The stress tensor describes the traction across oriented surfaces in a continuum. In the convention used here, a unit normal gives traction
. For linear isotropic elasticity with displacement
, its constitutive relation is
where
is the infinitesimal strain tensor and
are the Lamé coefficients. In the absence of
a body force, static equilibrium requires
. Boundary displacement-to-traction
data define the Dirichlet-to-Neumann
operator of this system.