Mechanical Behavior of Materials |
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Page 106
... energy ( neglecting the core energy ) U1 = U 1 = Gb2 In ( 24 ) Gb2 Απ ( 3.12 ) where U , is the dislocation strain energy per unit length of dislocation line . Approximate calculations indicate the core energy is but a small fraction of ...
... energy ( neglecting the core energy ) U1 = U 1 = Gb2 In ( 24 ) Gb2 Απ ( 3.12 ) where U , is the dislocation strain energy per unit length of dislocation line . Approximate calculations indicate the core energy is but a small fraction of ...
Page 176
... energy neutron bombardment , also give rise to a tetragonal distortion , as will the collapse of excess vacancies ( which can also be generated by irradiation ) into a ... Energy Energy Position Umodulus 176 MECHANICAL BEHAVIOR OF MATERIALS.
... energy neutron bombardment , also give rise to a tetragonal distortion , as will the collapse of excess vacancies ( which can also be generated by irradiation ) into a ... Energy Energy Position Umodulus 176 MECHANICAL BEHAVIOR OF MATERIALS.
Page 465
... energy . For high - strength materials , the impact energies are low , as shown in Fig . 10.16 . For high - strength materials other than carbon steels ( e.g. , Ti and Al alloys ) , the impact energy is fairly temperature - insensitive ...
... energy . For high - strength materials , the impact energies are low , as shown in Fig . 10.16 . For high - strength materials other than carbon steels ( e.g. , Ti and Al alloys ) , the impact energy is fairly temperature - insensitive ...
Contents
Elastic Behavior | 46 |
Plastic Deformation in Single and Polycrystalline | 137 |
Strengthening of Crystalline Materials | 162 |
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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