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Accurate projection methods for the incompressible Navier—Stokes equations

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In this article, the authors consider the accuracy of projection method approximations to the initial-boundary-value problem for the incompressible Navier-Stokes equations and present an improved projection algorithm which is fully second-order accurate.
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This article is published in Journal of Computational Physics.The article was published on 2001-04-10 and is currently open access. It has received 841 citations till now. The article focuses on the topics: Projection method & Pressure-correction method.

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Citations
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The Gauge-Uzawa Finite Element Method. Part I: The Navier-Stokes Equations

TL;DR: This first part introduces the gauge--Uzawa FEM method for the Navier--Stokes equations of incompressible fluids and shows unconditional stability and error estimates for both velocity and pressure via a variational approach under realistic regularity assumptions.
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Interaction of two tandem deformable bodies in a viscous incompressible flow

TL;DR: In this paper, a series of numerical simulations are designed and performed on the interaction of a pair of tandem flexible flags separated by a dimensionless vertical distance (0 ≤ D ≤ 5.5) in a flowing viscous incompressible fluid at lower Reynolds numbers (40 ≤ Re ≤ 220).
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Stability and convergence of efficient Navier‐Stokes solvers via a commutator estimate

TL;DR: For strong solutions of the Navier-Stokes equations in bounded domains with velocity specified at the boundary, the authors established the unconditional stability and convergence of discretization schemes that decouple the updates of pressure and velocity through explicit time stepping for pressure.
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A stable projection method for the incompressible Navier-Stokes equations on arbitrary geometries and adaptive Quad/Octrees

TL;DR: A novel stable implementation of the projection step is introduced, making use of the Marker And Cell layout for the data and the solver is validated numerically in two and three spatial dimensions.
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Reynolds number effects on lipid vesicles

TL;DR: The influence of inertia on the dynamics of a vesicle in a shearing flow is investigated using a novel level-set computational method in two dimensions and the maximum tension as a function of the Reynolds number is determined.
References
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Journal ArticleDOI

Numerical solution of the Navier-Stokes equations

TL;DR: In this paper, a finite-difference method for solving the time-dependent Navier-Stokes equations for an incompressible fluid is introduced, which is equally applicable to problems in two and three space dimensions.
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Application of a Fractional-Step Method to Incompressible Navier-Stokes Equations

TL;DR: In this paper, a numerical method for computing three-dimensional, time-dependent incompressible flows is presented based on a fractional-step, or time-splitting, scheme in conjunction with the approximate-factorization technique.
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High-order splitting methods for the incompressible Navier-Stokes equations

TL;DR: Improved pressure boundary conditions of high order in time are introduced that minimize the effect of erroneous numerical boundary layers induced by splitting methods, and a new family of stiffly stable schemes is employed in mixed explicit/implicit time-intgration rules.
Journal ArticleDOI

A second-order projection method for the incompressible navier-stokes equations

TL;DR: In this paper, a second-order projection method for the Navier-Stokes equations is proposed, which uses a specialized higher-order Godunov method for differencing the nonlinear convective terms.
Journal ArticleDOI

A second-order accurate pressure correction scheme for viscous incompressible flow

TL;DR: In this article, a pressure correction method for viscous incompressible flow is presented that is second order accurate in time and space, and a practical application is given for a numerical example.
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Frequently Asked Questions (11)
Q1. What have the authors contributed in "Accurate projection methods for the incompressible navier–stokes equations" ?

In this paper, the authors consider the second-order convergence of a projection method for the Navier-Stokes equations. 

The fact that the pressure itself is converging at the optimal rate indicates that the drop in convergence rates for the gradient is caused by spatial rather than temporal error. 

Since the test problems studied in the next section are all set in a periodic channel, the inversion of the Laplacian in the projection is made efficient by first taking the discrete Fourier transform of the equation in the x-direction. 

The errors are estimated at time 0.25 in the u-component of the velocity and the pressure when the maximum value of u is about 0.86, while the maximum of v has dropped to about 0.39. 

The class of incremental pressure projection methods discussed in this paper is characterized by the choice of three ingredients: the approximation to the pressure gradient term in the momentum equation, the formula used for the global pressure update during the time step, and the boundary conditions. 

a fractional step procedure can be used to approximate the solution of the coupled system by first solving an analog to Eq. (5) (without regard to the divergence constraint) for an intermediate quantity u∗, and then projecting this quantity onto the space of divergence-free fields to yield un+1. 

Methods are often categorized as “pressure-Poisson” or “projection” methods based on which form of the elliptic constraint equation is being used. 

The second-order method proposed by Perot uses q = 0 and replaces the pressure-update formula (12) with(I + ν1t 2 ∇2 ) pn+1/2 = φn+1. (25)This method still only obtains first-order convergence in the pressure since n̂ · ∇ p = 0 is the boundary condition used for the elliptic pressure equation. 

The continuity of ∇φ in time is implied by the fact that u∗ satisfies an elliptic equation with continuous forcing and 1t∇φ is simply (I− P)u∗. 

projection method II has substantially less error in the divergence of un than the other methods, and this error appears to be converging to zero at a higher rate than the other methods. 

In the next section it is shown that this extrapolation is necessary for the resulting velocity and pressure to be second-order accurate in the maximum norm.