Introduction to Solid State Physics |
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Page 203
In d - c measurements the resistivity in the superconducting state is zero . At
infrared frequencies the resistivity is that of the normal state ; that is , no change
in the resistivity , as by the fatic field . or behar measured by the EXPERIMENTAL
...
In d - c measurements the resistivity in the superconducting state is zero . At
infrared frequencies the resistivity is that of the normal state ; that is , no change
in the resistivity , as by the fatic field . or behar measured by the EXPERIMENTAL
...
Page 266
differ12 somewhat from the value deduced from heat capacities for several
reasons , including the fact that only longitudinal phonons are effective in the
resistivity , while both longitudinal and transverse contribute to the heat capacity .
differ12 somewhat from the value deduced from heat capacities for several
reasons , including the fact that only longitudinal phonons are effective in the
resistivity , while both longitudinal and transverse contribute to the heat capacity .
Page 302
Electrical resistivity vs . temperature for Cu , Au . The alloy was in equilibrium at
temperatures above 350°C . ( After Nix and Shockley . ) face . This tells us that
the form factor S { 100 } = 0 , as discussed in Chapter 1 . The same result holds in
a ...
Electrical resistivity vs . temperature for Cu , Au . The alloy was in equilibrium at
temperatures above 350°C . ( After Nix and Shockley . ) face . This tells us that
the form factor S { 100 } = 0 , as discussed in Chapter 1 . The same result holds in
a ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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Common terms and phrases
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
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |