arXiv subjects

R. D. Mills-Williams

Publications and source records attributed to R. D. Mills-Williams.

3 recordsLinked to original sources

arXiv2022

The Mean Field Fokker-Planck Equation with Nonlinear No-flux Boundary Conditions

We consider the mean field Fokker-Planck equation subject to nonlinear no-flux boundary conditions, which necessarily arise when subjecting a system of Brownian particles interacting via a pair potential in a bounded domain. With the additional presence of an external potential $V_1$, we show, by analysing the linearised Fokker-Planck operator, that the spectral properties of the equilibrium densities can differ considerably when compared with previous studies, e.g., with periodic boundary conditions. Amongst other mean field models of complex many-body particle systems, we present numerical experiments encompassing in a wide range of physical applications, including: generalised exponential models (Gaussian, Morse); a Kuramoto model, for noisy coupled oscillators; and an Onsager model for liquid crystals. We showcase our results by using the numerical methods developed in the pseudospectral collocation scheme 2DChebClass.

math.NA↗

arXiv2021

Well-Posedness and Equilibrium Behaviour of Overdamped Dynamic Density Functional Theory

We establish the global well-posedness of overdamped dynamic density functional theory (DDFT): a nonlinear, nonlocal integro-partial differential equation used in statistical mechanical models of colloidal fluids, and other applications including nonlinear reaction-diffusion systems and opinion dynamics. With nonlinear no-flux boundary conditions, we determine the existence and uniqueness of the weak density and flux, subject to two-body hydrodynamic interactions (HI). We also show that the density is Lyapunov stable with respect to the usual (Helmholtz) free energy functional. Principally, this is done by rewriting the dynamics for the density in an implicit gradient flow form, resembling the classical Smoluchowski equation but with spatially inhomogeneous diffusion and advection tensors. We also rigorously show that the stationary density is independent of the HI tensors, and prove exponentially fast convergence to equilibrium.

math.AP↗

arXiv2020

The Singular Hydrodynamic Interactions Between Two Spheres In Stokes Flow

We study exact solutions for the slow viscous flow of an infinite liquid caused by two rigid spheres approaching each either along or parallel to their line of centres, valid at all separations. This goes beyond the applicable range of existing solutions for singular hydrodynamic interactions (HIs) which, for practical applications, are limited to the near-contact or far field region of the flow. For the normal component of the HI, by use of a bipolar coordinate system, we derive the stream function for the flow as $Re\to 0$ and a formula for the singular (squeeze) force between the spheres as an infinite series. We also obtain the asymptotic behaviour of the forces as the nondimensional separation between the spheres goes to zero and infinity, rigorously confirming and improving upon known results relevant to a widely accepted lubrication theory. Additionally, we recover the force on a sphere moving perpendicularly to a plane as a special case. For the tangential component, again by using a bipolar coordinate system, we obtain the corresponding infinite series expression of the (shear) singular force between the spheres. All results hold for retreating spheres, consistent with the reversibility of Stokes flow. We demonstrate substantial differences in numerical simulations of colloidal fluids when using the present theory compared with existing multipole methods. Furthermore, we show that the present theory preserves positive definiteness of the resistance matrix $\boldsymbol{R}$ in a number of situations in which positivity is destroyed for multipole/perturbative methods.

physics.flu-dyn↗