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 159
... properties of both fermions and bosons are identical , as we show below . The quantum regime is the opposite of the classical regime : the occupancy of an orbital may be comparable to one or larger . Here the properties of a fermion gas ...
... properties of both fermions and bosons are identical , as we show below . The quantum regime is the opposite of the classical regime : the occupancy of an orbital may be comparable to one or larger . Here the properties of a fermion gas ...
Contents
STATES OF THE MODEL SYSTEM | 11 |
AN ELEMENTARY SOLUBLE SYSTEM | 17 |
SHARP PEAK OF gN | 19 |
Copyright | |
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approximation Boltzmann bosons calculated Carnot cycle chemical potential classical regime closed system cm³ combined system concentration defined definition denote derivative diffusive contact dipole distribution function electric field electron energy levels ensemble entropy equal equation equilibrium ergs example expansion experimental Fermi energy Fermi gas Fermi-Dirac fermions Figure fluctuations flux fractional free energy free particle frequency gases given grand sum He¹ He³ heat capacity helium ideal gas law increase integral isothermal kinetic lattice liquid low temperature m₁ magnetic field magnetic moment model system molecule N₁ negative temperature number of accessible number of atoms number of particles occupied P₁ partition function photons plotted pressure probable configuration Problem properties quantity quantum number reservoir result spin excess superfluid system in thermal term thermal average thermal contact thermodynamic potential total number U₁ unit velocity versus volume white dwarf ат