Why is the continuity equation hardly used in solid mechanics when it is essential in fluid mechanics? For any continuum, fluid or solid, we can express mass conservation through the continuity equation
$$\frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0 ,$$
where $\rho$ is density and $\mathbf{v}$ is velocity. We can also express momentum conservation through the Cauchy momentum equation
$$\frac{\partial \rho \mathbf{v}}{\partial t} + \nabla \cdot (\rho\mathbf{v}\mathbf{v}) = \nabla \cdot \mathbf{\sigma} + \mathbf{f} ,$$
where $\mathbf{\sigma}$ is the stress tensor and $\mathbf{f}$ is the body force density. Fluids and solids only differ in their stress tensor: In fluids, the stress is determined by the strain rate and pressure, giving the Navier-Stokes equation, while in solids (assuming linear elasticity), the stress is determined by the strain.
In fluid mechanics, both these equations are essential and very much used, often in an incompressible form where the density $\rho$ is assumed constant and the continuity equation hence becomes $\nabla \cdot \mathbf{v} = 0$. However, the continuity equation hardly seems to be used in solid mechanics. I have searched through a few books on elasticity, continuum mechanics, and waves in solids, and the continuity equation seems only to be mentioned in the context of fluid mechanics.
Why is it, then, that the continuity equation is essential in fluid mechanics but not in solid mechanics, when both solids and fluids are continua, governed by the same fundamental equations?
 A: The simplest formulation for almost all solid mechanics modelling is Lagrangian, not Eulerian. You are considering the motion of an element of the structure which has constant mass, and therefore mass conservation is "baked in" to the model. You don't need an equation to represent it.
The continuity equation would determine the local density distribution of the deformed solid, but since plastic deformation takes place at constant volume, unless the material can have large elastic strains the density changes will usually be small and are not interesting from a practical point of view. If you don't care about density changes, you don't need the continuity equation to calculate them.
There are some situations where an Eulerian formulation is useful to avoid numerical problems with large plastic deformations, but they usually involve some sort of "re-meshing" algorithm, not the fluid mechanics type of Eulerian formulation.
The shape of boundary of a solid is determined by the fact that the material is a solid, unlike a fluid whose the shape is constrained by the boundary conditions imposed on the model. Trying to use a Eulerian type of discretization that is "fixed in space" isn't very useful for most solid modeling applications, because it doesn't accurately represent boundary of a solid object when it deforms.
