Introduction to Solid State Physics |
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Page 46
STRESS COMPONENTS The force acting on a unit area in the solid is defined as
the stress . There are nine stress components : XX , Xy , X . , Y . , Yu , Y . , Z . , Zy ,
Zz . The capital letter indicates the direction of the force , and the subscript ...
STRESS COMPONENTS The force acting on a unit area in the solid is defined as
the stress . There are nine stress components : XX , Xy , X . , Y . , Yu , Y . , Z . , Zy ,
Zz . The capital letter indicates the direction of the force , and the subscript ...
Page 297
SHEAR STRENGTH OF SINGLE CRYSTALS The classical prediction for the
strength of crystals is that the critical shear stress oc should be of the order of
magnitude of the shear modulus G , which in a cubic crystal is equal to C44 . If x
is the ...
SHEAR STRENGTH OF SINGLE CRYSTALS The classical prediction for the
strength of crystals is that the critical shear stress oc should be of the order of
magnitude of the shear modulus G , which in a cubic crystal is equal to C44 . If x
is the ...
Page 310
An applied shear stress causes BC to curve as shown and to generate a
succession of dislocation rings . PRECIPITATION HARDENING Directly after
quenching , an alloy in the form of a supersaturated solid solution is mechanically
soft .
An applied shear stress causes BC to curve as shown and to generate a
succession of dislocation rings . PRECIPITATION HARDENING Directly after
quenching , an alloy in the form of a supersaturated solid solution is mechanically
soft .
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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