Large-Time Behavior of Solutions to Darcy–Boussinesq Equations with Non-Vanishing Scalar Acceleration Coefficient

We study the large-time behavior of solutions to Darcy–Boussinesq equations with a non-vanishing scalar acceleration coefficient, which model buoyancy-driven flows in porous media with spatially varying gravity. First, we show that the system admits steady-state solutions of the form (u,ρ,p)=(0,ρs,ps), where ρs is characterised by the hydrostatic balance ∇ps=−ρs∇Ψ. Second, we prove that the steady-state solution satisfying ∇ρs=δ(x,y)∇Ψ is linearly stable provided that δ(x,y)<δ0<0, while the system exhibits Rayleigh–Taylor instability if Ψ=gy, ρs=δ0g and δ0>0. Finally, despite the inherent Rayleigh–Taylor instability that may trigger exponential growth in time, we prove that for any sufficiently regular initial data, the solutions of the system asymptotically converge towards the vicinity of a steady-state solution, where the velocity field is zero, and the new state is determined by hydrostatic balance. This work advances porous media modeling for geophysical and engineering applications, emphasizing the critical interplay of gravity, inertia, and boundary conditions.

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Publication Details

Journal
Mathematics
Published
2025-05-10
DOI
https://doi.org/10.3390/math13101570
Primary Topic
Navier-Stokes equation solutions
Type
article
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article

Large-Time Behavior of Solutions to Darcy–Boussinesq Equations with Non-Vanishing Scalar Acceleration Coefficient

Quan Wang, Zhibo Hou, Huichao Wang
Mathematics
Navier-Stokes equation solutions
article

Large-Time Behavior of Solutions to Darcy–Boussinesq Equations with Non-Vanishing Scalar Acceleration Coefficient

Quan Wang, Zhibo Hou, Huichao Wang
article en

Abstract

We study the large-time behavior of solutions to Darcy–Boussinesq equations with a non-vanishing scalar acceleration coefficient, which model buoyancy-driven flows in porous media with spatially varying gravity. First, we show that the system admits steady-state solutions of the form (u,ρ,p)=(0,ρs,ps), where ρs is characterised by the hydrostatic balance ∇ps=−ρs∇Ψ. Second, we prove that the steady-state solution satisfying ∇ρs=δ(x,y)∇Ψ is linearly stable provided that δ(x,y)<δ0<0, while the system exhibits Rayleigh–Taylor instability if Ψ=gy, ρs=δ0g and δ0>0. Finally, despite the inherent Rayleigh–Taylor instability that may trigger exponential growth in time, we prove that for any sufficiently regular initial data, the solutions of the system asymptotically converge towards the vicinity of a steady-state solution, where the velocity field is zero, and the new state is determined by hydrostatic balance. This work advances porous media modeling for geophysical and engineering applications, emphasizing the critical interplay of gravity, inertia, and boundary conditions.

MathematicsVol. 13(10)
Xihua University (CN), Sichuan University (CN), Xuchang University (CN)
Openalex Percentile: Top 85%
Navier-Stokes equation solutions
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