Introduction to Solid State Physics |
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Page 128
thermodynamic methods that a case A transition does not have a latent heat of
transition , but is rather accompanied by a discontinuity in the heat capacity ; such
a transition is known in thermodynamics as a second order transition ; a case B ...
thermodynamic methods that a case A transition does not have a latent heat of
transition , but is rather accompanied by a discontinuity in the heat capacity ; such
a transition is known in thermodynamics as a second order transition ; a case B ...
Page 318
ground state : thus the absorption occurs from A to B , rather than from A to C .
After the transition a rearrangement of the neighboring ions takes place with the
system ending up at the equilibrium position C , the energy difference B - C being
...
ground state : thus the absorption occurs from A to B , rather than from A to C .
After the transition a rearrangement of the neighboring ions takes place with the
system ending up at the equilibrium position C , the energy difference B - C being
...
Page 318
ground state : thus the absorption occurs from A to B , rather than from A to C .
After the transition a rearrangement of the neighboring ions takes place with the
system ending up at the equilibrium position C , the energy difference B - C being
...
ground state : thus the absorption occurs from A to B , rather than from A to C .
After the transition a rearrangement of the neighboring ions takes place with the
system ending up at the equilibrium position C , the energy difference B - C being
...
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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 |