Summary of Scalings

On an accompanying Wiki page we have explained how to interpret the set of dimensionless units that Dominic Marcello is using in his rad-hydrocode. The following table summarizes some of the mathematical relationships that have been derived in that accompanying discussion.

General Relation

Case A:

<math> \frac{m_\mathrm{cgs}}{m_\mathrm{code}} </math>	<math> = </math>	<math> 0.4038~\mu_e^2 M_\mathrm{Ch} \biggl( \frac{\tilde{g}^3 \tilde{a}}{\tilde{r}^4 \bar{\mu}^4 } \biggr)^{1/2} </math>	<math>= ~~2.810\times 10^{33}~\mathrm{g} </math>
<math> \frac{\ell_\mathrm{cgs}}{\ell_\mathrm{code}} </math>	<math> = </math>	<math> 4.438\times 10^{-4}~ \mu_e \ell_\mathrm{Ch}~\biggl( \frac{\tilde{c}^4 \tilde{g} \tilde{a}} {\bar{\mu}^4 \tilde{r}^4} \biggr)^{1/2} </math>	<math>=~~ 8.179\times 10^{9}~\mathrm{cm}</math>
<math> \frac{t_\mathrm{cgs}}{t_\mathrm{code}} </math>	<math> = </math>	<math> 2.9261\times 10^{-6}~\mu_e^{1/2} t_\mathrm{Ch} ~\biggl( \frac{\tilde{c}^6 \tilde{g} \tilde{a}} {\bar{\mu}^4 \tilde{r}^4} \biggr)^{1/2} </math>	<math>= ~~54.1~\mathrm{s}</math>

where:

<math> \mu_e^2 M_\mathrm{Ch} = 1.14169\times 10^{34}~\mathrm{g} </math>; <math> \mu_e \ell_\mathrm{Ch} = 7.71311\times 10^{8}~\mathrm{cm} </math>; <math> \mu_e^{1/2} t_\mathrm{Ch} = 3.90812~\mathrm{s} </math>

Case A <math>\Rightarrow ~~~\tilde{g} = 1</math>; <math>\tilde{c} = 198</math>; <math>\tilde{r} = 0.44</math>; <math>\tilde{a} = 0.044</math>; <math>\bar\mu = 4/3</math>; <math>\rho_\mathrm{max} = 1</math>; <math>(\Delta R) = \frac{\pi}{128}</math>

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General Relation

Case A:

<math> f_\mathrm{Edd} \equiv \frac{L_\mathrm{acc}}{L_\mathrm{Edd}} </math>	<math> = </math>	<math> 1.25\times 10^{21} \biggl( \frac{\tilde{g}^{1/2} \tilde{r}^2 \bar{\mu}^2 }{\tilde{c}^5 \tilde{a}^{1/2}} \biggr) \biggl[ \frac{\dot{M}}{R_a} \biggr]_\mathrm{code} </math>	<math>= ~~6.74\times 10^9 \biggl[ \frac{\dot{M}}{R_a} \biggr]_\mathrm{code}</math>
<math> \frac{\rho_\mathrm{threshold}}{\rho_\mathrm{max}} \equiv \frac{1}{\rho_\mathrm{max}\kappa_\mathrm{T} (\Delta R)} </math>	<math> = </math>	<math> 5.164\times 10^{-21}~\biggl( \frac{\tilde{c}^4 \tilde{a}^{1/2}}{\bar{\mu}^2 \tilde{r}^2 \tilde{g}^{1/2}} \biggr) \biggl[ \frac{1}{\rho_\mathrm{max}(\Delta R)} \biggr]_\mathrm{code} </math>	<math>=~~ 4.83\times 10^{-12}</math>
<math> \Gamma \equiv \frac{P_\mathrm{gas}}{P_\mathrm{rad}} </math>	<math> = </math>	<math> 3 \biggl( \frac{\tilde{r}}{\bar{\mu} \tilde{a}} \biggr) \biggl[ \frac{ \rho }{T^3} \biggr]_\mathrm{code} </math>	<math>= ~~22.5 \biggl[ \frac{ \rho }{T^3} \biggr]_\mathrm{code}</math>
<math> \frac{v_\mathrm{circ}}{c} \equiv \frac{2\pi a_\mathrm{separation}}{c P_\mathrm{orbit}} </math>	<math> = </math>	<math> \frac{2\pi}{\tilde{c}} \biggl[\frac{a_\mathrm{sep}}{P_\mathrm{orb}}\biggr]_\mathrm{code} </math>	<math>= ~~0.032 \biggl[\frac{a_\mathrm{sep}}{P_\mathrm{orb}}\biggr]_\mathrm{code}</math>

Case A <math>\Rightarrow ~~~\tilde{g} = 1</math>; <math>\tilde{c} = 198</math>; <math>\tilde{r} = 0.44</math>; <math>\tilde{a} = 0.044</math>; <math>\bar\mu = 4/3</math>; <math>\rho_\mathrm{max} = 1</math>; <math>(\Delta R) = \frac{\pi}{128}</math>

Combining the above Case A relations with the RadHydro-code properties of the Q0.7 polytropic binary that serves as an initial condition for Dominic's simulations, we conclude the following:

(1) The system will experience "super-Eddington" accretion (i.e., <math>f_\mathrm{Edd} > 1</math>) when

<math> [\dot{M}]_\mathrm{code} > 1.3\times 10^{-10} . </math>

(2) The mean-free-path, <math>\ell_\mathrm{mfp}</math>, of a photon will be less than one grid cell <math>(\Delta R)_\mathrm{code}</math> when

<math> [\rho]_\mathrm{code} > \rho_\mathrm{threshold} = 5\times 10^{-12} . </math>

(3) The system is weakly relativistic because,

<math> \frac{v_\mathrm{circ}}{c} = 0.0026 . </math>

User:Tohline/Appendix/Ramblings/Radiation/SummaryScalings

Summary of Scalings

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