Pub Date : 2024-09-16DOI: 10.1007/s00021-024-00899-8
Mario Fuest, Michael Winkler
The chemotaxis-Navier–Stokes system
$$begin{aligned} left{ begin{array}{rcl} n_t+ucdot nabla n & =& Delta big (n c^{-alpha } big ), c_t+ ucdot nabla c & =& Delta c -nc, u_t + (ucdot nabla ) u & =& Delta u+nabla P + nnabla Phi , qquad nabla cdot u=0, end{array} right. end{aligned}$$
modelling the behavior of aerobic bacteria in a fluid drop, is considered in a smoothly bounded domain (Omega subset mathbb R^2). For all (alpha > 0) and all sufficiently regular (Phi ), we construct global classical solutions and thereby extend recent results for the fluid-free analogue to the system coupled to a Navier–Stokes system. As a crucial new challenge, our analysis requires a priori estimates for u at a point in the proof when knowledge about n is essentially limited to the observation that the mass is conserved. To overcome this problem, we also prove new uniform-in-time (L^p) estimates for solutions to the inhomogeneous Navier–Stokes equations merely depending on the space-time (L^2) norm of the force term raised to an arbitrary small power.
趋化-纳维尔-斯托克斯系统 $$begin{aligned}n_t+ucdot nabla n & =& Delta big (n c^{-alpha } big ),c_t+ ucdot nabla c & =&;Delta c -nc, u_t + (ucdot nabla ) u & =& Delta u+nabla P + nnabla Phi , qquad nabla cdot u=0, end{array}.对end{aligned}$$模拟好氧细菌在液滴中的行为,在平滑有界域 (Omega subset mathbb R^2) 中进行考虑。对于所有的(alpha > 0)和所有足够规则的(Phi ),我们构建了全局经典解,从而将最近的无流体类似结果扩展到了与纳维-斯托克斯系统耦合的系统。作为一个关键的新挑战,我们的分析要求在证明中的某一点对 u 进行先验估计,而此时关于 n 的知识基本上仅限于观察到质量是守恒的。为了克服这个问题,我们还为非均质纳维-斯托克斯方程的解证明了新的时间均匀(L^p)估计值,而这些估计值仅仅取决于力项的时空(L^2)规范,并将其提升到一个任意小的幂。
{"title":"Uniform $$L^p$$ Estimates for Solutions to the Inhomogeneous 2D Navier–Stokes Equations and Application to a Chemotaxis–Fluid System with Local Sensing","authors":"Mario Fuest, Michael Winkler","doi":"10.1007/s00021-024-00899-8","DOIUrl":"https://doi.org/10.1007/s00021-024-00899-8","url":null,"abstract":"<p>The chemotaxis-Navier–Stokes system </p><span>$$begin{aligned} left{ begin{array}{rcl} n_t+ucdot nabla n & =& Delta big (n c^{-alpha } big ), c_t+ ucdot nabla c & =& Delta c -nc, u_t + (ucdot nabla ) u & =& Delta u+nabla P + nnabla Phi , qquad nabla cdot u=0, end{array} right. end{aligned}$$</span><p>modelling the behavior of aerobic bacteria in a fluid drop, is considered in a smoothly bounded domain <span>(Omega subset mathbb R^2)</span>. For all <span>(alpha > 0)</span> and all sufficiently regular <span>(Phi )</span>, we construct global classical solutions and thereby extend recent results for the fluid-free analogue to the system coupled to a Navier–Stokes system. As a crucial new challenge, our analysis requires a priori estimates for <i>u</i> at a point in the proof when knowledge about <i>n</i> is essentially limited to the observation that the mass is conserved. To overcome this problem, we also prove new uniform-in-time <span>(L^p)</span> estimates for solutions to the inhomogeneous Navier–Stokes equations merely depending on the space-time <span>(L^2)</span> norm of the force term raised to an arbitrary small power.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142264117","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s00021-024-00897-w
Wancheng Sheng, Yang Zhou
In this paper, a kind of classic generalized Riemann problem for 2-dimensional isothermal Euler equations for compressible gas dynamics is considered. The problem is the gas ((u_{0}, v_{0}, r_{0} mid x mid ^{beta })) in the rectangular region expands into the vacuum. We construct the solution of the following form
$$begin{aligned} u=u(xi , eta ), v=v(xi , eta ), rho =t^{beta } varrho (xi , eta ), xi =frac{x}{t}, eta =frac{y}{t}, end{aligned}$$
where (rho ) and (u, v) denote the density and the velocity fields respectively, and (u_{0}, v_{0}, r_{0}>0) and (beta in (-1,0) cup (0,+infty )) are constants. The continuity of the self-similar solution depends on the value of (beta ). Under certain conditions, we get a weak solution with shock wave, which is necessarily generated initially and move apart along a plane. Furthermore, by the method of characteristic analysis, we explain the mechanism of the shock wave.
