Single Crystal Slip Dislocation Concept Cottrell Energy Argument Peierls-Nabarro Force Dislocation Motion

Single Crystal Slip Dislocation Concept Cottrell Energy Argument Peierls-Nabarro Force Dislocation Motion www.phwiki.com

Single Crystal Slip Dislocation Concept Cottrell Energy Argument Peierls-Nabarro Force Dislocation Motion

Lewis, Doris, Executive Producer of Digital Correspondent Content has reference to this Academic Journal, PHwiki organized this Journal Single Crystal Slip Adapted from Fig. 7.8, Callister 7e. Adapted from Fig. 7.9, Callister 7e. Calculation of Theoretical Shear Stress as long as a Perfect Lattice G. Dieter, Mechanical Metallurgy, 3rd Edition, McGraw-Hill, 1986. Dislocation Concept Concept of dislocation was first introduced to explain the discrepancy between observed in addition to theoretical shear strengths For the dislocation concept to be valid: The motion of a dislocation through a lattice must require less stress than the theoretical shear stress The movement of dislocations must produce steps or slip b in addition to s at free surfaces

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Cottrell Energy Argument Plastic de as long as mation is transition from unslipped to slipped state The process is opposed by an energy barrier To minimize energy the slipped material will grow by advance of an interfacial region (dislocation) To minimize energy of transition – interface thickness, w, small Distance w is width of dislocation Smaller w – lower interfacial energy Larger w – lower elastic energy of the crystal – atomic spacing in the slip direction is closer to atomic spacing Equilibrium width is a balance of these two components G. Dieter, Mechanical Metallurgy, 3rd Edition, McGraw-Hill, 1986. Peierls-Nabarro Force Dislocation width determines the as long as ce required to move a dislocation through a crystal lattice Peierls stress is the shear stress required to move a dislocation through a crystal lattice Note: wide dislocations require lower stress to move Makes sense: Wide – the highly distorted region at core is not localized on any particular atom In ductile metals the dislocation width is on the order of 10 atomic spacings a is distance between slip planes b is the distance between atoms in the slip direction In ceramics with directional covalent bonds – high interfacial energy, dislocations are narrow – relatively immobile Combined with restrictions on slip systems imposed by electrostatic as long as ces – low degree of plasticity Dislocation Motion

Dislocation Motion Dislocations & plastic de as long as mation Cubic & hexagonal metals – plastic de as long as mation by plastic shear or slip where one plane of atoms slides over adjacent plane by defect motion (dislocations). If dislocations don’t move, de as long as mation doesn’t occur! Adapted from Fig. 7.1, Callister 7e. Dislocation Motion Dislocation moves along slip plane in slip direction perpendicular to dislocation line Slip direction same direction as Burgers vector Edge dislocation Screw dislocation Adapted from Fig. 7.2, Callister 7e. Definition of a Slip System Slip plane – plane allowing easiest slippage: Minimize atomic distortion (energy) associated with dislocation motion Wide interplanar spacings – highest planar atomic densities (Close Packed) Slip direction – direction of movement Highest linear atomic densities on slip plane

Independent Slip Systems The number of independent slip systems is the total possible number of combinations of slip planes in addition to directions Example: FCC Slip occurs on {111} planes (close-packed) in <110> directions (close-packed) 4 Unique {111} planes On each plane 3 independent ‹110› Total of 12 slip systems in FCC Slip Systems Some slip systems in BCC are only activated at high temperatures BCC in addition to FCC have many possible slip systems – ductile materials HCP: Less possible slip systems – brittle material Stress in addition to Dislocation Motion Crystals slip due to a resolved shear stress, tR. Applied tension can produce such a stress.

Condition as long as dislocation motion: Crystal orientation can make it easy or hard to move dislocation Critical Resolved Shear Stress maximum at = = 45º Schmid’s Law Schmid Factor Ex: De as long as mation of single crystal So the applied stress of 6500 psi will not cause the crystal to yield. =35° =60° crss = 3000 psi a) Will the single crystal yield b) If not, what stress is needed = 6500 psi Adapted from Fig. 7.7, Callister 7e. Ex: De as long as mation of single crystal What stress is necessary (i.e., what is the yield stress, sy)

Lewis, Doris KGTV-TV Executive Producer of Digital Correspondent Content www.phwiki.com

Lewis, Doris Executive Producer of Digital Correspondent Content

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