Mechanical Behavior of Materials |
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Page 176
... effect interaction , the modulus effect ( whether it is attractive or repulsive ) does not depend on whether the solute atom lies above or below the glide plane . Both the size and modulus effects produce a dislocation - solute atom ...
... effect interaction , the modulus effect ( whether it is attractive or repulsive ) does not depend on whether the solute atom lies above or below the glide plane . Both the size and modulus effects produce a dislocation - solute atom ...
Page 179
... effect interaction energy , the modulus interaction energy can be either attractive or repulsive depending on whether & is negative or positive . Appropriate combination of the two interaction energies into one from which τ , can be ...
... effect interaction energy , the modulus interaction energy can be either attractive or repulsive depending on whether & is negative or positive . Appropriate combination of the two interaction energies into one from which τ , can be ...
Page 202
... effect is more important the higher the elastic - phase volume fraction ( or , alternatively , the higher the ratio of elastic - phase particle radius to elastic - phase interparticle spacing ) ; this effect is essentially absent in ...
... effect is more important the higher the elastic - phase volume fraction ( or , alternatively , the higher the ratio of elastic - phase particle radius to elastic - phase interparticle spacing ) ; this effect is essentially absent in ...
Contents
Elastic Behavior | 46 |
Plastic Deformation in Single and Polycrystalline | 137 |
Strengthening of Crystalline Materials | 162 |
Copyright | |
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alloys applied stress behavior Burgers vector Chap Coble creep composite crack growth crack tip craze creep fracture creep rate crystalline cubic cyclical decreases diffusion diffusional discussed dislocation density dislocation glide dislocation motion displacement ductile ductile fracture edge dislocation effect embrittlement energy fatigue fiber FIGURE flow stress fracture mechanism fracture toughness glass grain boundaries hardening high-temperature illustrated in Fig increases initial interaction length linear elastic low temperatures martensite material material's matrix mechanism map metals microscopic microstructural MN/m² Mode II fracture modulus Nabarro-Herring noncrystalline nucleation obstacles occurs particle phase plastic deformation plastic flow polycrystal polymers ratio recrystallization region result schematically screw dislocation shear stress shown in Fig single crystals slip plane slip systems solid steel strain rate strengthening stress levels stress-strain curve structure superplastic surface takes place TCRSS tensile strength tensile stress transition values viscoelastic viscosity void growth volume fraction yield strength