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MFC
Exascale flow solver
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Contains module m_reactive_burn. More...
Go to the source code of this file.
Modules | |
| module | m_reactive_burn |
| Condensed-phase reactive burn: a pressure-driven programmed-burn source that converts a "reactant" fluid into a "product" fluid on the multi-fluid model (num_fluids=2, chemistry='F'). The two fluids share the same stiffened-gas EOS (gamma, pi_inf) and differ only in their reference energy qv, so the reactant->product conversion releases (qv_reactant - qv_product) per unit mass through the mixture EOS with no explicit energy source. Because the two fluids are mechanically identical the volume-fraction swap is exact (the product volume fraction is the reaction progress), making this a reactive-Euler/ZND detonation model expressed through the diffuse-interface framework. A shock raises the pressure above rburnpign, the reactant burns, and the energy release sustains the shock – a self-propagating condensed-phase detonation. | |
Functions/Subroutines | |
| subroutine | m_reactive_burn::s_burn_rate (pres, lambda, alpha_rho_react, alpha_react, rate) |
| Programmed-burn rate dlambda/dt for one cell state. Both the RHS source and the operator-split integrator call this, so the rate law is stated once. | |
| subroutine, public | m_reactive_burn::s_compute_reactive_burn (rhs_vf, q_cons_vf, q_prim_vf, bounds) |
| Add the programmed-burn reaction source to the continuity and volume-fraction RHS. | |
| subroutine, public | m_reactive_burn::s_reactive_burn_substep (q_cons_vf, dtime, bounds) |
| Operator-split alternative to s_compute_reactive_burn, used when rburnsubsteps > 0. The flow is frozen and the burn ODE is integrated over one time step in equal sub-steps, so the reaction time scale is decoupled from the acoustic CFL. The mixture pressure is re-evaluated from the frozen internal energy each sub-step, which is what carries the rate's own feedback: the coefficients move as the reactant becomes product. | |
Contains module m_reactive_burn.
Definition in file m_reactive_burn.fpp.f90.