Introduction to Solid State Physics |
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Page 36
We compare the calculated Coulomb energy with the observed total binding
energy , and then estimate n on the basis of Eq . ( 2 . 5 ) . U ( Coulomb ) U . (
observed ) Substance ( kcal / mole ) ( kcal / mole ) NaCl 206 183 NaBr 195 173
NaI 180 ...
We compare the calculated Coulomb energy with the observed total binding
energy , and then estimate n on the basis of Eq . ( 2 . 5 ) . U ( Coulomb ) U . (
observed ) Substance ( kcal / mole ) ( kcal / mole ) NaCl 206 183 NaBr 195 173
NaI 180 ...
Page 266
9 shows that the Grüneisen relation works quite well for the metals indicated
there ; at quite low temperatures , however , departures from the TTM law are
usually observed . Reference to detailed theoretical calculations of the
conductivity of ...
9 shows that the Grüneisen relation works quite well for the metals indicated
there ; at quite low temperatures , however , departures from the TTM law are
usually observed . Reference to detailed theoretical calculations of the
conductivity of ...
Page 297
Thus we estimate for the critical shear stress ( 16 . 2 ) Oc ~ G / 4 . From values of
044 given in Table 3 . 1 we may expect the critical shear stress to be of the order
of 1010 to 1011 dynes / cm2 . The observed shearing stress required ...
Thus we estimate for the critical shear stress ( 16 . 2 ) Oc ~ G / 4 . From values of
044 given in Table 3 . 1 we may expect the critical shear stress to be of the order
of 1010 to 1011 dynes / cm2 . The observed shearing stress required ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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Common terms and phrases
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
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |