Correspondence between Electrostatics and Contact Mechanics with Further Results in Equilibrium Charge Distributions

It is common in mesoscopic systems to find instances where several charges interact among themselves. These particles are usually confined by an external potential that shapes the symmetry of the equilibrium charge configuration. In the case of classical charges moving on a plane and repelling each other via the Coulomb potential, they possess a ground state a la Thomson or Wigner crystal. As the number of particles N increases, the number of local minima grows exponentially and direct or heuristic optimization methods become prohibitively costly. Therefore the only feasible approximation to the problem is to treat the system in the continuum limit. Since the underlying framework is provided by potential theory, we shall by-pass the corresponding mathematical formalism and list the most common cases found in the literature. Then we prove a (albeit known) mathematical correspondence that will enable us to re-discover analytical results in electrostatics. In doing so, we shall provide different methods for finding the equilibrium surface density of charges, analytical and numerical. Additionally, new systems of confined charges in three-dimensional surfaces will be under scrutiny. Finally, we shall highlight exact results regarding a modified power-law Coulomb potential in the d-dimensional ball, thus generalizing the existing literature. The authors review the connections existing, based on potential theory, between contact mechanics and equilibrium electrostatics. This little known correspondence is exploited so that problems scattered in many works can be easily solved by bringing to light their "duals" in elastic theory. Numerical and analytic tools are extended to a variety of new results, for which the literature is blank.image