4.6 Review

Smoothed profile method for direct numerical simulations of hydrodynamically interacting particles

Journal

SOFT MATTER
Volume 17, Issue 16, Pages 4226-4253

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d0sm02210a

Keywords

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Funding

  1. Japan Science and Technology Agency (JST) through PRESTO project
  2. JSPS KAKENHI [26247069, 17H01083, 18K03563, 20K03786, 20H05619, 20xcdccH00129, JP 23244087]
  3. Japan Science and Technology Agency (JST) through CREST project
  4. Grants-in-Aid for Scientific Research [17H01083, 18K03563, 26247069, 20H05619, 20K03786] Funding Source: KAKEN

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The presented method efficiently calculates the motions of hydrodynamically interacting particles in various host fluids by coupling continuum fluid mechanics with moving particles. By modeling the interface between solid particles and host fluid as a thin shell region, the method achieves high accuracy and versatility.
A general method is presented for computing the motions of hydrodynamically interacting particles in various kinds of host fluids for arbitrary Reynolds numbers. The method follows the standard procedure for performing direct numerical simulations (DNS) of particulate systems, where the Navier-Stokes equation must be solved consistently with the motion of the rigid particles, which defines the temporal boundary conditions to be satisfied by the Navier-Stokes equation. The smoothed profile (SP) method provides an efficient numerical scheme for coupling the continuum fluid mechanics with the dispersed moving particles, which are allowed to have arbitrary shapes. In this method, the sharp boundaries between solid particles and the host fluid are replaced with a smeared out thin shell (interfacial) region, which can be accurately resolved on a fixed Cartesian grid utilizing a SP function with a finite thickness. The accuracy of the SP method is illustrated by comparison with known exact results. In the present paper, the high degree of versatility of the SP method is demonstrated by considering several types of active and passive particle suspensions.

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