Introduction to Solid State Physics |
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Page 179
The fact that a sufficiently small particle , with diameter less than 10 - 4 or 10 – 5
cm , is composed of a single domain is a ... It can be shown 21 that with such very
small particles the formation of a domain boundary is energetically unfavorable ...
The fact that a sufficiently small particle , with diameter less than 10 - 4 or 10 – 5
cm , is composed of a single domain is a ... It can be shown 21 that with such very
small particles the formation of a domain boundary is energetically unfavorable ...
Page 208
Superconductivity of small particles . The diamagnetic susceptibility of small
particles is less than that of bulk superconductors . A large mercury sphere ( Fig .
11 . 4 ) exhibits an effective volume susceptibility of Xo = - 3 / 87 , whereas ...
Superconductivity of small particles . The diamagnetic susceptibility of small
particles is less than that of bulk superconductors . A large mercury sphere ( Fig .
11 . 4 ) exhibits an effective volume susceptibility of Xo = - 3 / 87 , whereas ...
Page 310
As aging continues , the particle size of the precipitate becomes large and
resoftening takes place ; the effect is known as ... Maximum hardness is found
when the average spacing between precipitate particles is of the order of 25 to 50
lattice ...
As aging continues , the particle size of the precipitate becomes large and
resoftening takes place ; the effect is known as ... Maximum hardness is found
when the average spacing between precipitate particles is of the order of 25 to 50
lattice ...
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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