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M1 RK1 and FLD: model comparisons

All eight problems compare both closures at the same refinement level and physical time. Partial pairs remain visible while their partner is pending. References are attached to the model they describe.

M1 and FLD solve different transport closures. Both updates are first order in time. A small model discrepancy does not establish accuracy against an exact solution. M1 evolves radiation flux; FLD reconstructs diagnostic flux from its energy gradient. Flux differences are not errors in a shared radiation-momentum conservation law. FLD uses physical light speed on the CPU. Moving cases include gas transport and radiation force/work; their derived lab-frame flux includes radiation enthalpy advection.

ProblemAvailable referenceComparison status
Streaming Wavefree-streaming analytic profile (M1); no supplied FLD spatial analytic reference (FLD)L2: matched; L3: matched; L4: pending
Streaming Frontfree-streaming analytic profile (M1); no supplied FLD spatial analytic reference (FLD)L2: matched; L3: awaiting matching method; L4: pending
Gaussian Pulselinearized analytic reference (M1); periodic constant-diffusion analytic reference (FLD limit)L2: matched; L3: pending; L4: pending
Equilibrium Spherediffusion-limit analytic reference (M1); steady Gaussian-emitter diffusion-limit analytic reference (FLD limit)L2: matched; L3: pending; L4: pending
Subcritical Shockno supplied analytic or digitized numerical profile (M1); no supplied independent reference profile (FLD)L2: matched; L3: pending; L4: pending
Supercritical Shockno supplied analytic or digitized numerical profile (M1); no supplied independent reference profile (FLD)L2: matched; L3: pending; L4: pending
Radiating Blastno supplied analytic or digitized numerical profile (M1); no supplied independent reference profile (FLD)L2: matched; L3: pending; L4: pending
MarshakSu–Olson diffusion reference (M1); Su–Olson linear diffusion analytic reference (FLD limit)L2: matched; L3: pending; L4: pending

Comparison manifest (JSON)