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Hot Plasmas in Supernova Remnants

Published online by Cambridge University Press:  30 March 2016

F. D. Kahn*
Affiliation:
Department of Astronomy, University of Manchester

Extract

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Supernovae occur in highly evolved, massive stars and typically release 1051 to 1052 erg. Their light curves show that the stellar radius is about one A.U. at the time of the explosion. The typical energy density in the star is about 1011 or 1012erg cm-3 when the blast reaches the stellar surface. Much of the energy is present in thermal form. Since the density of the material is high, thermal equilibrium is attained rapidiy between the radiation field and the thermal motions. The temperature in the interior of the star becomes about 106K, and most of the energy is present in the form of radiation.

At this time the star has a large optical depth, of order 107. Therefore the effective diffusion speed for radiation is very low, about 3000 cm s-1. But the effective sound speed is large, of order 109 cm s-1, and the large input of energy has destroyed the gravitational equilibrium. So the star begins violently to expand, and the pressure of the stored radiation field does work in producing mass motion of the material. Only a small fraction of the radiant energy is released from the exploded star. The photosphere, in this phase, lies in the region where the gas changes from being ionized to non-ionized, so that the photo-spheric temperature remains low, of order 104K. There is little chance of observing any high-temperature phenomena at this stage in the evolution of a supernova.

Type
Joint Discussion
Copyright
Copyright © Cambridge University Press 1980

References

Comments and References

Woltjer, L. Annual Review Astron. Astrophys. 10, 129, 1972CrossRefGoogle Scholar
Kahn, F.D. 14th International Cosmic Ray Conference, volume 11, 3566, 1975 Google Scholar
Chevalier, R.A. discusses models of the supernova explosion and the nature of their photosphere in Astrophys. J. 207, 872, 1976.CrossRefGoogle Scholar
The definition of the various phases in the development of a remnant is discussed by Woltjer, (op. cit.).Google Scholar
Kamper, K. and S., v.d.Bergh give a detailed account of the structure of Cassiopaeia A in Astrophys. J. Supplement 32, 351, 1976.CrossRefGoogle Scholar
The Sedov solution is described in more detail by Kahn, (op.cit.).Google Scholar
Raymond, J.C., D.P., Cox and B.W., Smith describe the cooling of interstellar gas in Astrophys. J. 204, 290, 1976.CrossRefGoogle Scholar
The simple approximation to their calculated Л(Т) comes from Kahn, F.D., Astron. Astrophys. 50, 145, 1976.Google Scholar
A galactic corona, with somewhat smaller density than adopted here, is described by Chevalier, R.A. and Oergerle, R. in Astrophys. J. 227, 398, 1979.CrossRefGoogle Scholar
Isothermal rather than adiabatic remnants were first discussed in detail by Solinger, A., S.Rappaport, and Buff, J. in Astrophys. J. 201, 381, 1875.CrossRefGoogle Scholar
But Cowie, L.L. later considered some of the restrictions on thermal conduction by electrons in Astrophys. J. 215, 226, 1977 CrossRefGoogle Scholar
McKee, C.F., Cowie, L.L. and Ostriker, J.P. deal with the properties of inhomogeneous models of supernova remnants in Astrophys. J. 219, L23, 1978.CrossRefGoogle Scholar
The textbook “Electrodynamics of Particles and Plasmas” (Addison Wesley, 1969) by Clemmow, P.C. and Dougherty, J.P. contains a section (11.5) on plasma transport processes, and deals with the mirror instability in section 11.6.3.Google Scholar
For some primitive ideas on the ionization and evaporation of dense clouds in interstellar space see Kahn, F.D., Physica 41, 172, 1969.CrossRefGoogle Scholar