A copper crystal ( , ) contains two straight

PHYSICS · Multi-part · Fermi University Physics · Fluids & Continuum Physics · Solid continuum mechanics and complex fluids · Solid continuum mechanics and complex fluids

Bending, Ringing, Breaking and Flowing, Ch Dislocations and the onset of plastic flow

Problem

A copper crystal (G=48 GPaG = 48\,\mathrm{GPa}, b=0.256 nmb = 0.256\,\mathrm{nm}) contains two straight, parallel edge dislocations lying along zz, both gliding on the same slip plane y=0y=0. Dislocation A sits at x=0x=0 with Burgers vector bA=b x^\mathbf{b}_A = b\,\hat{\mathbf x}; dislocation B sits at x=d=50 nmx = d = 50\,\mathrm{nm} with Burgers vector bB=−b x^\mathbf{b}_B = -b\,\hat{\mathbf x} (same magnitude, opposite sign: an edge dislocation dipole). A uniform stress is applied to the crystal with σxy=τ=15 MPa\sigma_{xy} = \tau = 15\,\mathrm{MPa} and all other stress components zero. ((a)) Using the Peach-Koehler force f=(σ⋅b)×ξ\mathbf f = (\boldsymbol\sigma\cdot\mathbf b)\times\boldsymbol\xi (with ξ=z^\boldsymbol\xi = \hat{\mathbf z}), find the glide force per unit length on each dislocation, stating its direction along xx. ((b)) Predict whether the pair glides together (towards annihilation) or apart, under this applied stress alone.

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