Introduction to Solid State Physics |
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Page 23
11 ) sin MT dr * = f * u ( a ) sin war de O ur for the atomic scattering factor . It is the
ratio of the ... Tables of atomic scattering factors calculated by the Hartree and
Thomas - Fermi methods have been published . The results for sodium are
plotted ...
11 ) sin MT dr * = f * u ( a ) sin war de O ur for the atomic scattering factor . It is the
ratio of the ... Tables of atomic scattering factors calculated by the Hartree and
Thomas - Fermi methods have been published . The results for sodium are
plotted ...
Page 91
The constant N is known as the depolarization factor or , more commonly , as the
demagnetization factor , and its value depends on the axial ratio . It is
exceptionally important in the field of magnetism . Values of N are plotted in Fig .
6 .
The constant N is known as the depolarization factor or , more commonly , as the
demagnetization factor , and its value depends on the axial ratio . It is
exceptionally important in the field of magnetism . Values of N are plotted in Fig .
6 .
Page 110
w tano , 47 where the loss angle or power factor is defined as ( 6 . 48 ) tan 8 = 62
! €1 . The Q factor of a systein is defined as maximum stored energy ( 6 . 49 )
average energy loss per radian which in the dielectric case reduces to Q = - Eico
...
w tano , 47 where the loss angle or power factor is defined as ( 6 . 48 ) tan 8 = 62
! €1 . The Q factor of a systein is defined as maximum stored energy ( 6 . 49 )
average energy loss per radian which in the dielectric case reduces to Q = - Eico
...
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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 |