Introduction to Solid State Physicsproblems after each chapter |
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Page 61
Design on paper a rotating - crystal experiment to determine the crystal structure of a single crystal specimen of NaBr . ... target material , distances , spacing of different reflections , and other relevant experimental factors .
Design on paper a rotating - crystal experiment to determine the crystal structure of a single crystal specimen of NaBr . ... target material , distances , spacing of different reflections , and other relevant experimental factors .
Page 80
THEORETICAL AND EXPERIMENTAL LATTICE ENERGIES At Room TEMPERATURE Lattice Energy ( kcal / mole ) Lattice Crystal Constant ( A ) Theoretical Theoretical Experimental ( Mayer et al . ) ( Slater ) ( 0 ° K ) LiF 4.02 240.1 231 Lici 5.13 ...
THEORETICAL AND EXPERIMENTAL LATTICE ENERGIES At Room TEMPERATURE Lattice Energy ( kcal / mole ) Lattice Crystal Constant ( A ) Theoretical Theoretical Experimental ( Mayer et al . ) ( Slater ) ( 0 ° K ) LiF 4.02 240.1 231 Lici 5.13 ...
Page 411
in the Ni - Fe alloy Supermalloy by Yager and Bozorth.13 A schematic experimental arrangement is shown in Fig . 15.6 . In the experiments it is found that the apparent g values are often very much higher than 300 200 100 80 60 40 20 10 ...
in the Ni - Fe alloy Supermalloy by Yager and Bozorth.13 A schematic experimental arrangement is shown in Fig . 15.6 . In the experiments it is found that the apparent g values are often very much higher than 300 200 100 80 60 40 20 10 ...
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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 normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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