Introduction to Solid State Physicsproblems after each chapter |
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Page 108
The solution for k = * / L has u o sin nta / L and vanishes for n = 0 and n = N as
required , with a maximum for n = N / 2 . The solution for k = N / L = a / a = km has
u o sin na , permitting no motion at all , because sin ni vanishes at each particle .
The solution for k = * / L has u o sin nta / L and vanishes for n = 0 and n = N as
required , with a maximum for n = N / 2 . The solution for k = N / L = a / a = km has
u o sin na , permitting no motion at all , because sin ni vanishes at each particle .
Page 236
or , if vo ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the
approach to equilibrium is described by the appropriate solution of ( 10 . 3 ) : ( 10
. 4 ) VD ( I ) = vd ( 0 ) et / 7 . We have thus arranged things so that a disturbance ...
or , if vo ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the
approach to equilibrium is described by the appropriate solution of ( 10 . 3 ) : ( 10
. 4 ) VD ( I ) = vd ( 0 ) et / 7 . We have thus arranged things so that a disturbance ...
Page 274
The evolution of the standing wave solution is traced through in detail in
Appendix I . What is important at present is that the solutions for k = fala combine
to give standing waves of different energies , the energies being different not
through the ...
The evolution of the standing wave solution is traced through in detail in
Appendix I . What is important at present is that the solutions for k = fala combine
to give standing waves of different energies , the energies being different not
through the ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials, ISSN 0084-0203 Wiley series on the science and technology of materials. J. H. Hollomon, advisory editor |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1956 |
| Original from | the University of Michigan |
| Digitized | 24 Feb 2009 |
| ISBN | 0852264674, 9780852264676 |
| Length | 617 pages |
| Export Citation | BiBTeX EndNote RefMan |