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Strongly overdamped dissipative particle dynamics for fluid-solid systems

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Figure

Figure 1: A DPD system and its initial configuration: fluid modelled by blue particles andsolid walls modelled by magenta particles.
Figure 2: Couette flow: Scheme 2 converges much faster than Scheme 1. Given a toleranceof 10−7, the Picard algorithm typically requires about 2100 and 450 iterations for Scheme 1and Scheme 2, respectively.
Figure 3: Couette flow, Lx × Ly = 10 × 10, ∆t = 0.01: variations of number density andvelocities on the flow cross section by Scheme 2.
Figure 4: Couette flow, ∆t(2two cases: = 0.01, 2000 time steps: Developments of velocity profile in m = 1 (top) and m = 0 (bottom), where results are displayed at time levels, 4, · · · , 20)
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