2013
DOI: 10.1007/978-3-319-01601-6_26
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Mimetic Spectral Element Advection

Abstract: We present a discretization of the linear advection of differential forms on bounded domains. The framework established in [4] is extended to incorporate the Lie derivative, L, by means of Cartan's homotopy formula. The method is based on a physics-compatible discretization with spectral accuracy . It will be shown that the derived scheme has spectral convergence with local mass conservation. Artificial dispersion depends on the order of time integration.

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Cited by 7 publications
(5 citation statements)
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“…Possible extensions to spectral methods were described by Robidoux, [109]. A different approach for constructing arbitrary order mimetic finite elements has been proposed by the authors [31,64,92,96], with applications to advection problems [95], Stokes' flow [81], MHD equilibrium [94], Navier-Stokes [93], and within a Least-Squares finite element formulation [16,62,63,91].…”
Section: Overview Of Mimetic Discretizationsmentioning
confidence: 99%
“…Possible extensions to spectral methods were described by Robidoux, [109]. A different approach for constructing arbitrary order mimetic finite elements has been proposed by the authors [31,64,92,96], with applications to advection problems [95], Stokes' flow [81], MHD equilibrium [94], Navier-Stokes [93], and within a Least-Squares finite element formulation [16,62,63,91].…”
Section: Overview Of Mimetic Discretizationsmentioning
confidence: 99%
“…Now that we understand how momentum density should be integrated over a volume, we can also define convection of momentum density. After pairing with an arbitrary vector field, w, we obtain a volume form and we apply the Lie derivative to this volume form, see [11]. The Lie derivative for a volume form, β (n) , is given by…”
Section: Convectionmentioning
confidence: 99%
“…1, and P m w is the matrix which maps discrete velocity (which is discretized as mass-fluxes) to discrete momentum (on the staggered-grid). The discrete representation of momentum-flux, pressure force i w p (n) and traction forces, µ (∇ w v) (which can be equivalently writ- • Convective-flux, see [11], F…”
Section: Discrete Representationmentioning
confidence: 99%
“…In this paper we will make use of the spectral element method described in [9,19], application of these ideas to Stokes' flow see [16][17][18]; Poisson equation for volume forms [22]; advection equation [21]; derivation of a momentum conservation scheme [24]. Extension to compatible isogeometric methods see [11,12].…”
Section: Darcy Flowmentioning
confidence: 99%