Thermal Physics |
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Page 237
... given in Table 2 and in Fig . 11. The electron ve- locity up at the Fermi surface is also given in the table ; it is defined so that the kinetic energy of an electron at the Fermi surface is equal to € F : + mvp2 = € F , ( 36 ) where m ...
... given in Table 2 and in Fig . 11. The electron ve- locity up at the Fermi surface is also given in the table ; it is defined so that the kinetic energy of an electron at the Fermi surface is equal to € F : + mvp2 = € F , ( 36 ) where m ...
Page 321
... Given the energy U ( o , V , N ) : T = ( 0 ) = ( 0 ) p ; T U , N T = = ( 20 ) V.N − p = μ = V , σ , N ( c ) Given the energy U ( T , V , N ) : σ = Su dv dU ; Cv = T ( 흥미 ) = kB ( 37 ) v N V , N V , ( d ) Given the chemical potential ...
... Given the energy U ( o , V , N ) : T = ( 0 ) = ( 0 ) p ; T U , N T = = ( 20 ) V.N − p = μ = V , σ , N ( c ) Given the energy U ( T , V , N ) : σ = Su dv dU ; Cv = T ( 흥미 ) = kB ( 37 ) v N V , N V , ( d ) Given the chemical potential ...
Page 403
... given range are ignored . We show below that the thermal noise power per unit frequency range de- livered by a ... given in Chapter 15 for the distribution of 1 H. Nyquist , Physical Review 32 , 110 ( 1928 ) ; a deeper discussion is ...
... given range are ignored . We show below that the thermal noise power per unit frequency range de- livered by a ... given in Chapter 15 for the distribution of 1 H. Nyquist , Physical Review 32 , 110 ( 1928 ) ; a deeper discussion is ...
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