Crystals stirred up: 1. Direct numerical simulations of crystal settling in nondilute magmatic suspensions

[1] This is the first paper in a two-part series examining the fluid dynamics of crystal settling and flotation in the lunar magma ocean. A key challenge in constraining solidification processes is determining the ability of individual crystals to decouple from vigorous thermal convection and settle out or float. The goal of this paper is to develop a computational methodology capable of capturing the complex solid-fluid interactions that determine settling and flotation. In the second paper, we use this computational approach to explore the conditions under which plagioclase feldspar would be able to buoyantly float and form the earliest crust on the Moon. The direct numerical method described in this paper relies on a fictitious domain approach and captures solid-body motion in 2D and 3D with little overhead beyond single fluid calculations. The two main innovations of our numerical implementation of a fictitious domain approach are an analytical quadrature scheme, which increases accuracy and reduces computational expense, and the derivation of a multibody collision scheme. Advantages of this approach over previous simulations of crystal-bearing magmatic suspensions include the following: (1) we fully resolve the two-way interaction between fluid and solid phases, implying that crystals are not only passively advected in an ambient flow field but are also actively driving flow, and (2) we resolve the flow around each individual crystal without assuming specific settling speeds or drag coefficients. We present several benchmark problems and convergence tests to validate our approach.

[1]  J. Sethian,et al.  Crystals stirred up: 2. Numerical insights into the formation of the earliest crust on the Moon , 2012 .

[2]  D. May,et al.  Numerical modelling of magma transport in dykes , 2012 .

[3]  L. Caricchi,et al.  Potential causes for the non‐Newtonian rheology of crystal‐bearing magmas , 2010 .

[4]  Jean-Christophe Nave,et al.  It takes three to tango: 1. Simulating buoyancy‐driven flow in the presence of large viscosity contrasts , 2010 .

[5]  B. Kaus,et al.  Direct numerical simulation of two-phase flow: Effective rheology and flow patterns of particle suspensions , 2010 .

[6]  J. Schmalzl,et al.  A numerical method for investigating crystal settling in convecting magma chambers , 2009 .

[7]  Mathieu Martin,et al.  A numerical method for fully resolved simulation (FRS) of rigid particle-flow interactions in complex flows , 2009, J. Comput. Phys..

[8]  Boris J. P. Kaus,et al.  Comparison of Eulerian and Lagrangian numerical techniques for the Stokes equations in the presence of strongly varying viscosity , 2008 .

[9]  P. Ruprecht,et al.  Modeling of gas‐driven magmatic overturn: Tracking of phenocryst dispersal and gathering during magma mixing , 2008 .

[10]  Rajat Mittal,et al.  A versatile sharp interface immersed boundary method for incompressible flows with complex boundaries , 2008, J. Comput. Phys..

[11]  Marcin Dabrowski,et al.  MILAMIN: MATLAB‐based finite element method solver for large problems , 2008 .

[12]  Cin-Ty A. Lee,et al.  Paleo-viscometry of magma bodies , 2008 .

[13]  R. Rangel,et al.  Numerical investigation of particle–particle and particle–wall collisions in a viscous fluid , 2008, Journal of Fluid Mechanics.

[14]  Jianren Fan,et al.  A modified immersed boundary method for simulations of fluid–particle interactions , 2007 .

[15]  David A. Yuen,et al.  Robust characteristics method for modelling multiphase visco-elasto-plastic thermo-mechanical problems , 2007 .

[16]  Krishnaswamy Nandakumar,et al.  A fictitious domain formulation for flows with rigid particles: A non-Lagrange multiplier version , 2007, J. Comput. Phys..

[17]  J. Schmalzl,et al.  Dynamics of metal‐silicate separation in a terrestrial magma ocean , 2006 .

[18]  Roberto Zenit,et al.  A note on the modelling of the bouncing of spherical drops or solid spheres on a wall in viscous fluid , 2006 .

[19]  John F. Brady,et al.  STOKESIAN DYNAMICS , 2006 .

[20]  J. Schmalzl,et al.  Formation of compositional structures by sedimentation in vigorous convection , 2005 .

[21]  Andrea Prosperetti,et al.  A second-order method for three-dimensional particle simulation , 2005 .

[22]  H. Udaykumar,et al.  Sharp interface Cartesian grid method I: An easily implemented technique for 3D moving boundary computations , 2005 .

[23]  Dominique Legendre,et al.  Experimental study of a drop bouncing on a wall in a liquid , 2005 .

[24]  N. Patankar,et al.  A fast computation technique for the direct numerical simulation of rigid particulate flows , 2005 .

[25]  J. Bec,et al.  Clustering and collisions of heavy particles in random smooth flows , 2004, nlin/0407013.

[26]  Z. Feng,et al.  Proteus: a direct forcing method in the simulations of particulate flows , 2005 .

[27]  David A. Yuen,et al.  Characteristics-based marker-in-cell method with conservative finite-differences schemes for modeling geological flows with strongly variable transport properties , 2003 .

