2015
DOI: 10.1063/1.4920981
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Hydrodynamics and Brownian motions of a spheroid near a rigid wall

Abstract: Articles you may be interested in PHYSICS 142, 194901 (2015) Hydrodynamics and Brownian motions of a spheroid near a rigid wall In this work, we study in detail the hydrodynamics and the Brownian motions of a spheroidal particle suspended in a Newtonian fluid near a flat rigid wall. We employ 3D Finite Element Method (FEM) simulations to compute how the mobility tensor of the spheroid varies with both the particle-wall separation distance and the particle orientation. We then study the Brownian motion of th… Show more

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Cited by 43 publications
(68 citation statements)
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References 43 publications
(61 reference statements)
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“…23 By that we have also verified earlier theoretical developments and recent numerical predictions. 22 Our results are in agreement with numerical calculations even in the case when L/H ∼ O(1), rendering them practical for large and moderate wall-particle distances. …”
Section: Discussionsupporting
confidence: 86%
See 1 more Smart Citation
“…23 By that we have also verified earlier theoretical developments and recent numerical predictions. 22 Our results are in agreement with numerical calculations even in the case when L/H ∼ O(1), rendering them practical for large and moderate wall-particle distances. …”
Section: Discussionsupporting
confidence: 86%
“…The structure of the near-wall tensors is identical to that given in Ref. 22. In the body-fixed frame of reference RW, the correction tensors in Eqs.…”
Section: Dynamics Of Axisymmetric Particlesmentioning
confidence: 71%
“…Here U p = v ∞ xx + U yŷ , and Ω p = Ω φφ + Ω θθ is the full 3D particle reorientation rate for the particle orientation n = (sin θ p cos φ p , sin θ p sin φ p , cos θ p ) with Ω φ =γ w {β(y)F (α) sin(φ B − φ p )/(8π sin θ p ) − (1 − J cos 2φ p )/2}, Ω θ =γ w {β(y)F (α) cos θ p cos(φ B − φ p )/(8π) + J sin 2θ p sin 2φ p /4} [28]. H is calculated from the translational diffusion tensor D(φ p , θ p ) = D1 + 1 2 ∆DM(φ p , θ p ) = 1 2 H · H T where M(φ p , θ p ) is a symmetric 3x3 matrix [40] andD = (D 1 + D 2 )/2, ∆D = D 1 − D 2 where D 1 = k B T a −1 η −1 K 1 (α) and D 2 = k B T a −1 η −1 K 2 (α) are the respective longitudinal and transverse diffusion coefficients of an ellipsoid of aspect ratio α with shape functions K 1 (α) > K 2 (α) [33,40,[45][46][47]. The rotational diffusion constant D r = k B T a −3 η −1 K r (α) with the shape function K r (α) [33,36,40].…”
mentioning
confidence: 99%
“…It is well-known that HI and the Brownian motion of colloidal particles are dramatically affected by the presence of walls [12,26]. In particular, several experiments have been carried out to understand the singleparticle diffusion near to a flat wall [27][28][29].…”
mentioning
confidence: 99%
“…As mentioned previously, the dynamics of nonspherical colloids is nowadays a challenging topic of paramount importance within the context of condensed matter physics. From theoretical point of view, recent advances have been achieved by solving the NavierStokes equations in the limit of low Reynolds number, Re ≪ 1, for anisotropic particles [26,30]. In particular, Zabarankin [30] calculated the drag force and the resisting torque experienced by a dicolloid-like particle at the bulk.…”
mentioning
confidence: 99%