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Controlling Fluid Simulations with Custom Fields in Houdini Master ...

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Figure 8: The node tree show<strong>in</strong>g the body forces <strong>in</strong>side the preset smoke solver<strong>in</strong> Houd<strong>in</strong>i as discussed <strong>in</strong> (4.3.2)Pressure and Incompressibility (non-divergence)PressurepThe pressure can be considered as the uid from the area <strong>with</strong> high pressurethat will be pushed by the pressure towards the area <strong>with</strong> lower pressure. Thisforce is represented by the gradient of the pressure eld, p [18].The <strong>in</strong>compressibility condition∇ · −→ u = 0Another way to th<strong>in</strong>k about pressure is that it is whatever it takes to keepthe velocity divergence-free so the <strong>in</strong>compressibility condition is satised [4].With<strong>in</strong> Houd<strong>in</strong>i these terms come <strong>in</strong> the shape of a Gas Project Non Divergentmicrosolver that removes any divergent portions of a velocity eld. Theseare parts of the velocity eld that represent expansion or contraction. Thisis done by comput<strong>in</strong>g a pressure eld that counteracts any compression andapply<strong>in</strong>g that pressure eld <strong>in</strong>stantaneously [16].4.3.3 Vorticity ConnementWhen simulations of stable uids are run, some of the velocity is lost due tonumerical dissipation which is the results of a necessary weighted averag<strong>in</strong>g step15

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