Introduction to Solid State Physics |
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Page 151
removed , so that the specimen follows the isoentropic path BC , ending up at
temperature T 2 . ULTIMATE TEMPERATURE REACHED The lowest
temperature reached in adiabatic demagnetization is largely limited by the
natural splitting of ...
removed , so that the specimen follows the isoentropic path BC , ending up at
temperature T 2 . ULTIMATE TEMPERATURE REACHED The lowest
temperature reached in adiabatic demagnetization is largely limited by the
natural splitting of ...
Page 246
A more detailed study of the quantum theory of transport processes in metals
shows that the Lorenz number is expected to be independent of temperature only
above the Debye temperatures , 13 as the differences between the types of ...
A more detailed study of the quantum theory of transport processes in metals
shows that the Lorenz number is expected to be independent of temperature only
above the Debye temperatures , 13 as the differences between the types of ...
Page 305
Free energy of an AB alloy as a function of the degree of order S , for various
temperatures . ... The order is determined as a function of temperature by the
requirement that the free energy F = U – TS be a minimum with respect to the
order ...
Free energy of an AB alloy as a function of the degree of order S , for various
temperatures . ... The order is determined as a function of temperature by the
requirement that the free energy F = U – TS be a minimum with respect to the
order ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero