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Global Strong Well-posedness of the heat-conducting, compressible primitive Equations

Tarek Zöchling

Abstract

The full heat-conducting compressible primitive equations are considered, extending the compressible primitive-equation framework by coupling the temperature through the ideal gas law and the thermal energy balance in the presence of gravity. Global strong well-posedness is established for small perturbations of an equilibrium state, thereby providing a result beyond the isothermal regime. The proof relies on a structural representation of the density in terms of the temperature and on a new Lagrangian transformation.

Global Strong Well-posedness of the heat-conducting, compressible primitive Equations

Abstract

The full heat-conducting compressible primitive equations are considered, extending the compressible primitive-equation framework by coupling the temperature through the ideal gas law and the thermal energy balance in the presence of gravity. Global strong well-posedness is established for small perturbations of an equilibrium state, thereby providing a result beyond the isothermal regime. The proof relies on a structural representation of the density in terms of the temperature and on a new Lagrangian transformation.
Paper Structure (7 sections, 5 theorems, 133 equations)

This paper contains 7 sections, 5 theorems, 133 equations.

Key Result

Theorem 3.1

Let $\tau>0$ and $\overline{\varrho}^\ast,\Theta^\ast>0$. Assume that the initial data $(\overline{\varrho}_0,v_0,\Theta_0)$ satisfy assu:data0. Then there exists such that for every $\varepsilon\in(0,\varepsilon_0)$ the reformulated system eq:full prim reformulated subject to the boundary conditions eq: bc admits a unique strong solution $(\overline{\varrho},v,\Theta)$ with With $\hat{B}(\Theta

Theorems & Definitions (9)

  • Theorem 3.1: Global, strong well-posedness of \ref{['eq:full prim']}
  • Remark 1
  • Lemma 1
  • Lemma 2
  • proof
  • Lemma 3
  • proof
  • Corollary 1
  • proof : Proof of \ref{['thm main']}