Lagrangian density of linear elastic solid I need the general expression for the lagrangian density of a linear elastic solid. I haven't been able to find this anywhere. Thanks.
 A: the Lagrangian density is $L=T-U$, the difference between the kinetic and potential energy density, as we're used to in all of mechanics. 
The kinetic energy density is $T = \rho v(x,y,z)^2/2$ where one has to calculate the density $\rho$ properly. The potential energy is more general and complicated,
$$U = \frac{1}{2} C_{ijkl}u_{ij}u_{kl}$$
where the tensor $C$ with four indices is called the elastic. The tensors $u$ are obtained from the displacement vectors as 
$$ u_{ij} = \frac{1}{2} (\partial_i u_j + \partial_j u_i) $$
Note that the density $\rho$ in the kinetic energy also depends on the displacement vectors, if you want to re-express it via the mass density at rest (without displacement).
For isotropic materials, 
$$ C_{ijkl} = \lambda \delta_{ij} \delta_{kl} + \mu (\delta_{ik} \delta_{jl} + \delta_{il} \delta_{jk} ) $$
where $\lambda$ and $\mu$ are known as Lamé constants. For more general (but linear) crystals, however, $C$ is a general tensor symmetric under the $ij$ exchange, $kl$ exchange, and the exchange of $ij$ and $kl$ as pairs.
