| 158 | |
| 159 | My next idea was to revert back to just DM cooling instead of the new Z cooling. Perhaps, the Z cooling routine is not implemented quite right, and there is some "double counting" for cooling strength or something like this. So here is a smaller data table where I used DM instead of Z. The improvement column is the decrease in relative error from the comparable Z cooling run. |
| 160 | |
| 161 | ||= Effective Resolution =||= cells/lcool =||= Tps (10^3^ K) =||= Relative Error (%) =||= Improvement =|| |
| 162 | ||= 800 =||= 85.43 =||= 47.65 =||= 18.28 =||= 6.81 =|| |
| 163 | ||= 1600 =||= 170.85 =||= 51.37 =||= 11.91 =||= 8.07 =|| |
| 164 | ||= 3200 =||= 341.70 =||= 53.30 =||= 8.60 =||= 6.94 =|| |
| 165 | ||= 6400 =||= 683.40 =||= 53.98 =||= 7.43 =||= 4.80 =|| |
| 166 | ||= 12800 =||= 1366.81 =||= 54.14 =||= 7.16 =||= 1.61 =|| |
| 167 | |
| 168 | The DM cooling gets closer to what I expect but the Tps is still a little low. In both cases, Tps seems to be converging to some other value different from my expected value of 58.3123. However, when I do a run with no cooling, I get post-shock temperatures reaching 58.3123, and some even higher...closer to 60.75 with just 100 cells and no AMR. |