Chapter 4 Flashcards
Ideal strength of a Material
Possible to approach this in microscopic fibers
Strength of macroscopic chunks of materials limited by crystal defects
0 D
Vacancy
Missing atom where one should exist in lattice
0 D
Interstitial
Extra atom at location in crystal where there should not be an atom
Almost always a very small atom
0 D
Substitutional Impurity
Atom of a different variety replace a native atom in the crystal
Can be larger or smaller
1 D
Edge Dislocation
Linear defect in crystal where the Burgers vector is perpendicular to the line of the dislocation
Characterized by the insertion of an extra half-plane into the crystal
1 D
Screw Dislocation
Linear defect in crystal where the Burgers vector is parallel to the line of the dislocation
Characterized by a spiral pattern of atoms about the dislocation
2 D
Grain Boundaries
Location where two crystals of different orientation meet.
2 D
Phase Boundary
Surface between two different materials
2 D (Of secondary importance)
Twin boundaries -
Stacking Faults -
3 D
Volume Defects
Voids
Cracks
Particles of a different material
Plastic Deformation in Metallic Materials at Low Temperatures is due to line defects
Both edge and screw dislocations produce permanent shear strain in response to applied shear stress of sufficient magnitude
Caused by slip in planes of maximum area packing density in direction of maximum linear density
At low temperature, motion of dislocations can be impeded by point, line, plane, and volume
At high temp, only point and volume defects are effective for strengthening