In steady state, in a uniform conductor, the charge density within the body of the conductor is $0$. All net charge lies on the surface(s) of that conductor.
Proof:
In steady state, all derivatives with respect to time, vanish.
Thus, the continuity equation
$$\nabla \cdot \vec{J} + \frac{\partial \rho}{\partial t} = 0$$
becomes
$$\nabla \cdot \vec{J} = 0$$
The microscopic version of Ohm's law says
$$\vec{J} = \sigma\vec{E}$$
so
$$\nabla \cdot \sigma \vec{E} = 0$$
Expanding we get
$$(\nabla\sigma)\cdot\vec{E} + \sigma(\nabla\cdot\vec{E})=0$$
Wherever $\nabla\sigma=\vec{0}$, we have
$$\nabla\cdot\vec{E}=0$$
But from Gauss's Law
$$\nabla \cdot \vec{E} = \frac{\rho}{\epsilon_0}$$
where $\rho$ is the charge density.
So, wherever $\nabla\sigma=\vec{0}$, we have the charge density must be $0$ i.e.
$$\rho=0$$
If we assume that the conductor is uniform, the only places where $\nabla\sigma \ne \vec{0}$ are on the surfaces of the conductor.
Thus, in steady state (all time derivatives vanish) for a uniform conductor, the only location where we will find non-zero charge density is on the surfaces of the conductor.