| 142 | | Here we look at what post-shock temperature the simulation gives as a function of the effective resolution. The effective resolution = (# cells) x 2^(# AMR levels)^. For Tps I will use the highest temperature that I get from the simulation. |
| 143 | | ||= Effective Resolution =||= cells/lcool =||= Tps (10^3^ K) =|| |
| 144 | | ||= 100 =||= 10.68 =||= |
| 145 | | ||= 200 =||= 21.36 =||= |
| 146 | | ||= 400 =||= 42.71 =||= |
| 147 | | ||= 800 =||= 85.43 =||= |
| 148 | | ||= 1600 =||= 170.85 =||= |
| 149 | | ||= 3200 =||= 341.70 =||= |
| | 142 | Here we look at what post-shock temperature the simulation gives as a function of the effective resolution. The effective resolution = (# cells) x 2^(# AMR levels)^. For Tps I will use the highest temperature that I get from the simulation. The highest temperature always occurs early on in the simulation and then the post-shock temperature slowly decreases over time, but stays relatively constant at some lower temperature. |
| | 143 | ||= Effective Resolution =||= cells/lcool =||= Tps (10^3^ K) =||= Relative Error (%) =|| |
| | 144 | ||= 100 =||= 10.68 =||= 34.37 =||= 41.06 =|| |
| | 145 | ||= 200 =||= 21.36 =||= 37.11 =||= 36.36 =|| |
| | 146 | ||= 400 =||= 42.71 =||= 40.21 =||= 31.04 =|| |
| | 147 | ||= 800 =||= 85.43 =||= 43.68 =||= 25.09 =|| |
| | 148 | ||= 1600 =||= 170.85 =||= 46.66 =||= 19.98 =|| |
| | 149 | ||= 3200 =||= 341.70 =||= 49.25 =||= 15.54 =|| |
