Laplace's Equation is applied to determine the electric potential of a cone, with the potential varying primarily with the angle theta, which is the angle between the positive Z-axis and the cone's surface. The discussion highlights that the potential does not depend on the azimuthal angle phi or the radial distance r, as changes in these coordinates do not affect the potential when theta is held constant. The surface of the cone acts as an equipotential surface, meaning the electric field is perpendicular to it. The potential varies with theta because different cones, defined by distinct theta values, exhibit different potentials on their surfaces. This analysis is crucial for understanding the behavior of conductors and equipotential surfaces in electrostatics.