Introduction to Solid State Physics |
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Page 27
Show that the maximum proportion of the available volume which may be filled
by hard spheres arranged in various structures is Simple cubic Body - centered
cubic Face - centered cubic Hexagonal close - packed Diamond a / 6 ( = 0 .
Show that the maximum proportion of the available volume which may be filled
by hard spheres arranged in various structures is Simple cubic Body - centered
cubic Face - centered cubic Hexagonal close - packed Diamond a / 6 ( = 0 .
Page 198
Show that the total energy is a minimum when eii = Bi [ c12 – ai ? ( C11 + 2012 ) ]
/ [ ( c11 – C12 ) ( c11 + 2c12 ) ] ; lij = – B2QjQj / C44 ( i = j ) . This is a formal
explanation of the origin of magnetostriction . 10 . 4 . Show that the magnetic
energy ...
Show that the total energy is a minimum when eii = Bi [ c12 – ai ? ( C11 + 2012 ) ]
/ [ ( c11 – C12 ) ( c11 + 2c12 ) ] ; lij = – B2QjQj / C44 ( i = j ) . This is a formal
explanation of the origin of magnetostriction . 10 . 4 . Show that the magnetic
energy ...
Page 247
Charles Kittel. PROBLEMS 12 . 1 . Show that the kinetic energy of a free electron
gas at 0°K is U . ENWr ! . 12 . 2 . Using conventional valencies , show that for
sodium , potassium , and aluminum the values of W po are 3 . 12 , 2 . 14 , and 11
.
Charles Kittel. PROBLEMS 12 . 1 . Show that the kinetic energy of a free electron
gas at 0°K is U . ENWr ! . 12 . 2 . Using conventional valencies , show that for
sodium , potassium , and aluminum the values of W po are 3 . 12 , 2 . 14 , and 11
.
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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