本文考虑了可压缩气体动力学二维等温欧拉方程的一种经典广义黎曼问题。问题是气体 ((u_{0}, v_{0}, r_{0} mid x mid ^{beta }))在矩形区域膨胀到真空中。我们构建了如下形式的解 $$begin{aligned} u=u(xi , eta ),v=v(xi , eta ),rho =t^{beta }varrho (xi , eta ),xi =frac{x}{t},eta =frac{y}{t}, end{aligned}$$ 其中 (rho ) 和 (u, v) 分别表示密度场和速度场,(u_{0}, v_{0}, r_{0}>;0)和(beta in (-1,0) cup (0,+infty )) 是常数。自相似解的连续性取决于 (beta) 的值。在一定条件下,我们会得到一个带有冲击波的弱解,它必然在初始时产生并沿着一个平面移动开来。此外,通过特征分析的方法,我们解释了冲击波的机理。
{"title":"Self-Similar Solution of the Generalized Riemann Problem for Two-Dimensional Isothermal Euler Equations","authors":"Wancheng Sheng, Yang Zhou","doi":"10.1007/s00021-024-00897-w","DOIUrl":"https://doi.org/10.1007/s00021-024-00897-w","url":null,"abstract":"<p>In this paper, a kind of classic generalized Riemann problem for 2-dimensional isothermal Euler equations for compressible gas dynamics is considered. The problem is the gas <span>((u_{0}, v_{0}, r_{0} mid x mid ^{beta }))</span> in the rectangular region expands into the vacuum. We construct the solution of the following form </p><span>$$begin{aligned} u=u(xi , eta ), v=v(xi , eta ), rho =t^{beta } varrho (xi , eta ), xi =frac{x}{t}, eta =frac{y}{t}, end{aligned}$$</span><p>where <span>(rho )</span> and (<i>u</i>, <i>v</i>) denote the density and the velocity fields respectively, and <span>(u_{0}, v_{0}, r_{0}>0)</span> and <span>(beta in (-1,0) cup (0,+infty ))</span> are constants. The continuity of the self-similar solution depends on the value of <span>(beta )</span>. Under certain conditions, we get a weak solution with shock wave, which is necessarily generated initially and move apart along a plane. Furthermore, by the method of characteristic analysis, we explain the mechanism of the shock wave.\u0000</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142180271","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-02DOI: 10.1007/s00021-024-00895-y
Cherif Amrouche, Guillaume Leloup, Roger Lewandowski
We are considering a steady-state turbulent Reynolds-Averaged Navier–Stokes (RANS) one-equation model, that couples the equation for the velocity-pressure mean field with the equation for the turbulent kinetic energy. Eddy viscosities vanish at the boundary, characterized by terms like (d(x, Gamma )^eta ) and (d(x, Gamma )^beta ), where (0< eta , beta < 1). We determine critical values (eta _c) and (beta _c) for which the system has a weak solution. This solution is obtained as the limit of viscous regularizations for (0< eta < eta _c) and (0< beta < beta _c).
