What are the methods to manipulate a gradient? Vector Calc has been a while, and I can't seem to find anything about this online. How can I solve for D in an equation like so: $$\nabla\cdot D = \rho_v$$
How do I "move" the gradient to the other side?
 A: Depending on smoothness and boundary conditions there may or may not be a solution and it is not uniquely determined since you can add any divergence-free field and still satisfy the PDE.
Helmholtz's theorem states that any sufficiently smooth vector field $\mathbf{D}$ that decays sufficiently fast can be decomposed  into curl-free and divergence-free components of the form
$$\mathbf{D} = \nabla \phi + \nabla \times\mathbf{A}.$$
Hence,
$$\nabla \cdot \mathbf{D} = \nabla \cdot \nabla \phi + \nabla \cdot \nabla \times \mathbf{A} = \nabla^2\phi,$$
and $\phi$ must be a solution of the Poisson equation
$$\nabla^2 \phi = \rho_v.$$
Given suitable boundary conditions a unique solution for $\phi$ can be obtained leaving $\mathbf{D}$ determined up to the addition of an arbitrary divergence free field. 
On an unbounded domain for well-behaved $\rho_v$ we have the solution
$$\phi(\mathbb{x}) = \frac{-1}{4 \pi}\int_{\mathbb{R}^3} \frac{\rho_v(\mathbb{x}')}{|\mathbb{x} - \mathbb{x}'|}d\, \mathbb{x}'.$$
Ignoring the divergence-free part, this effectively "moves" $\nabla$ to the other side:
$$\mathbf{D} = \frac{-1}{4 \pi} \nabla \int_{\mathbb{R}^3} \frac{\rho_v(\mathbb{x}')}{|\mathbb{x} - \mathbb{x}'|}d\, \mathbb{x}'.$$
In physical terms,if $\rho_v$ is the electric charge distribution, then the integral is the electric potential and the electric field $\mathbf{D}$ is the gradient of the potential.
