Step 1: Establish the relationship between electric potential and electric field. The electric field \(\vec{E}\) is the negative gradient of the electric potential \(V\), expressed as \(\vec{E} = -\vec{abla}V\). In one dimension, this simplifies to \(E = -dV/dr\).
Step 2: Apply the given condition of constant potential. Given that the potential \(V\) is constant within the sphere, its derivative with respect to position is zero. Thus, \(dV/dr = 0\), which implies \(E = 0\). Consequently, the electric field inside the conductor is zero.
Step 3: Relate the electric field to charge distribution using Gauss's Law. Gauss's Law in differential form, also known as Poisson's equation, is \(\vec{abla} \cdot \vec{E} = \rho/\epsilon_0\), where \(\rho\) is the volume charge density. Since \(\vec{E} = 0\) throughout the interior of the sphere, its divergence, \(\vec{abla} \cdot \vec{E}\), must also be zero. This leads to \(\vec{abla} \cdot (0) = 0\), which means \(\rho/\epsilon_0 = 0\), and therefore \(\rho = 0\). This indicates that there is no net charge within the volume of the conductor. Any net charge present on a conductor must reside on its surface.