Searcharxiv⌕ Search

arXiv · 2610.26547

Global strong solutions to the aligned 2.5D non-resistive full MHD system with high temperature and a strong magnetic field

Abstract

We study the Cauchy problem for an aligned vertical-field reduction of the full compressible non-resistive MHD equations in two space variables. The shear and bulk viscosities are proportional to $θ^α$, and the heat conductivity is proportional to $θ^β$. For $2<α<β<α+2$, we prove global existence and uniqueness of strong solutions when the background temperature and the comparable magnetic background are sufficiently large, while the positive density background is fixed. The velocity and temperature perturbations belong initially to $H^2$, and the transported magnetic perturbation belongs to $H^1\cap D^{1,4}$; their absolute norms may be bounded by an arbitrary fixed constant. Alignment is essential and implies a small density perturbation relative to the magnetic background. Our proof combines relative energy estimates, uniform in the background temperature and magnetic field, with coupled estimates for the material derivatives of the velocity and temperature. These bounds control the source terms in the damped magnetic-gradient equation, allowing us to close the global a priori estimates without a separate large-time decay assumption. We construct the global strong solution by smooth approximation and Sobolev energy estimates for the approximating solutions, and prove uniqueness by an energy estimate for the difference of two solutions.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Yachun Li, Zixuan Qu, Zhaoyang Shang. 2026-10-19. Global strong solutions to the aligned 2.5D non-resistive full MHD system with high temperature and a strong magnetic field. https://arxiv.org/abs/2610.26547

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

On the dispersive estimates for the discrete Schrödinger equation on a honeycomb lattice

The discrete Schrödinger equation on a two-dimensional honeycomb lattice is a fundamental tight-binding approximation model that describes the propagation of waves on graphene. For free evolution, we first show that the degenerate frequencies of the dispersion relation are completely characterized by three symmetric periodic curves (Theorem 2.1), and that the three curves meet at Dirac points where conical singularities appear (see Figure 2.1). Based on this observation, we prove the $L^1\to L^\infty$ dispersion estimates for the linear flow depending on the frequency localization (Theorem 2.3). Collecting all, we obtain the dispersion estimate with $O(|t|^{-2/3})$ decay as well as Strichartz estimates. As an application, we prove small data scattering for a nonlinear model (Theorem 2.10). The proof of the key dispersion estimates is based on the associated oscillatory integral estimates with degenerate phases and conical singularities at Dirac points. Our proof is direct and uses only elementary methods.

math.AP↗

Well-posedness and Stability of Thermoelastic Suspension Bridges with Cattaneo Heat Conduction: The Role of Viscoelastic Memory

Thermoelastic suspension bridges operate under strong thermo-mechanical coupling, and the classical Fourier law fails to capture the finite speed of thermal propagation observed in low-conductivity materials such as concrete. This paper investigates a suspension bridge model in which the heat flux is governed by the Cattaneo law with relaxation time $τ$, and in which the bridge deck may or may not possess viscoelastic memory. Using operator semigroup theory, we establish well-posedness and derive sharp decay rates for both regimes. For the memoryless system ($δ=0$), we show that the semigroup is polynomially stable with rate $t^{-1/2}$ when the structural parameters satisfy $\frac{ρ_1}κ = \frac{ρ_2}{b}$, and that the rate deteriorates to $t^{-1/4}$ otherwise; moreover, exponential stability fails whenever $χ_0 \neq 0$, or $χ_0 = 0$ and $χ_1 = 0$, where $χ_0$ and $χ_1$ are parameter-dependent coefficients. In sharp contrast, when viscoelastic memory is present ($δ=1$), the semigroup becomes exponentially stable, regardless of the structural parameter ratio. This reveals a regularizing role of viscoelastic memory: it converts polynomial decay into exponential decay and removes the parameter-ratio obstruction. The results provide a theoretical basis for exploiting inherent viscoelasticity in long-span bridges and for optimizing deck parameters in memoryless structures.

math.AP↗