1983
DOI: 10.1093/mnras/204.4.1269
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Numerical fits to important rates in high temperature astrophysical plasmas

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Cited by 175 publications
(179 citation statements)
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“…The pseudo-Newtonian potential is adopted in the momentum equation. q ei , q br and qsyn are the energy transfer rate from ions to electrons by Coulomb collisions, the cooling rate of electrons by electron-ion and electron-electron bremsstrahlungs and the synchrotron cooling rate, respectively (Esin et al 1996;Narayan & Yi 1995;Stepney & Guilbert 1983). In calculation of qsyn, we give the magnetic field B at each radius, assuming that the ratio β of the magnetic energy density to the thermal energy density is constant throughout the region.…”
Section: Basic Equationsmentioning
confidence: 99%
“…The pseudo-Newtonian potential is adopted in the momentum equation. q ei , q br and qsyn are the energy transfer rate from ions to electrons by Coulomb collisions, the cooling rate of electrons by electron-ion and electron-electron bremsstrahlungs and the synchrotron cooling rate, respectively (Esin et al 1996;Narayan & Yi 1995;Stepney & Guilbert 1983). In calculation of qsyn, we give the magnetic field B at each radius, assuming that the ratio β of the magnetic energy density to the thermal energy density is constant throughout the region.…”
Section: Basic Equationsmentioning
confidence: 99%
“…Following Stepney & Guilbert (1983), where the z-axis is chosen to be parallel to the sum of the initial electron momenta, we rewrite Eq. (1) as follows:…”
Section: Electron-electron Thermal Bremsstrahlungmentioning
confidence: 99%
“…The boundary values of T 1 , μ 1 , μ 2 and θ max are given in Appendix of Stepney & Guilbert (1983). Here it should be also noted that our definition of G(x, τ) in Eq.…”
Section: Electron-electron Thermal Bremsstrahlungmentioning
confidence: 99%
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