Introduction to Solid State Physicsproblems after each chapter |
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Page 61
tion , are treated at length in the book by Barrett listed at the end of the chapter
and also in the papers by Barrett , Guinier , and Warren and Averbach in the
symposium volume entitled Imperfections in nearly perfect crystals . PROBLEMS
2 . 1 .
tion , are treated at length in the book by Barrett listed at the end of the chapter
and also in the papers by Barrett , Guinier , and Warren and Averbach in the
symposium volume entitled Imperfections in nearly perfect crystals . PROBLEMS
2 . 1 .
Page 173
tion is neglected , the Onsager model gives ( 7 . 32 ) E = [ 1 + 3x + 3 ( 1 + six + x )
! ) , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in
Appendix C , does not give a critical point . Further discussion of the problem
would ...
tion is neglected , the Onsager model gives ( 7 . 32 ) E = [ 1 + 3x + 3 ( 1 + six + x )
! ) , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in
Appendix C , does not give a critical point . Further discussion of the problem
would ...
Page 390
tion of junctions a small pellet of indium ( for example ) is placed on a crystal of n
- type germanium . On heating the indium melts and dissolves some germanium ;
on subsequent cooling most of the dissolved germanium precipitates on ...
tion of junctions a small pellet of indium ( for example ) is placed on a crystal of n
- type germanium . On heating the indium melts and dissolves some germanium ;
on subsequent cooling most of the dissolved germanium precipitates on ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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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