By Kang M., Fedkiw R. P., Liu X.
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Extra info for A Boundary Condition Capturing Method for Multiphase Incompressible Flow
Time:12:59 LOP8M. B. Page 01:01 Codes: 1224 Signs: 780 . Length: 44 pic 2 pts, 186 mm 354 Kang, Fedkiw, and Liu We emphasize that the higher degree of instability demonstrated by the GFM is due to the more accurate interface representation and not due to nonphysical parasitic flows. 01 m centered in the middle of the domain. Here we set gravity to zero in order to demonstrate the ability of our scheme to accurately compute sharp pressure jumps across the interface using the numerical algorithm in .
77, 439 471. 17. , and Osher, S. (1994). A level set approach for computing solutions to incompressible two-phase flow. J. Comput. Phys. 114, 146 154. 18. Tau, E. Y. (1994). A second order projection method for the incompressible Navier Stokes equations in arbitrary domains. J. Comput. Phys. 115, 147 152. 19. Unverdi, S. , and Tryggvason, G. (1992). A front-tracking method for viscous, incompressible, multi-fluid flows. J. Comput. Phys. 100, 25 37.
Steady state air bubble Ghost Fluid Method. File: 854J 706032 . By:XX . Date:18:01:01 . Time:12:59 LOP8M. B. Page 01:01 Codes: 1395 Signs: 1019 . Length: 44 pic 2 pts, 186 mm Boundary Condition Capturing Method 355 results are comparable with the GFM even though the pressure is smeared out as shown in Fig. 12. 1 mÂs indicating that it is the delta function method that is more likely to suffer from nonphysical parasitic flows due to the nonphysical smearing of the interface. Note that the exact solution has an identically zero velocity field.