Systematic Derivation of Jump Conditions for the Immersed Interface Method in Three-Dimensional Flow Simulation

In this paper, we systematically derive jump conditions for the immersed interface method [SIAM J. Numer. Anal., 31 (1994), pp. 1019-1044; SIAM J. Sci. Comput., 18 (1997), pp. 709-735] to simulate three-dimensional incompressible viscous flows subject to moving surfaces. The surfaces are represented as singular forces in the Navier--Stokes equations, which give rise to discontinuities of flow quantities. The principal jump conditions across a closed surface of the velocity, the pressure, and their normal derivatives have been derived by Lai and Li [Appl. Math. Lett., 14 (2001), pp. 149-154]. In this paper, we first extend their derivation to generalized surface parametrization. Starting from the principal jump conditions, we then derive the jump conditions of all first-, second-, and third-order spatial derivatives of the velocity and the pressure. We also derive the jump conditions of first- and second-order temporal derivatives of the velocity. Using these jump conditions, the immersed interface method is applicable to the simulation of three-dimensional incompressible viscous flows subject to moving surfaces, where near the surfaces the first- and second-order spatial derivatives of the velocity and the pressure can be discretized with, respectively, third- and second-order accuracy, and the first-order temporal derivatives of the velocity can be discretized with second-order accuracy.

[1]  J. L U Mley Turbulence over a compliant surface: numerical simulation and analysis , 2003 .

[2]  Mohamed Gad-el-Hak,et al.  Compliant coatings: The simpler alternative , 1998 .

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

[4]  L. Greengard,et al.  A Fast Poisson Solver for Complex Geometries , 1995 .

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

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

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

[8]  D. Calhoun A Cartesian Grid Method for Solving the Two-Dimensional Streamfunction-Vorticity Equations in Irregular Regions , 2002 .

[9]  K. Bube,et al.  The Immersed Interface Method for Nonlinear Differential Equations with Discontinuous Coefficients and Singular Sources , 1998 .

[10]  Charles S. Peskin,et al.  Improved Volume Conservation in the Computation of Flows with Immersed Elastic Boundaries , 1993 .

[11]  Adrian L. R. Thomas,et al.  Leading-edge vortices in insect flight , 1996, Nature.

[12]  Randall J. LeVeque,et al.  Immersed Interface Methods for Stokes Flow with Elastic Boundaries or Surface Tension , 1997, SIAM J. Sci. Comput..

[13]  R. LeVeque,et al.  A comparison of the extended finite element method with the immersed interface method for elliptic equations with discontinuous coefficients and singular sources , 2006 .

[14]  M. Minion,et al.  The Blob Projection Method for Immersed Boundary Problems , 2000 .

[15]  Charles S. Peskin,et al.  Modeling Arteriolar Flow and Mass Transport Using the Immersed Boundary Method , 1998 .

[16]  Andreas Wiegmann,et al.  The Explicit-Jump Immersed Interface Method: Finite Difference Methods for PDEs with Piecewise Smooth Solutions , 2000, SIAM J. Numer. Anal..

[17]  S. N. Fry,et al.  The Aerodynamics of Free-Flight Maneuvers in Drosophila , 2003, Science.

[18]  M. Berger,et al.  An Adaptive Version of the Immersed Boundary Method , 1999 .

[19]  Charles S. Peskin,et al.  Stability and Instability in the Computation of Flows with Moving Immersed Boundaries: A Comparison of Three Methods , 1992, SIAM J. Sci. Comput..

[20]  H. S. Udaykumar,et al.  A Sharp Interface Cartesian Grid Methodfor Simulating Flows with ComplexMoving Boundaries , 2001 .

[21]  L. Fauci,et al.  A computational model of aquatic animal locomotion , 1988 .

[22]  C. Peskin,et al.  A three-dimensional computational method for blood flow in the heart. 1. Immersed elastic fibers in a viscous incompressible fluid , 1989 .

[23]  M. Dickinson,et al.  Wing rotation and the aerodynamic basis of insect flight. , 1999, Science.

[24]  R. LeVeque,et al.  Analysis of a one-dimensional model for the immersed boundary method , 1992 .

[25]  A. Mayo The Fast Solution of Poisson’s and the Biharmonic Equations on Irregular Regions , 1984 .

[26]  Z. J. Wang Vortex shedding and frequency selection in flapping flight , 2000, Journal of Fluid Mechanics.

[27]  Z. J. Wang,et al.  A cartesian grid method for modeling multiple moving objects in 2D incompressible viscous flow , 2003 .

[28]  Robert L. Ash,et al.  Effect of compliant wall motion on turbulent boundary layers , 1977 .

[29]  Z. Jane Wang,et al.  An immersed interface method for simulating the interaction of a fluid with moving boundaries , 2006, J. Comput. Phys..

[30]  James P. Keener,et al.  Immersed Interface Methods for Neumann and Related Problems in Two and Three Dimensions , 2000, SIAM J. Sci. Comput..

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

[32]  Christopher Davies,et al.  Hydrodynamics and compliant walls: does the dolphin have a secret? , 2000 .

[33]  Zhilin Li,et al.  A remark on jump conditions for the three-dimensional Navier-Stokes equations involving an immersed moving membrane , 2001, Appl. Math. Lett..

[34]  A. Fogelson,et al.  A fast numerical method for solving the three-dimensional Stokes' equations in the presence of suspended particles , 1988 .

[35]  C. Peskin,et al.  Simulation of a Flapping Flexible Filament in a Flowing Soap Film by the Immersed Boundary Method , 2002 .

[36]  M. Dickinson,et al.  Spanwise flow and the attachment of the leading-edge vortex on insect wings , 2001, Nature.