## Introduction to Solid State Physicsproblems after each chapter |

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Page 543

slip plane . To a first approximation these forces cancel , and so the external

stress required to move a

not straight , the cancellation will be even more ! il - 8 - 8 - 846 - 6 - - - 6 - 6 - 60 a

2 .

slip plane . To a first approximation these forces cancel , and so the external

stress required to move a

**dislocation**will be quite small . If the**dislocation**line isnot straight , the cancellation will be even more ! il - 8 - 8 - 846 - 6 - - - 6 - 6 - 60 a

2 .

Page 557

in nickel , Brown25 estimates 3 X 1011

deformation . ... If an edge

along its length will eat away a portion of the extra halfplane of atoms and cause

the ...

in nickel , Brown25 estimates 3 X 1011

**dislocations**/ cm2 for severe plasticdeformation . ... If an edge

**dislocation**is present , lattice vacancies precipitatingalong its length will eat away a portion of the extra halfplane of atoms and cause

the ...

Page 560

If L is the mean spacing of particles on a slip plane , the stress necessary to force

a

which is ( 19 . 13 ) rewritten . The smaller the spacing L , the higher is the yield ...

If L is the mean spacing of particles on a slip plane , the stress necessary to force

a

**dislocation**between particles should be approximately ( 19 . 14 ) 0 / G = b / L ,which is ( 19 . 13 ) rewritten . The smaller the spacing L , the higher is the yield ...

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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