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Variational Discretizations of Ideal Magnetohydrodynamics in Smooth Regime Using Finite Element Exterior Calculus


Core Concepts
The author proposes variational discretizations for ideal compressible magnetohydrodynamic equations using finite element exterior calculus, aiming to conserve mass, entropy, and energy while preserving the divergence-free nature of the magnetic field.
Abstract

The content introduces a novel approach to discretize ideal MHD equations using variational principles and finite element methods. By leveraging differential forms and Lie derivatives, the scheme conserves key properties like mass, entropy, and energy. The methodology ensures stability and accuracy in simulations by preserving essential invariants such as total mass and solenoidal characteristics of the magnetic field. The proposed time discretization maintains conservation laws and reversibility. Specific choices for discrete spaces, operators, and projections are detailed to enhance numerical results.

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Stats
Variational approximations developed for fluid models in the last decade. Semi-discrete approximations conserve total mass, entropy, and energy. Divergence-free nature of the magnetic field is preserved. Numerical simulations verify accuracy and invariant preservation. Differential forms represented through Cartan's formula for Lie derivatives. FEEC framework used for discretization of differential forms and vector fields. Conservation properties include mass, entropy, energy preservation. Fully reversible time discretization scheme proposed.
Quotes

Deeper Inquiries

How does this variational approach compare with traditional numerical methods

The variational approach presented in the context above offers several advantages compared to traditional numerical methods for solving fluid dynamics problems. Firstly, the variational discretization based on a discrete Euler-Poincaré principle provides a more geometrically structured framework for approximating solutions to ideal magnetohydrodynamics equations. This allows for better conservation properties and stability in the solutions obtained. Secondly, by representing vector fields as operators on differential forms using Finite Element Exterior Calculus (FEEC), the method can handle complex geometries and maintain important calculus identities such as curl grad = 0 and div curl = 0 at a discrete level. This is particularly useful when dealing with problems involving magnetic fields or other physical constraints. Overall, this variational approach offers a more elegant and mathematically rigorous way of discretizing fluid dynamics equations, leading to improved accuracy and stability in simulations compared to traditional finite volume or discontinuous Galerkin schemes.

What implications do these conservation properties have on long-term simulations

The conservation properties exhibited by this methodology have significant implications for long-term simulations of fluid dynamics systems. For example, the preservation of total mass, entropy, energy, and solenoidal character of the magnetic field ensures that important physical quantities are accurately maintained over time. This leads to more reliable results in simulations conducted over extended periods. Additionally, these conservation properties contribute to numerical stability by preventing artificial dissipation or accumulation of errors that could affect the accuracy of long-term predictions. The reversible nature of the scheme also allows for backward time integration without loss of information or fidelity in the simulation results. In essence, these conservation properties provide confidence in using this methodology for prolonged simulations where maintaining physical consistency and accuracy is crucial.

How can this methodology be extended to other complex fluid dynamics problems

This methodology can be extended to address other complex fluid dynamics problems by adapting its variational principles and discretization techniques accordingly. For instance: For compressible flows: By modifying the Lagrangian formulation and advection equations appropriately, this approach can be applied to simulate compressible fluids with varying densities. For turbulent flows: Incorporating turbulence models into the Lagrangian action functional can enable modeling turbulent effects within ideal MHD equations. For multiphase flows: Extending the variational discretization to account for multiple phases interacting through different forces would allow simulating complex multiphase flow phenomena accurately. By tailoring projection operators, hat maps, and discrete spaces specific to each problem's requirements while maintaining key conservation laws like mass preservation or energy balance intact during extension efforts will ensure robustness across various challenging scenarios in fluid dynamics analysis.
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