Changes between Version 52 and Version 53 of u/erica/LowResMHDShearFlows
- Timestamp:
- 06/03/14 13:46:04 (11 years ago)
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u/erica/LowResMHDShearFlows
v52 v53 41 41 [[Image(xz_plane_rho.gif, 25%)]] 42 42 43 For production runs, the domain needs to be extended in x so that the sheared interface doesn't reach the boundaries. 43 44 45 '''Instabilities''': Beta = 1 is too strong of a field, as it completely prevents formation of the 3 instabilities relevant to molecular cloud formation; thermal instabilities, kelvin helmoltz waves, and the NTSI are all absent in the strong field case. The NTSI seems to be strongest in the hydro case, and KH seems to increase in strength with increasing shear angle. 44 46 45 47 == Column Density Maps == 46 48 47 These column density maps are made by summing the density over all cells through a given dimension, using both the gas and sink components . You can use the above 3D plot for orientation. In the 'down the barrel case', the vertical dimension is z, and the horizontal axis is y. The axes are given in the other plots.49 These column density maps are made by summing the density over all cells through a given dimension, using both the gas and sink components of mass/cell. Recall, the interface is rotated about y (as can be seen in above [http://astrobear.pas.rochester.edu/trac/wiki/u/erica/LowResMHDShearFlows?action=edit#OrientationofCollisionInterface plot]). In the 'down the barrel case', the vertical dimension is z, and the horizontal axis is y. The axes are given in the other plots. 48 50 49 51 ''''Down the Barrel'''' … … 107 109 And here are the 3 different initial conditions for orientation: 108 110 109 Bx 111 Bx, By, Bz 110 112 111 113 [[Image(Bx_Init.png, 25%)]] 112 113 By114 115 114 [[Image(By_Init.png, 25%)]] 116 117 Bz118 119 115 [[Image(Bz_Init.png, 25%)]] 120 116