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Page 82
... tion closely approaches its maximum possible value called the saturation polarization . Upon cycling 5 , the path subsequently traced is [ A to PR to Ec to B to ( PR ) ] to [ A to PR ] to E , to B to ( PR ) ] PR is called the remanent ...
... tion closely approaches its maximum possible value called the saturation polarization . Upon cycling 5 , the path subsequently traced is [ A to PR to Ec to B to ( PR ) ] to [ A to PR ] to E , to B to ( PR ) ] PR is called the remanent ...
Page 183
... tion alone cannot account for van der Waals cohesion since there is an interac- tion term which is independent of temperature . The dipole is not rigid , but rather the charge distribution of one dipole changes the field of a ...
... tion alone cannot account for van der Waals cohesion since there is an interac- tion term which is independent of temperature . The dipole is not rigid , but rather the charge distribution of one dipole changes the field of a ...
Page 445
... tion will be reached throughout ( copper and nickel form a continuous solid substitutional solution ; see Figure 16.4.6 ) . From the macroscopic viewpoint the only difference between these processes is the rate : Diffusion is fastest in ...
... tion will be reached throughout ( copper and nickel form a continuous solid substitutional solution ; see Figure 16.4.6 ) . From the macroscopic viewpoint the only difference between these processes is the rate : Diffusion is fastest in ...
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