J. A. Santiago, G. Chacon-Acosta, O. Gonzalez-Gaxiola
Using classical differential geometry, the problem of elastic curves and surfaces in the presence of long-range interactions $\Phi$, is posed. Starting from a variational principle, the balance of elastic forces and the corresponding projections ${\bf n}_i\cdot \nabla\Phi$, are found. In the case of elastic surfaces, a force coupling the mean curvature with the external potential, $K\Phi$, appears; it is also present in the shape equation along the normal principal in the case of curves. The potential $\Phi$ contributes to the effective tension of curves and surfaces and also to the orbital torque. The confinement of a curve on a surface is also addressed, in such a case, the potential contributes to the normal force through the terms $-\kappa\Phi -{\bf n}\cdot \nabla\Phi$. In general, the equation of motion becomes integro-differential that must be numerically solved.
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http://arxiv.org/abs/1301.2217
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