Sources of spurious force oscillations from an immersed boundary method for moving-body problems

When a discrete-forcing immersed boundary method is applied to moving-body problems, it produces spurious force oscillations on a solid body. In the present study, we identify two sources of these force oscillations. One source is from the spatial discontinuity in the pressure across the immersed boundary when a grid point located inside a solid body becomes that of fluid with a body motion. The addition of mass source/sink together with momentum forcing proposed by Kim et al. [J. Kim, D. Kim, H. Choi, An immersed-boundary finite volume method for simulations of flow in complex geometries, Journal of Computational Physics 171 (2001) 132-150] reduces the spurious force oscillations by alleviating this pressure discontinuity. The other source is from the temporal discontinuity in the velocity at the grid points where fluid becomes solid with a body motion. The magnitude of velocity discontinuity decreases with decreasing the grid spacing near the immersed boundary. Four moving-body problems are simulated by varying the grid spacing at a fixed computational time step and at a constant CFL number, respectively. It is found that the spurious force oscillations decrease with decreasing the grid spacing and increasing the computational time step size, but they depend more on the grid spacing than on the computational time step size.

[1]  Elias Balaras,et al.  An embedded-boundary formulation for large-eddy simulation of turbulent flows interacting with moving boundaries , 2006, J. Comput. Phys..

[2]  M. Uhlmann An immersed boundary method with direct forcing for the simulation of particulate flows , 2005, 1809.08170.

[3]  L. Sirovich,et al.  Modeling a no-slip flow boundary with an external force field , 1993 .

[4]  Elias Balaras,et al.  A moving-least-squares reconstruction for embedded-boundary formulations , 2009, J. Comput. Phys..

[5]  P. Moin,et al.  Accurate Immersed-Boundary Reconstructions for Viscous Flow Simulations , 2009 .

[6]  G. Golub,et al.  Structured inverse eigenvalue problems , 2002, Acta Numerica.

[7]  C. Peskin Numerical analysis of blood flow in the heart , 1977 .

[8]  C. Peskin The immersed boundary method , 2002, Acta Numerica.

[9]  J. Ferziger,et al.  A ghost-cell immersed boundary method for flow in complex geometry , 2002 .

[10]  Haecheon Choi,et al.  Immersed boundary method for flow around an arbitrarily moving body , 2006, J. Comput. Phys..

[11]  Zhilin Li,et al.  The immersed interface method for the Navier-Stokes equations with singular forces , 2001 .

[12]  C. Peskin Flow patterns around heart valves: A numerical method , 1972 .

[13]  P. Queutey,et al.  A NUMERICAL SIMULATION OF VORTEX SHEDDING FROM AN OSCILLATING CIRCULAR CYLINDER , 2002 .

[14]  M. Lai,et al.  An Immersed Boundary Method with Formal Second-Order Accuracy and Reduced Numerical Viscosity , 2000 .

[15]  R. Verzicco,et al.  Combined Immersed-Boundary Finite-Difference Methods for Three-Dimensional Complex Flow Simulations , 2000 .

[16]  E. Balaras Modeling complex boundaries using an external force field on fixed Cartesian grids in large-eddy simulations , 2004 .

[17]  Z. J. Wang Two dimensional mechanism for insect hovering , 2000 .

[18]  Haecheon Choi,et al.  Two-dimensional mechanism of hovering flight by single flapping wing , 2007 .

[19]  Tim Colonius,et al.  The immersed boundary method: A projection approach , 2007, J. Comput. Phys..

[20]  Haecheon Choi,et al.  Numerical solutions of flow past a circular cylinder at Reynolds numbers up to 160 , 1998 .

[21]  Gianluca Iaccarino,et al.  IMMERSED BOUNDARY METHODS , 2005 .

[22]  Jungwoo Kim,et al.  An immersed-boundary finite-volume method for simulations of flow in complex geometries , 2001 .

[23]  F. Durst,et al.  Low-Reynolds-number flow around an oscillating circular cylinder at low Keulegan–Carpenter numbers , 1998, Journal of Fluid Mechanics.