Introduction to Solid State Physics |
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Results 1-3 of 59
Page 104
If the induced polarization is neglected , the Onsager model gives ( 6 . 32 ) E = { [
1 + 3x + 3 ( 1 + x + x2 ) " ] , x = 41Np2 / 3kT . It is easily seen that this expression ,
which is derived in Appendix D , does not gives a critical point . Further ...
If the induced polarization is neglected , the Onsager model gives ( 6 . 32 ) E = { [
1 + 3x + 3 ( 1 + x + x2 ) " ] , x = 41Np2 / 3kT . It is easily seen that this expression ,
which is derived in Appendix D , does not gives a critical point . Further ...
Page 227
This gives gi – ni = ea + BW i , ni or ( 12 . 16 ) _ _ 9i ni = . ea + Bw ; + 1 The
Lagrangian multiplier a is determined by the condition Eni = N . We may
determine the constant B by the observation that at very high temperatures ni / gi
must be « 1 ...
This gives gi – ni = ea + BW i , ni or ( 12 . 16 ) _ _ 9i ni = . ea + Bw ; + 1 The
Lagrangian multiplier a is determined by the condition Eni = N . We may
determine the constant B by the observation that at very high temperatures ni / gi
must be « 1 ...
Page 353
... if r is measured from the nucleus , and in mononuclear systems gives rise only
to paramagnetism . The * J . Pirenne , Helv . Phys . Acta 22 , 479 ( 1949 ) .
second term gives for a spherically symmetric system a diamagnetic APPENDIX
353.
... if r is measured from the nucleus , and in mononuclear systems gives rise only
to paramagnetism . The * J . Pirenne , Helv . Phys . Acta 22 , 479 ( 1949 ) .
second term gives for a spherically symmetric system a diamagnetic APPENDIX
353.
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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
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 |