我们考虑的是稳态湍流雷诺平均纳维-斯托克斯(RANS)一元模型,它将速度-压力平均场方程与湍流动能方程耦合在一起。涡流粘度在边界处消失,其特征为 (d(x, Gamma )^eta ) 和 (d(x, Gamma )^beta ),其中 (0< eta , beta < 1).我们确定临界值(eta _c)和(beta _c),对于这两个值,系统有一个弱解。这个解是作为 (0< eta < eta _c) 和 (0< beta < beta _c) 的粘性正则化的极限而得到的。
{"title":"TKE Model Involving the Distance to the Wall—Part 1: The Relaxed Case","authors":"Cherif Amrouche, Guillaume Leloup, Roger Lewandowski","doi":"10.1007/s00021-024-00895-y","DOIUrl":"https://doi.org/10.1007/s00021-024-00895-y","url":null,"abstract":"<p>We are considering a steady-state turbulent Reynolds-Averaged Navier–Stokes (RANS) one-equation model, that couples the equation for the velocity-pressure mean field with the equation for the turbulent kinetic energy. Eddy viscosities vanish at the boundary, characterized by terms like <span>(d(x, Gamma )^eta )</span> and <span>(d(x, Gamma )^beta )</span>, where <span>(0< eta , beta < 1)</span>. We determine critical values <span>(eta _c)</span> and <span>(beta _c)</span> for which the system has a weak solution. This solution is obtained as the limit of viscous regularizations for <span>(0< eta < eta _c)</span> and <span>(0< beta < beta _c)</span>.\u0000</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142180270","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-29DOI: 10.1007/s00021-024-00892-1
Wen Feng, Weinan Wang, Jiahong Wu
Several fundamental problems on the 2D magnetohydrodynamic (MHD) equations with only magnetic diffusion (no velocity dissipation) remain open, especialy in the case when the spatial domain is the whole space ({mathbb {R}}^2). This paper establishes that, near a background magnetic field, any fractional dissipation in one direction in the velocity equation would allow us to establish the global existence and stability for perturbations near the background. The magnetic diffusion here is not required to be given by the standard Laplacian operator but any general fractional Laplacian with positive power.
{"title":"Stability for a System of the 2D Incompressible MHD Equations with Fractional Dissipation","authors":"Wen Feng, Weinan Wang, Jiahong Wu","doi":"10.1007/s00021-024-00892-1","DOIUrl":"https://doi.org/10.1007/s00021-024-00892-1","url":null,"abstract":"<p>Several fundamental problems on the 2D magnetohydrodynamic (MHD) equations with only magnetic diffusion (no velocity dissipation) remain open, especialy in the case when the spatial domain is the whole space <span>({mathbb {R}}^2)</span>. This paper establishes that, near a background magnetic field, any fractional dissipation in one direction in the velocity equation would allow us to establish the global existence and stability for perturbations near the background. The magnetic diffusion here is not required to be given by the standard Laplacian operator but any general fractional Laplacian with positive power.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142180311","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-22DOI: 10.1007/s00021-024-00894-z
Luigi De Rosa, Theodore D. Drivas, Marco Inversi
By means of a unifying measure-theoretic approach, we establish lower bounds on the Hausdorff dimension of the space-time set which can support anomalous dissipation for weak solutions of fluid equations, both in the presence or absence of a physical boundary. Boundary dissipation, which can occur at both the time and the spatial boundary, is analyzed by suitably modifying the Duchon & Robert interior distributional approach. One implication of our results is that any bounded Euler solution (compressible or incompressible) arising as a zero viscosity limit of Navier–Stokes solutions cannot have anomalous dissipation supported on a set of dimension smaller than that of the space. This result is sharp, as demonstrated by entropy-producing shock solutions of compressible Euler (Drivas and Eyink in Commun Math Phys 359(2):733–763, 2018. https://doi.org/10.1007/s00220-017-3078-4; Majda in Am Math Soc 43(281):93, 1983. https://doi.org/10.1090/memo/0281) and by recent constructions of dissipative incompressible Euler solutions (Brue and De Lellis in Commun Math Phys 400(3):1507–1533, 2023. https://doi.org/10.1007/s00220-022-04626-0 624; Brue et al. in Commun Pure App Anal, 2023), as well as passive scalars (Colombo et al. in Ann PDE 9(2):21–48, 2023. https://doi.org/10.1007/s40818-023-00162-9; Drivas et al. in Arch Ration Mech Anal 243(3):1151–1180, 2022. https://doi.org/10.1007/s00205-021-01736-2). For (L^q_tL^r_x) suitable Leray–Hopf solutions of the (d-)dimensional Navier–Stokes equation we prove a bound of the dissipation in terms of the Parabolic Hausdorff measure (mathcal {P}^{s}), which gives (s=d-2) as soon as the solution lies in the Prodi–Serrin class. In the three-dimensional case, this matches with the Caffarelli–Kohn–Nirenberg partial regularity.
