Consider a hypothetical linear stress-strain relation for an isotropic solid,

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

Invariance, Ch Index notation and Cartesian tensors

Problem

Consider a hypothetical linear stress-strain relation for an isotropic solid, σij=Cijklekl\sigma_{ij}=C_{ijkl}e_{kl}, where ekl=elke_{kl}=e_{lk} is the (symmetric) strain. Someone proposes adding, to the ordinary Lamé terms, an isotropic antisymmetric pieceCijklextra=κ (δikδjl−δilδjk)C^{\rm extra}_{ijkl}=\kappa\,(\delta_{ik}\delta_{jl}-\delta_{il}\delta_{jk})for some scalar κ\kappa. ((a)) Using the contracted Levi-Civita identity in the form δikδjl−δilδjk=ϵijmϵklm\delta_{ik}\delta_{jl}-\delta_{il}\delta_{jk}=\epsilon_{ijm}\epsilon_{klm}, write CijklextraeklC^{\rm extra}_{ijkl}e_{kl} as κ ϵijmwm\kappa\,\epsilon_{ijm}w_m for some vector wmw_m, and identify wmw_m in terms of ekle_{kl}. ((b)) Show that wm=0w_m=0 for any symmetric strain, so that this extra term never contributes to the stress. ((c)) Say in one sentence why this is consistent with the ordinary reduction of the elastic tensor to the two Lamé constants λ,μ\lambda,\mu.

Browse the problem library