A compressible fluid particle model based on the Voronoi ...
A compressible fluid particle model based on the Voronoi ...
A compressible fluid particle model based on the Voronoi ...
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C<strong>on</strong>clusi<strong>on</strong>s<br />
-The discrete <str<strong>on</strong>g>model</str<strong>on</strong>g> formulated <strong>on</strong> physical grounds can be interpreted<br />
as a Lagrangian discretizati<strong>on</strong> of <strong>the</strong> c<strong>on</strong>tinuum Navier Stokes<br />
equati<strong>on</strong>s that preserves First and Sec<strong>on</strong>d law of <strong>the</strong>rmodynamics.<br />
Any physical reas<strong>on</strong>able <str<strong>on</strong>g>model</str<strong>on</strong>g> should be compatible with <strong>the</strong><br />
<strong>the</strong>rmodynamic laws.<br />
-In order to be able to include <strong>the</strong>rmal fluctuati<strong>on</strong>s in any <str<strong>on</strong>g>model</str<strong>on</strong>g> we have<br />
to be sure that <strong>the</strong> dissipative matrix M(x) of <strong>the</strong> irreversible dynamics is<br />
positive definite.<br />
-In order to be able to exploit <strong>the</strong> Lagrangian power of <strong>the</strong> techniques for<br />
applicati<strong>on</strong>s to complex <str<strong>on</strong>g>fluid</str<strong>on</strong>g>s some more <strong>the</strong>oretical work has to be<br />
d<strong>on</strong>e to get good discrete versi<strong>on</strong>s of <strong>the</strong> sec<strong>on</strong>d derivative operators<br />
in n<strong>on</strong> uniform grids.