Hydrodynamics of suspensions of passive and active rigid particles: a rigid multiblob approach

Journal Article · Tue Jan 12 00:00:00 EST 2016 · Communications in Applied Mathematics and Computational Science

DOI:https://doi.org/10.2140/camcos.2016.11.217· OSTI ID:1393005

Usabiaga, Florencio Balboa ^[1]; Kallemov, Bakytzhan ^[2]; Delmotte, Blaise ^[1]; Bhalla, Amneet Pal Singh ^[3]; Griffith, Boyce E. ^[3]; Donev, Aleksandar ^[1]

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1. New York Univ., New York, NY (United States)
2. New York Univ., New York, NY (United States); Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
3. Univ. of North Carolina, Chapel Hill, NC (United States)

We develop a rigid multiblob method for numerically solving the mobility problem for suspensions of passive and active rigid particles of complex shape in Stokes flow in unconfined, partially confined, and fully confined geometries. As in a number of existing methods, we discretize rigid bodies using a collection of minimally resolved spherical blobs constrained to move as a rigid body, to arrive at a potentially large linear system of equations for the unknown Lagrange multipliers and rigid-body motions. Here we develop a block-diagonal preconditioner for this linear system and show that a standard Krylov solver converges in a modest number of iterations that is essentially independent of the number of particles. Key to the efficiency of the method is a technique for fast computation of the product of the blob-blob mobility matrix and a vector. For unbounded suspensions, we rely on existing analytical expressions for the Rotne-Prager-Yamakawa tensor combined with a fast multipole method (FMM) to obtain linear scaling in the number of particles. For suspensions sedimented against a single no-slip boundary, we use a direct summation on a graphical processing unit (GPU), which gives quadratic asymptotic scaling with the number of particles. For fully confined domains, such as periodic suspensions or suspensions confined in slit and square channels, we extend a recently developed rigid-body immersed boundary method by B. Kallemov, A. P. S. Bhalla, B. E. Griffith, and A. Donev (Commun. Appl. Math. Comput. Sci. 11 (2016), no. 1, 79-141) to suspensions of freely moving passive or active rigid particles at zero Reynolds number. We demonstrate that the iterative solver for the coupled fluid and rigid-body equations converges in a bounded number of iterations regardless of the system size. In our approach, each iteration only requires a few cycles of a geometric multigrid solver for the Poisson equation, and an application of the block-diagonal preconditioner, leading to linear scaling with the number of particles. We optimize a number of parameters in the iterative solvers and apply our method to a variety of benchmark problems to carefully assess the accuracy of the rigid multiblob approach as a function of the resolution. We also model the dynamics of colloidal particles studied in recent experiments, such as passive boomerangs in a slit channel, as well as a pair of non-Brownian active nanorods sedimented against a wall.

• Research Organization: Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
• Sponsoring Organization: National Science Foundation (NSF); USDOE
• Grant/Contract Number: AC02-05CH11231
• OSTI ID: 1393005
• Journal Information: Communications in Applied Mathematics and Computational Science, Vol. 11, Issue 2; ISSN 1559-3940
• Publisher: Mathematical Sciences Publishers
• Country of Publication: United States
• Language: English

Related Subjects

97 MATHEMATICS AND COMPUTING
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
Stokes flow
colloidal suspensions
Stokesian dynamics
immersed boundary method