3.3.5 Radiative Stars 3.3.6 Solutions

3.3.5 Radiative Stars 3.3.6 Solutions

3.3.5 Radiative stars • Repeat for mass continuity, energy generation and radiative energy transport to get 4 simultaneous eqs in the four indices α... • Determinant of matrix in LHS is: Denotes diffusive radiative transfer in energy transport equation; Drad ≠ 0. AS 4013 Stellar Physics 3.3.6 Solutions • Solutions of matrix equation are: AS 4013 Stellar Physics Page ‹#› 3.3.7 Convective stars • Energy transport by fully adiabatic convection gives: • Matrix equation becomes: • Slightly simpler determinant and solutions. AS 4013 Stellar Physics 3.3.8 Upper-main sequence stars • Dominant opacity source is electron scattering which is independent of ρ, T so n = s = 0. • Energy source is thermonuclear CNO cycle for which λ = 1 and ν ~ 15. • Equation of state: ideal gas (P ∝ ρT) so χρ=χΤ=1. • Substitute these values in equations for radiative stars to get: AS 4013 Stellar Physics Page ‹#› Upper MS stars • Hence for M > 1 MSun: • Not too bad: recall that L ∝ M3.6 for high-mass stars in binaries. • Average density falls, temperature rises with increasing mass. • But we’ve made some major approximations and haven’t solved any DEs! AS 4013 Stellar Physics Interlude: The Virial Theorem • Whole system is in equilibrium if hydrostatic equilibrium is satisfied at all r. • Hence get relation between average internal pressure and gravitational PE of whole system. AS 4013 Stellar Physics Page ‹#› Average internal pressure Volume-averaged Gravitational PE pressure of system Volume of system AS 4013 Stellar Physics Pressure: nonrelativistic gas Fundamentally important result! Means that tightly bound systems in hydrostatic equilibrium have high particle KE, i.e. they’re HOT. AS 4013 Stellar Physics Page ‹#› Pressure: ultra-relativistic gas • For a gas of ultra-relativistic particles: • As UR limit is approached, binding energy decreases and system is easily disrupted. AS 4013 Stellar Physics Common ultra-relativistic gases • Radiation-pressure dominated: • Pressure from photons, UR by definition! – e.g. supermassive stars. • Degenerate electron-pressure dominated: • If electron temperature becomes very high – e.g. massive white dwarfs. • Both to be discussed in more detail later. AS 4013 Stellar Physics Page ‹#›.

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