2001
DOI: 10.1090/qam/1827812
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On the dynamics of continuous distributions of dislocations

Abstract: Abstract.For materials with continuous distributions of dislocations a configuration space which unifies the continuum theory of defects with classical elasticity is given. Weak equations of motion are derived from the principle of virtual work. Using the Helmholtz decomposition theorem, this yields a coupled system of equations for the dynamics of dislocations and classical elasticity.

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Cited by 2 publications
(2 citation statements)
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“…and N is the outward-pointing unit normal vector on the boundary ∂M. This is known as the Helmholtz decomposition [24,25,40]. Let ψ ∈ C ∞ (M; R 3 ) be a component of the exact part and let Θ ∈ D(M; R 3 ) be the other component in the non-exact part.…”
Section: Helmholtz Decomposition and Variational Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…and N is the outward-pointing unit normal vector on the boundary ∂M. This is known as the Helmholtz decomposition [24,25,40]. Let ψ ∈ C ∞ (M; R 3 ) be a component of the exact part and let Θ ∈ D(M; R 3 ) be the other component in the non-exact part.…”
Section: Helmholtz Decomposition and Variational Formulationmentioning
confidence: 99%
“…dislocation and disclination, and the torsion and curvature in the affine connection [15,16,17,18]. This theory was developed further by Noll [19], Wang [20], de Wit [21], Le and Stumpf [22,23], Wenzelburger [24] and Binz et al [25]. Yavari and Goriely reformulated the theories using modern differential geometry and derived analytical solutions to the nonlinear boundary value problems [26,27,28].…”
Section: Introductionmentioning
confidence: 99%