Spectral element simulations of interactive particles in a fluid

Abstract This paper presents three-dimensional simulations of interactive particles in a fluid. The originality of this paper is the integrated Eulerian–Lagrangian algorithms implemented with high-order methods in both space and time for numerical solutions to Navier–Stokes equations with additional source terms. Implementation of fourth order Stiffly Stable Schemes was tested for time integration before they were used in computations. In order to provide the h p -type mesh refinement, for extra flexibility to achieve higher spatial resolution, a modal spectral element method was used to solve governing equations in three dimensions. Another originality is the efficiency in handling moving particles without adaptive or moving mesh. Simulation results were validated with experimental data and verified with exact solutions. In addition, numerical results were also compared with solutions at higher resolutions and good agreement was accomplished. Results indicate that algorithms and implementations are accurate and appropriate for investigating three dimensional interactive particles in a fluid involving many moving objects.

[1]  H. Kreiss,et al.  Time-Dependent Problems and Difference Methods , 1996 .

[2]  S. Orszag,et al.  Boundary conditions for incompressible flows , 1986 .

[3]  R. F. Boisvert,et al.  A boundary integral method for the simulation of two-dimensional particle coarsening , 1986 .

[4]  Steven A. Orszag,et al.  Boundary integral methods for axisymmetric and three-dimensional Rayleigh-Taylor instability problems , 1984 .

[5]  A. Ardekani,et al.  Interaction between a pair of particles settling in a stratified fluid. , 2013, Physical review. E, Statistical, nonlinear, and soft matter physics.

[6]  K. Park An Improved Stiffly Stable Method for Direct Integration of Nonlinear Structural Dynamic Equations , 1975 .

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

[8]  Y. Qian,et al.  Lattice BGK Models for Navier-Stokes Equation , 1992 .

[9]  G. Karniadakis,et al.  Spectral/hp Element Methods for Computational Fluid Dynamics , 2005 .

[10]  Ivo Babuska,et al.  The p and h-p Versions of the Finite Element Method, Basic Principles and Properties , 1994, SIAM Rev..

[11]  Moshe Dubiner Spectral methods on triangles and other domains , 1991 .

[12]  Robert Michael Kirby,et al.  Parallel Scientific Computing in C++ and MPI - A Seamless Approach to Parallel Algorithms and their Implementation , 2003 .

[13]  Yonglai Zheng,et al.  Simulation of flow around rigid vegetation stems with a fast method of high accuracy , 2016 .

[14]  M. G. Duffy,et al.  Quadrature Over a Pyramid or Cube of Integrands with a Singularity at a Vertex , 1982 .

[15]  Q. Chen,et al.  Grain-resolved simulation of micro-particle dynamics in shear and oscillatory flows , 2015 .

[16]  H. Bungartz,et al.  A Coupled Approach for Fluid Dynamic Problems Using the PDE Framework Peano , 2012 .

[17]  D. Joseph,et al.  Nonlinear mechanics of fluidization of beds of spherical particles , 1987, Journal of Fluid Mechanics.

[18]  G. Karniadakis,et al.  Simulations of dynamic self-assembly of paramagnetic microspheres in confined microgeometries , 2005 .

[19]  Thomas Y. Hou,et al.  Boundary integral methods for multicomponent fluids and multiphase materials , 2001 .

[20]  Howard H. Hu Direct simulation of flows of solid-liquid mixtures , 1996 .

[21]  P. K. Banerjee,et al.  Boundary element methods in engineering science , 1981 .

[22]  Timothy C. Warburton,et al.  Basis Functions for Triangular and Quadrilateral High-Order Elements , 1999, SIAM J. Sci. Comput..

[23]  D. Juric,et al.  A front-tracking method for the computations of multiphase flow , 2001 .

[24]  C. W. Gear,et al.  Numerical initial value problem~ in ordinary differential eqttations , 1971 .

[25]  L. Schwartz,et al.  A boundary-integral method for two-phase displacement in Hele-Shaw cells , 1986, Journal of Fluid Mechanics.

[26]  A. Ladd,et al.  Lattice-Boltzmann Simulations of Particle-Fluid Suspensions , 2001 .

[27]  Gretar Tryggvason,et al.  Dynamics of homogeneous bubbly flows Part 1. Rise velocity and microstructure of the bubbles , 2002, Journal of Fluid Mechanics.

[28]  Suhas V. Patankar,et al.  A NEW FINITE-DIFFERENCE SCHEME FOR PARABOLIC DIFFERENTIAL EQUATIONS , 1978 .

[29]  Tayfun E. Tezduyar,et al.  3D Simulation of fluid-particle interactions with the number of particles reaching 100 , 1997 .

[30]  M. Deville,et al.  Pressure and time treatment for Chebyshev spectral solution of a Stokes problem , 1984 .

[31]  Y. Wang,et al.  Spectral element modeling of sediment transport in shear flows , 2011 .

[32]  C. Peskin The Fluid Dynamics of Heart Valves: Experimental, Theoretical, and Computational Methods , 1982 .

[33]  T. A. Zang,et al.  Spectral methods for fluid dynamics , 1987 .

[34]  Dong Liu,et al.  Spectral distributed Lagrange multiplier method: algorithm and benchmark tests , 2004 .

[35]  R. Glowinski,et al.  A new formulation of the distributed Lagrange multiplier/fictitious domain method for particulate flows , 2000 .

[36]  M. Maxey,et al.  Localized force representations for particles sedimenting in Stokes flow , 2001 .

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

[38]  Don Liu,et al.  Modal Spectral Element Solutions to Incompressible Flows over Particles of Complex Shape , 2014, J. Comput. Eng..

[39]  Howard H. Hu,et al.  Direct numerical simulations of fluid-solid systems using the arbitrary Langrangian-Eulerian technique , 2001 .

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

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

[42]  George Em Karniadakis,et al.  Modeling and optimization of colloidal micro-pumps , 2004 .

[43]  Martin R. Maxey,et al.  A fast method for particulate microflows , 2002 .

[44]  Stefano Ubertini,et al.  A partitioned approach for two-dimensional fluid–structure interaction problems by a coupled lattice Boltzmann-finite element method with immersed boundary , 2014 .

[45]  Howard H. Hu,et al.  The dynamics of two spherical particles in a confined rotating flow: pedalling motion , 2008, Journal of Fluid Mechanics.

[46]  M. N. Spijker Stiffness in numerical initial-value problems , 1996 .

[47]  Charles S. Peskin,et al.  Two-Dimensional Simulations of Valveless Pumping Using the Immersed Boundary Method , 2001, SIAM J. Sci. Comput..

[48]  S. Orszag,et al.  High-order splitting methods for the incompressible Navier-Stokes equations , 1991 .

[49]  M. Ferdows,et al.  Spectral element simulations of three dimensional convective heat transfer , 2017 .

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

[51]  J. Tinsley Oden,et al.  Optimal h-p finite element methods , 1994 .

[52]  G. Tryggvason,et al.  A front-tracking method for viscous, incompressible, multi-fluid flows , 1992 .

[53]  D. Liu,et al.  Force-coupling method for flows with ellipsoidal particles , 2009, J. Comput. Phys..

[54]  J. Boon The Lattice Boltzmann Equation for Fluid Dynamics and Beyond , 2003 .

[55]  R. Glowinski,et al.  A distributed Lagrange multiplier/fictitious domain method for particulate flows , 1999 .

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