This is an interesting question.

__Non-Coulombic electrostatic potential and Gauss' Law__

The first point is, what would happen if Coulomb's force law went like 1/r^3?

It would completely change the nature of what we mean by electrostatics (and magnetism).

The famous Gauss' Law of electrostatics would not apply. Gauss's law says that if you take the electric field and calculate its ``flux" through a closed surface (like a sphere enclosing a point charge), the result is proportional to the total charge enclosed by the surface, no matter what the shape or size of the surface.

__This is only possible because we live in 3 spatial dimensions and the Coulomb force law is an inverse square law.__ (If we lived in 4 spatial dimensions, then Coulomb's law would have to be 1/r^3 in order for Gauss's Law to apply).

You can check that with a 1/r^3 Coulomb law, the flux from a point charge through a sphere of radius R falls off as 1/R (in reality the flux is independent of R).

__Field inside Meta__l

Having said that, let us still try to think of the academic question you've posed. Suppose the force law has this unphysical form and you put some positive charge on a solid metallic sphere. Now, here comes a key point -- what do you mean by a metal ? A metal or conductor is one with free charges (electrons) that can move around to cancel all electric field in the metal. If the field were not zero, the electrons would move around and current would flow until the fields cancelled out. So the answer to your question, namely, what is the field inside a solid metallic sphere once charges are put on it -- __it should still be zero.__

In fact, the charge on the sphere __would not __reside only on the surface. If it did, you could use your new Coulomb law and linear superposition to calculate the electric field inside the sphere and the answer is non-zero (this is easy to see).You should, in principle, be able to use the vanishing of the electric field inside the solid metallic sphere, and assuming linear superposition principle, to find what the charge distribution would have to be. This is not an easy exercise for the 1/r^3 potential, but would be interesting to attempt. The exercise has been done in the following article which appears not to be an open access paper:

https://aapt.scitation.org/doi/10.1119/1.1339279

f I find the result quoted in it I will post it here.