Just another though,
considering the surface of a conductor, we know the equipotential surfaces very neer the surface of the conductor is neerly the shape of that conductor.
Therefore, by knowing the equation of the surface we also know the equation of the equapotential lines neer the surface of the conductor.
(Getting to my point very soon)
Take a Conducting Sphere for example, We can represent the sphere in spherical coordinates by R, if I am correct I believe V varies by R.
Take a parallel plate capacitor, two plates parallel to the xy plane, one plate in the plane Z = 0 and Z = zi. essentially you can think of the surface of one of the capacitors as a constant function of Z.. and varies in the Z direction..
NOW the cone. A distinc surface of a cone is defined by keeping the angle θ between the +z-axis constant, hence V for distinct cones vary by θ in spherical coord.