All problem comparisons · Campaign
Streaming Wave: Euler and ADER2
Reference: exact analytic solution. Exact nonlinear M1 periodic-advection cell averages.
Coupled ADER2 accuracy remains under investigation. A completed run or a small difference does not establish uniform second-order accuracy.
Revision 6 validation limits. Streaming-wave temporal-order thresholds failed at limiter transitions even with resolved references. Optically thick radiation temporal probes remain unresolved under the unchanged 1e-12 measurement guard. Strict stiff coupled temporal tests have not been rerun for revision 6 and remain an open limitation.
Level 2
Euler (first order): complete results, parameters and reference discussion
Coupled ADER2: complete results, parameters and reference discussion
matched. No other refinement level or physical time is substituted for a missing partner.

Matched profile coordinates and values (CSV)
ADER2 minus Euler: slice discrepancy
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 3.974018e-02 | 4.133068e-02 | 4.785348e-02 |
| Radiation flux x | erg/(cm^2 s) | 6.368198e+08 | 6.623069e+08 | 7.668320e+08 |
| Radiation flux y | erg/(cm^2 s) | 9.552297e+08 | 9.934603e+08 | 1.150248e+09 |
| Radiation flux z | erg/(cm^2 s) | 3.184099e+08 | 3.311534e+08 | 3.834160e+08 |
Euler (first order) versus exact analytic solution
Area-weighted errors on this method’s original leaf slice.
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 5.075526e-02 | 6.418457e-02 | 1.191588e-01 |
| Radiation flux x | erg/(cm^2 s) | 8.133318e+08 | 1.028531e+09 | 1.909470e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.219998e+09 | 1.542796e+09 | 2.864204e+09 |
| Radiation flux z | erg/(cm^2 s) | 4.066659e+08 | 5.142654e+08 | 9.547348e+08 |
Solver-reported full-volume reference norms
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 5.075526e-02 | 6.418457e-02 | 1.191588e-01 |
| Radiation flux x | erg/(cm^2 s) | 8.133318e+08 | 1.028531e+09 | 1.909470e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.219998e+09 | 1.542796e+09 | 2.864204e+09 |
| Radiation flux z | erg/(cm^2 s) | 4.066659e+08 | 5.142654e+08 | 9.547348e+08 |
Source slice CSV · Run metadata
Coupled ADER2 versus exact analytic solution
Area-weighted errors on this method’s original leaf slice.
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 7.740758e-02 | 9.514244e-02 | 1.633612e-01 |
| Radiation flux x | erg/(cm^2 s) | 1.240424e+09 | 1.524618e+09 | 2.617795e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.860636e+09 | 2.286927e+09 | 3.926693e+09 |
| Radiation flux z | erg/(cm^2 s) | 6.202120e+08 | 7.623089e+08 | 1.308898e+09 |
Solver-reported full-volume reference norms
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 7.740758e-02 | 9.514244e-02 | 1.633612e-01 |
| Radiation flux x | erg/(cm^2 s) | 1.240424e+09 | 1.524618e+09 | 2.617795e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.860636e+09 | 2.286927e+09 | 3.926693e+09 |
| Radiation flux z | erg/(cm^2 s) | 6.202120e+08 | 7.623089e+08 | 1.308898e+09 |
Level 3
Euler (first order): complete results, parameters and reference discussion
Coupled ADER2: complete results, parameters and reference discussion
matched. No other refinement level or physical time is substituted for a missing partner.

Matched profile coordinates and values (CSV)
ADER2 minus Euler: slice discrepancy
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 3.523321e-02 | 3.847428e-02 | 7.191846e-02 |
| Radiation flux x | erg/(cm^2 s) | 5.645974e+08 | 6.165342e+08 | 1.152463e+09 |
| Radiation flux y | erg/(cm^2 s) | 8.468961e+08 | 9.248013e+08 | 1.728695e+09 |
| Radiation flux z | erg/(cm^2 s) | 2.822987e+08 | 3.082671e+08 | 5.762316e+08 |
Euler (first order) versus exact analytic solution
Area-weighted errors on this method’s original leaf slice.
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 4.639050e-02 | 5.446053e-02 | 1.012121e-01 |
| Radiation flux x | erg/(cm^2 s) | 7.433884e+08 | 8.727072e+08 | 1.621881e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.115083e+09 | 1.309061e+09 | 2.432821e+09 |
| Radiation flux z | erg/(cm^2 s) | 3.716942e+08 | 4.363536e+08 | 8.109404e+08 |
Solver-reported full-volume reference norms
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 4.639050e-02 | 5.446053e-02 | 1.012121e-01 |
| Radiation flux x | erg/(cm^2 s) | 7.433884e+08 | 8.727072e+08 | 1.621881e+09 |
| Radiation flux y | erg/(cm^2 s) | 1.115083e+09 | 1.309061e+09 | 2.432821e+09 |
| Radiation flux z | erg/(cm^2 s) | 3.716942e+08 | 4.363536e+08 | 8.109404e+08 |
Source slice CSV · Run metadata
Coupled ADER2 versus exact analytic solution
Area-weighted errors on this method’s original leaf slice.
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 2.988865e-02 | 3.420566e-02 | 6.205922e-02 |
| Radiation flux x | erg/(cm^2 s) | 4.789530e+08 | 5.481313e+08 | 9.944730e+08 |
| Radiation flux y | erg/(cm^2 s) | 7.184295e+08 | 8.221969e+08 | 1.491709e+09 |
| Radiation flux z | erg/(cm^2 s) | 2.394765e+08 | 2.740656e+08 | 4.972365e+08 |
Solver-reported full-volume reference norms
| Field | Units | L₁ | L₂ | L∞ |
|---|---|---|---|---|
| Radiation energy density | erg/cm^3 | 2.988865e-02 | 3.420566e-02 | 6.205922e-02 |
| Radiation flux x | erg/(cm^2 s) | 4.789530e+08 | 5.481313e+08 | 9.944730e+08 |
| Radiation flux y | erg/(cm^2 s) | 7.184295e+08 | 8.221969e+08 | 1.491709e+09 |
| Radiation flux z | erg/(cm^2 s) | 2.394765e+08 | 2.740656e+08 | 4.972365e+08 |
Level 4
Euler (first order): pending.
Coupled ADER2: pending.
How these comparisons are measured
All field values use the saved units (CGS for the seven original problems; normalized units for Marshak). The central profiles share x coordinates and the positive row adjacent to y = z = 0. Adaptive leaf-cell averages are prolonged as constants onto the finest common Cartesian x-y partition, with no extrapolation or time interpolation. Different leaf sizes may average different z extents adjacent to the plane. The plotted curves therefore represent the saved finite-volume slices.
Slice L₁ is mean absolute difference, L₂ is root-mean-square difference, and L∞ is maximum absolute difference, with area weighting. These are two-dimensional slice diagnostics. The separately labeled solver norms cover the full volume.
Each method uses its own saved cell-average reference where supplied; finer meshes can change the sampled reference.