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An all-topology two-fluid model for two-phase flows derived through Hamilton's Stationary Action Principle

Ward Haegeman, Giuseppe Orlando, Samuel Kokh, Marc Massot

TL;DR

The paper addresses the need for a robust, all-topology, compressible two-fluid model capable of handling shocks and topology changes without interface tracking. It develops a two-trajectory Stationary Action Principle framework that yields a fully closed system with new interfacial work and a mass-weighted interfacial velocity $u=Y_1u_1+Y_2u_2$, producing an interfacial pressure $p_I=Y_2p_1+Y_1p_2$ and a momentum-exchange term that preserves total momentum and energy. In 1D, the model is hyperbolic and symmetrizable under a non-resonance condition, admits a conservative entropy equation to select admissible shocks, and provides well-defined jump conditions for weak solutions; in 2D, lift forces arise via a new potential velocity $\mathbf{v}=\nabla\zeta$, with $\rho\mathrm{D}_t\zeta=p_1-p_2$, indicating rich interfacial dynamics that warrant further study. The work offers a physically consistent, mathematically well-posed foundation for future numerical simulations of complex two-phase flows, including potential reductions and Riemann-solver development.

Abstract

We present a novel multi-fluid model for compressible two-phase flows. The model is derived through a newly developed Stationary Action Principle framework. It is fully closed and introduces a new interfacial quantity, the interfacial work. The closures for the interfacial quantities are provided by the variational principle. They are physically sound and well-defined for all type of flow topologies. The model is shown to be hyperbolic, symmetrizable, and admits an entropy conservation law. Its non-conservative products yield uniquely defined jump conditions which are provided. As such, it allows for the proper treatment of weak solutions. In the multi-dimensional setting, the model presents lift forces which are discussed. The model constitutes a sound basis for future numerical simulations.

An all-topology two-fluid model for two-phase flows derived through Hamilton's Stationary Action Principle

TL;DR

The paper addresses the need for a robust, all-topology, compressible two-fluid model capable of handling shocks and topology changes without interface tracking. It develops a two-trajectory Stationary Action Principle framework that yields a fully closed system with new interfacial work and a mass-weighted interfacial velocity , producing an interfacial pressure and a momentum-exchange term that preserves total momentum and energy. In 1D, the model is hyperbolic and symmetrizable under a non-resonance condition, admits a conservative entropy equation to select admissible shocks, and provides well-defined jump conditions for weak solutions; in 2D, lift forces arise via a new potential velocity , with , indicating rich interfacial dynamics that warrant further study. The work offers a physically consistent, mathematically well-posed foundation for future numerical simulations of complex two-phase flows, including potential reductions and Riemann-solver development.

Abstract

We present a novel multi-fluid model for compressible two-phase flows. The model is derived through a newly developed Stationary Action Principle framework. It is fully closed and introduces a new interfacial quantity, the interfacial work. The closures for the interfacial quantities are provided by the variational principle. They are physically sound and well-defined for all type of flow topologies. The model is shown to be hyperbolic, symmetrizable, and admits an entropy conservation law. Its non-conservative products yield uniquely defined jump conditions which are provided. As such, it allows for the proper treatment of weak solutions. In the multi-dimensional setting, the model presents lift forces which are discussed. The model constitutes a sound basis for future numerical simulations.

Paper Structure

This paper contains 17 sections, 85 equations.

Theorems & Definitions (5)

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