A method of immersed layers on Cartesian grids, with application to incompressible flows

TL;DR

This paper introduces a novel immersed layer method on Cartesian grids that distinguishes interface sides, enabling more precise simulation of incompressible flows with moving interfaces, improving upon traditional immersed boundary methods.

Contribution

The paper develops a discrete Heaviside function and extended PDE forms to separately specify conditions on each side of an interface, enhancing interface treatment in immersed boundary methods.

Findings

Successfully applied to 2D incompressible flows around rotating objects.

Allows individual side constraints, improving interface force representation.

Demonstrates improved accuracy in flow simulations with moving interfaces.

Abstract

The immersed boundary method (IBM) of Peskin (J. Comput. Phys., 1977), and derived forms such as the projection method of Taira and Colonius (J. Comput. Phys., 2007), have been useful for simulating flow physics in problems with moving interfaces on stationary grids. However, in their interface treatment, these methods do not distinguish one side from the other, but rather, apply the motion constraint to both sides, and the associated interface force is an inseparable mix of contributions from each side. In this work, we define a discrete Heaviside function, a natural companion to the familiar discrete Dirac delta function (DDF), to define a masked version of each field on the grid which, to within the error of the DDF, takes the intended value of the field on the respective sides of the interface. From this foundation we develop discrete operators and identities that are uniformly applicable to any surface geometry. We use these to develop extended forms of prototypical partial differential equations, including Poisson, convection-diffusion, and incompressible Navier-Stokes, that govern the discrete masked fields. These equations contain the familiar forcing term of the IBM, but also additional terms that regularize the jumps in field quantities onto the grid and enable us to individually specify the constraints on field behavior on each side of the interface. Drawing the connection between these terms and the layer potentials in elliptic problems, we refer to them generically as immersed layers. We demonstrate the application of the method to several representative problems, including two-dimensional incompressible flows inside a rotating cylinder and external to a rotating square.