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Thomson problemThe Thomson problem is that of determining the minimum (ground state) energy configuration of N classical electrons on the surface of the 2-sphere S2 . The electrons repel each other with a force given by Coulomb's law. This problem is named for J. J. Thomson, who posed it in 1904 as part of the development of the plum pudding model of the atom. In this model, the electrons formed spherical shells. This one hundred year old puzzle (Thomson wrote "I have not as yet succeeded in getting a general solution") has many important physical realizations including multi-electron bubbles and the surface ordering of liquid metal drops confined in Paul traps. The Thomson problem is solved exactly for a few particles on the sphere and the energy per particle is known for a large number of particles on the surface of the sphere. Numerical results provide the best known solutions for a wide range of particle numbers. The configurations that are found have a great variety of geometrical structure. Additional recommended knowledgeOne can also ask for ground states of particles interacting with arbitrary potentials: this is the generalized Thomson problem. The generalized Thomson problem arises, for example, in determining the arrangements of the protein subunits which comprise the shells of spherical viruses. The "particles" in this application are clusters of protein subunits arranged on a shell. Other realizations include regular arrangements of colloid particles in colloidosomes, proposed for encapsulation of active ingredients such as drugs, nutrients or living cells, fullerene patterns of carbon atoms, and VSEPR Theory. An example with long range logarithmic interactions is provided by the Abrikosov vortices which would form at low temperatures in a superconducting metal shell with a large monopole at the center. The Thomson problem is of outstanding mathematical interest not only for the asymptotics (large N behavior) of the growth of minimum energy configurations but also for the characteristics of the minimum energy configurations themselves. Minimum Energy Configuration for Coulomb Potential
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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Thomson_problem". A list of authors is available in Wikipedia. |