Introduction to Solid State Physicsproblems after each chapter |
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Page 151
1000 800 Iron alloys 600 400 Mild 0.1 % C 2 % Ni 200 3 % Ni 2 % Mn -13 % Cr -4 % AI 13 % Mn Thermal conductivity ( milliwatts / cm deg K ) 100 57 % Ni 80 60 -39 % Mn 13 % Cr , quenched 19 % Cr 40 or 13 % Mn , 1 % Cry 24 % Ni31 % Ni-36 ...
1000 800 Iron alloys 600 400 Mild 0.1 % C 2 % Ni 200 3 % Ni 2 % Mn -13 % Cr -4 % AI 13 % Mn Thermal conductivity ( milliwatts / cm deg K ) 100 57 % Ni 80 60 -39 % Mn 13 % Cr , quenched 19 % Cr 40 or 13 % Mn , 1 % Cry 24 % Ni31 % Ni-36 ...
Page 312
12 Application of Brillouin Zone Theory to Metals and Alloys In this chapter we shall apply band theory in a descriptive and qualitative way to account for a number of physical properties of metals and alloys .
12 Application of Brillouin Zone Theory to Metals and Alloys In this chapter we shall apply band theory in a descriptive and qualitative way to account for a number of physical properties of metals and alloys .
Page 561
Estimates of y for brass and for copper - gold alloys , based upon the thermodynamics of the alloys , give order of magnitude agreement with the observed strengths of these alloys . It is well known that the strength of a crystalline ...
Estimates of y for brass and for copper - gold alloys , based upon the thermodynamics of the alloys , give order of magnitude agreement with the observed strengths of these alloys . It is well known that the strength of a crystalline ...
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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