Step 1: Relate electric potential and electric field.
The electric field \(\vec{E}\) is related to the electric potential \(V\) by \(\vec{E} = -\vec{\nabla}V\). In one dimension, this is \(E = -dV/dr\).
Step 2: Apply the given condition.
We are given that the potential \(V\) is constant inside the sphere. If \(V\) is constant, its derivative with respect to position must be zero.
\[ \frac{dV}{dr} = 0 \implies E = 0 \]
So, the electric field inside the conductor is zero.
Step 3: Relate electric field to charge distribution using Gauss's Law.
Gauss's Law in differential form (Poisson's equation) is \(\vec{\nabla} \cdot \vec{E} = \rho/\epsilon_0\), where \(\rho\) is the volume charge density.
Since \(\vec{E} = 0\) everywhere inside the sphere, its divergence \(\vec{\nabla} \cdot \vec{E}\) must also be zero.
\[ \vec{\nabla} \cdot (0) = 0 \implies \frac{\rho}{\epsilon_0} = 0 \implies \rho = 0 \]
This means there is no net charge at any point inside the volume of the conductor. Any net charge on a conductor must reside on its surface.