Spitzer resistivity

The Spitzer resistivity, or its opposite the Spitzer conductivity first formulated by Lyman Spitzer in 1950,[1][2] is an equation showing the electrical resistance in a plasma decreases in proportion to the electron temperature as .

The Spitzer resistivity is a classical model of electrical resistivity commonly used in plasma physics, based upon electron-ion collisions.[3][4][5] It is given by:

where is the ionization of nuclei, is the electron mass, is the electric permittivity of free space, is the Coulomb logarithm, is Boltzmann's constant, and is the temperature in kelvins.

References

  1. Cohen, Robert S.; Spitzer, Jr., Lyman; McR. Routly, Paul (October 1950). "The Electrical Conductivity of an Ionized Gas" (PDF). Physical Review. 80 (2): 230–238. doi:10.1103/PhysRev.80.230.
  2. Spitzer, Jr., Lyman; Härm, Richard (March 1953). "Transport Phenomena in a completely ionized gas" (PDF). Physical Review. 89 (5): 977–981. doi:10.1103/PhysRev.89.977.
  3. Trintchouk, Fedor, Yamada, M., Ji, H., Kulsrud, R. M., Carter, T. A. (2003). "Measurement of the transverse Spitzer resistivity during collisional magnetic reconnection" (Submitted manuscript). Physics of Plasmas. 10: 319–322. doi:10.1063/1.1528612.
  4. Davies, J. R. (2003). "Electric and magnetic field generation and target heating by laser-generated fast electrons". Physical Review E. 68 (5): 056404. doi:10.1103/physreve.68.056404. PMID 14682891.
  5. Forest, C. B., Kupfer, K., Luce, T. C., Politzer, P. A., Lao, L. L., Wade, M. R., Whyte, D. G., Wroblewski, D. (1994). "Determination of the noninductive current profile in tokamak plasmas" (Submitted manuscript). Physical Review Letters. 73 (18): 2444–2447. doi:10.1103/physrevlett.73.2444. PMID 10057061.
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