290 | | For the outflow pattern, the leading edge is bounded by intermediate shocks and the trailing edge is bounded by slow shocks. There are totally four slow mode shocks stemming from the Sweet-Parker region, as shown in the following figure.[[BR]][[BR]] |
291 | | |
292 | | The time evolution model can be given by the Semenov solution.[[BR]] |
293 | | |
294 | | |
| 290 | For the outflow pattern, the leading edge is bounded by intermediate shocks and the trailing edge is bounded by slow shocks(Petschek-type). There are totally four slow mode shocks stemming from the Sweet-Parker region, as shown in the following figure.[[BR]][[BR]] |
| 291 | [[Image(http://www.pas.rochester.edu/~shuleli/petschek_diagram.png, 50%)]][[BR]][[BR]] |
| 292 | The time evolution model can be given by the Semenov solution, which is obtained by assuming a large resistivity box at the stagnation point. See the following figure.[[BR]][[BR]] |
| 293 | [[Image(http://www.pas.rochester.edu/~shuleli/semenov_evolution.png, 50%)]][[BR]][[BR]] |
| 294 | The flow pattern for our setup is shown in the following plot:[[BR]][[BR]] |
| 295 | [[Image(http://www.pas.rochester.edu/~shuleli/hhc_flowpattern.png, 50%)]][[BR]][[BR]] |
| 296 | The 2-D mach number plot is shown below:[[BR]][[BR]] |
| 297 | [[Image(http://www.pas.rochester.edu/~shuleli/hhc_mach.png, 50%)]][[BR]][[BR]] |