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Page 94
... Note that X - 10-5 for diamagnetic materials . Thus dia- magnetic materials tend to repel the lines of flux . Note also that Xm 104 for paramagnetic materials . Paramagnetic materials are weakly attracted by a magnet . For example ...
... Note that X - 10-5 for diamagnetic materials . Thus dia- magnetic materials tend to repel the lines of flux . Note also that Xm 104 for paramagnetic materials . Paramagnetic materials are weakly attracted by a magnet . For example ...
Page 276
... Note , however , that far from the dislocation line the packing arrangement is correct , although the atoms there ... note that the Burgers vector equals a translation vector of the lattice ( in the direction of the Burgers vector ) . We ...
... Note , however , that far from the dislocation line the packing arrangement is correct , although the atoms there ... note that the Burgers vector equals a translation vector of the lattice ( in the direction of the Burgers vector ) . We ...
Page 758
... Note that the period of this potential is now a since b -1 cos ka ≤ 1 . a . Why ? - 0. Note that Note that the function y ( aa ) P ( sin xa / αa ) + cos da is really a function of the energy only ( assuming P and a are fixed ) . b ...
... Note that the period of this potential is now a since b -1 cos ka ≤ 1 . a . Why ? - 0. Note that Note that the function y ( aa ) P ( sin xa / αa ) + cos da is really a function of the energy only ( assuming P and a are fixed ) . b ...
Common terms and phrases
alloy aluminum Answer assume atoms band behavior bonds Burgers vector Calculate called carbon cell coefficient component composition concentration conduction band constant cooling copper crystal structure cubic crystal curve deformation density dielectric diffusion dipole discussed dislocation line edge dislocation elastic electrical electron entropy Equation equilibrium eutectic eutectoid EXAMPLE fcc crystal field fraction fracture free energy frequency function Gibbs free energy given glass grain boundary heat Hence high temperatures hydrogen ions lattice layer liquid magnetic martensite materials mechanical melting metals modulus mole molecules NaCl Note p-n junction particles pearlite plane plastic polymer potential pressure Problem properties radius room temperature screw dislocation Section semiconductor shear stress shown in Figure silicon single crystals steel strain superconducting surface Table tensile tensile stress thermal tion transformation unit vacancy valence valence band vector velocity viscosity volume yield strength York zero