NANAJun 26, 2018

Constrained particle-mesh projections in a hybridized discontinuous Galerkin framework with applications to advection-dominated flows

arXiv:1806.099161 citationsh-index: 27
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This work addresses the need for accurate and conservative advection schemes in computational fluid dynamics, particularly for advection-dominated flows.

The paper presents a novel particle-mesh scheme combining PIC and HDG methods that achieves diffusion-free advection and local mass/momentum conservation with high-order spatial accuracy. Numerical results demonstrate optimal spatial accuracy and second-order time accuracy for advection-diffusion and Navier-Stokes equations.

By combining concepts from particle-in-cell (PIC) and hybridized discontinuous Galerkin (HDG) methods, we present a particle-mesh scheme which allows for diffusion-free advection, satisfies mass and momentum conservation principles in a local sense, and allows the extension to high-order spatial accuracy. To achieve this, we propose a novel particle-mesh projection operator required for the exchange of information between the particles and the mesh. Key is to cast these projections as a PDE-constrained $\ell^2$-optimization problem to allow the advective field naturally located on Lagrangian particles to be expressed as a mesh quantity. By expressing the control variable in terms of single-valued functions at cell interfaces, this optimization problem seamlessly fits in a HDG framework. Owing to this framework, the resulting scheme can be implemented efficiently via static condensation. The performance of the scheme is demonstrated by means of various numerical examples for the linear advection-diffusion equation and the incompressible Navier-Stokes equations. The results show that optimal spatial accuracy can be achieved, and given the particular time-stepping strategy, second-order time accuracy is confirmed. The robustness of the scheme is illustrated by considering benchmarks for advection of discontinuous fields and the Taylor-Green vortex instability in the high Reynolds number regime.

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