| 196 | |
| 197 | == Embedding clumps == |
| 198 | |
| 199 | Also looked at embedding clumps in flows that are in pressure equilibrium. Here the flow density sets the clump density and the clump density contrast. For a flow density of 1 part/cc the clumps have to be at 132 part/cc. For a flow density of 3 part/cc the contrast is around 10 so the clumps will be at 30 part/cc. |
| 200 | [[Image(eq_constrast.png, width=400)]] |
| 201 | |
| 202 | |
| 203 | Given the clump density we can calculate the jeans length for the clumps which effectively sets their maximum gravitational stable size. For a density of 1 part/cc this gives a jeans length of about 11 pc. Setting the clump radius to be < .1 Jeans length ensures that the clumps won't collapse. |
| 204 | |
| 205 | [[Image(eq_jeans_length.png, width=400)]] |
| 206 | |
| 207 | |
| 208 | And finally the desired mean density of the flow sets the filling fraction of clumps. For example for a flow density of 1 part/cc, a filling fraction of 2% will yield a mean flow density of 3.6. |
| 209 | |
| 210 | [[Image(mean_eq_density.png, width=400)]] |
| 211 | |
| 212 | |
| 213 | First run was an flow density of 1 which gives a clump density of 132 and a clump jeans length of about 11 pc. The radius was set to .1 jeans length so the clumps have a radius of 1 pc. And the mean density was set to 3 part/cc so the filling fraction is ~ 2% |
| 214 | |
| 215 | || IX || |
| 216 | || [[Image(clumpyflow100.png, width=400)]] || |
| 217 | || [attachment:clumpyflow100.gif movie] || |
| 218 | |
| 219 | Next we increased the mean density to 3 part/cc so that the density contrast would be 10 instead of ~100. However the mean density had to be increased to 5 to get a reasonable filling fraction of 5% |
| 220 | |
| 221 | || X || |
| 222 | || [[Image(clumpflow10.png, width=400)]] || |
| 223 | || [attachment:clumpyflow10.gif movie] || |
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