[28]  J. Derksen Numerical Simulation of Solids Suspension in a Stirred Tank , 2003 .

[29]  Yuri Y. Podladchikov,et al.  Analytical solutions for deformable elliptical inclusions in general shear , 2003 .

[30]  A. Burgisser,et al.  Reconciling Pyroclastic Flow and Surge: the Multiphase Physics of Pyroclastic Density Currents. , 2002 .

[31]  Philippe Gondret,et al.  Bouncing motion of spherical particles in fluids , 2002 .

[32]  D. Joseph,et al.  Modeling and numerical simulation of particulate flows by the Eulerian–Lagrangian approach , 2001 .

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

[34]  M. Manga,et al.  The yield strength of subliquidus basalts — experimental results , 2001 .

[35]  R. Glowinski,et al.  A fictitious domain approach to the direct numerical simulation of incompressible viscous flow past moving rigid bodies: application to particulate flow , 2001 .

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

[37]  Martin O. Saar,et al.  Numerical models of the onset of yield strength in crystal–melt suspensions , 2001 .

[38]  N. Patankar A formulation for fast computations of rigid particulate flows , 2001 .

[39]  Reghan J. Hill,et al.  INERTIAL EFFECTS IN SUSPENSION AND POROUS-MEDIA FLOWS , 2001 .

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

[41]  W. Carlson,et al.  Plagioclase-chain networks in slowly cooled basaltic magma , 1999 .

[42]  Philippe Gondret,et al.  Experiments on the motion of a solid sphere toward a wall: From viscous dissipation to elastohydrodynamic bouncing , 1999 .

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

[44]  D. Koch,et al.  Lubrication flows between spherical particles colliding in a compressible non-continuum gas , 1997, Journal of Fluid Mechanics.

[45]  Tayfun E. Tezduyar,et al.  Simulation of multiple spheres falling in a liquid-filled tube , 1996 .

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

[47]  Clayton T. Crowe,et al.  Numerical models for two-phase turbulent flows , 1996 .

[48]  C. Williamson Vortex Dynamics in the Cylinder Wake , 1996 .

[49]  R. Henderson Details of the drag curve near the onset of vortex shedding , 1995 .

[50]  A. Ladd Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 2. Numerical results , 1993, Journal of Fluid Mechanics.

[51]  A. Ladd Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 1. Theoretical foundation , 1993, Journal of Fluid Mechanics.

[52]  J. Hogan Monomineralic Glomerocrysts: Textural Evidence for Mineral Resorption during Crystallization of Igneous Rocks , 1993, The Journal of Geology.

[53]  C. Williamson The natural and forced formation of spot-like ‘vortex dislocations’ in the transition of a wake , 1992, Journal of Fluid Mechanics.

[54]  Howard H. Hu,et al.  Direct simulation of fluid particle motions , 1992 .

[55]  M. Rudman Two-phase natural convection: implications for crystal settling in magma chambers , 1992 .

[56]  H. Huppert,et al.  Sedimentation of particles from a convecting fluid , 1990, Nature.

[57]  D. Yuen,et al.  Evolution of crystal-settling in magma-chamber convection , 1988 .

[58]  W. Zijl GENERALIZED POTENTIAL FLOW THEORY AND DIRECT CALCULATION OF VELOCITIES APPLIED TO AND THE BOUSSINESQ EQUATIONS THE NUMERICAL SOLUTION OF THE NAVIER-STOKES , 1988 .

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

[60]  E. J. Hinch,et al.  The elastohydrodynamic collision of two spheres , 1986, Journal of Fluid Mechanics.

[61]  Robert H. Davis,et al.  Sedimentation of noncolloidal particles at low Reynolds numbers , 1985 .

[62]  J. Riley,et al.  Equation of motion for a small rigid sphere in a nonuniform flow , 1983 .

[63]  W. Russel Review of the Role of Colloidal Forces in the Rheology of Suspensions , 1980 .

[64]  A. Arzi Critical phenomena in the rheology of partially melted rocks , 1978 .

[65]  I. Orlanski A Simple Boundary Condition for Unbounded Hyperbolic Flows , 1976 .

[66]  Howard Brenner,et al.  Rheology of a dilute suspension of axisymmetric Brownian particles , 1974 .

[67]  G. Batchelor,et al.  Transport Properties of Two-Phase Materials with Random Structure , 1974 .

[68]  A. Chorin Numerical solution of the Navier-Stokes equations , 1968 .

[69]  G. Batchelor,et al.  An Introduction to Fluid Dynamics , 1968 .

[70]  R. Whitmore,et al.  Experimental determination of the wall effect for spheres falling axially in cylindrical vessels , 1961 .

[71]  Sadatoshi Taneda,et al.  Experimental Investigation of the Wakes behind Cylinders and Plates at Low Reynolds Numbers , 1956 .

[72]  A. Einstein Eine neue Bestimmung der Moleküldimensionen , 1905 .

[73]  G G J O S E P H,et al.  Particle – wall collisions in a viscous fluid , 2022 .