He³ heat capacity helium ideal gas ideal gas law integral interaction isothermal kinetic lattice liquid low temperatures m₁ magnetic field magnetic moment model system molecule N₁ number of atoms number of particles obtain occupied P₁ partition function phase photons plotted pressure probable configuration Problem properties quantity quantum number relation reservoir result solid spin excess superfluid system in thermal term thermal average thermal contact thermodynamic potential total number U₁ unit vapor velocity versus volume white dwarf ат