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biconic cusp
The biconic cusp was an early method for modeling plasma confinement.〔Containment in a cusped Plasma System, Dr. Harold Grad, NYO-9496〕 They were studied at the Courant Institute by Harold Grad in the late 1950s and early 1960s.
== Description ==
The magnetic fields in this system were made by electromagnets placed close together. This was a theoretical construct used to model how to contain plasma. The fields were made by two coils of wire facing one another. These electromagnets had poles which faced one another and in the center was a null point in the magnetic field. This was also termed a zero point field. These devices were explored theoretically by Dr. Harold Grad at NYU's Courant Institute in the late 1950s and early 1960s.〔J Berowitz, H Grad and H Rubin, in proceedings of the second United Nations International conference on peaceful uses of atomic energy, Geneva, 1958, Vol 31, Page 177〕〔Grad, H. Theory of Cusped Geometries, I. General Survey, NYO-7969, Inst. Math. Sci., N.Y.U., December 1, 1957〕〔Berkowitz, J., Theory of Cusped Geometries, II. Particle Losses, NYO-2530, Inst. Math. Sci., N.Y.U., January 6, 1959.〕 Because the fields were planar symmetric this plasma system was simple to model.
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