Advecting radiation pulse test
This test demonstrates the code's ability to deal with the relativistic correction source terms that arise from the mixed frame formulation of the RHD moment equations, in a fully-coupled RHD problem. The problems involve the advection of the a pulse of radiation energy in an optically thick (\(\tau \gg 1\)) gas in both static (\(\beta \tau \ll 1\)) and dynamic (\(\beta \tau \gg 1\)) diffusion regimes, with a uniform background flow velocity (Krumholz, Klein, McKee, & Bolstad, 2007)1.
Parameters
Initial condition of the problem in static diffusion regime:
The simulation is run till \(t_{\rm end} = 2 w/v = 4.8 \times 10^{-5} ~{\rm s}\).
Initial condition of the problem in dynamic diffusion regime: same parameters as in the static diffusion regime except
Results
Static diffusion regime:
radhydro_pulse_temperature-static-diffusion
radhydro_pulse_density-static-diffusion
radhydro_pulse_velocity-static-diffusion
Dynamic diffusion regime:
radhydro_pulse_temperature-dynamic-diffusion
radhydro_pulse_density-dynamic-diffusion
radhydro_pulse_velocity-dynamic-diffusion
-
Krumholz, M. R., Klein, R. I., McKee, C. F., & Bolstad, J. (2007). Equations and Algorithms for Mixed-frame Flux-limited Diffusion Radiation Hydrodynamics. The Astrophysical Journal, 667, 626–643. https://doi.org/10.1086/520791 ↩