通过统一的度量理论方法,我们建立了时空集合豪斯多夫维度的下限,该维度可以支持流体方程弱解的反常耗散,无论是否存在物理边界。边界耗散既可能发生在时间边界,也可能发生在空间边界,我们通过适当修改 Duchon & Robert 内部分布方法对边界耗散进行了分析。我们结果的一个含义是,作为纳维-斯托克斯解的零粘度极限而产生的任何有界欧拉解(可压缩或不可压缩),都不可能在维度小于空间维度的集合上支持异常耗散。这一结果是尖锐的,可压缩欧拉的产生熵的冲击解(Drivas 和 Eyink 在 Commun Math Phys 359(2):733-763, 2018. https://doi.org/10.1007/s00220-017-3078-4; Majda 在 Am Math Soc 43(281):93, 1983. https://doi.org/10.1090/memo/0281)以及最近的耗散不可压缩欧拉解的构造(Brue 和 De Lellis 在 Commun Math Phys 400(3):1507-1533, 2023.https://doi.org/10.1007/s00220-022-04626-0 624;Brue 等人在 Commun Pure App Anal,2023),以及被动标量(Colombo 等人在 Ann PDE 9(2):21-48,2023。https://doi.org/10.1007/s40818-023-00162-9;Drivas 等人在 Arch Ration Mech Anal 243(3):1151-1180,2022。https://doi.org/10.1007/s00205-021-01736-2)。对于(L^q_tL^r_x)维纳维-斯托克斯方程的合适勒雷-霍普夫解,我们用抛物线豪斯多夫量(mathcal {P}^{s})证明了耗散的约束,只要解位于普罗迪-塞林类,就可以得到(s=d-2)。在三维情况下,这与 Caffarelli-Kohn-Nirenberg 部分正则性相吻合。
{"title":"On the Support of Anomalous Dissipation Measures","authors":"Luigi De Rosa, Theodore D. Drivas, Marco Inversi","doi":"10.1007/s00021-024-00894-z","DOIUrl":"https://doi.org/10.1007/s00021-024-00894-z","url":null,"abstract":"<p>By means of a unifying measure-theoretic approach, we establish lower bounds on the Hausdorff dimension of the space-time set which can support anomalous dissipation for weak solutions of fluid equations, both in the presence or absence of a physical boundary. Boundary dissipation, which can occur at both the time and the spatial boundary, is analyzed by suitably modifying the Duchon & Robert interior distributional approach. One implication of our results is that any bounded Euler solution (compressible or incompressible) arising as a zero viscosity limit of Navier–Stokes solutions cannot have anomalous dissipation supported on a set of dimension smaller than that of the space. This result is sharp, as demonstrated by entropy-producing shock solutions of compressible Euler (Drivas and Eyink in Commun Math Phys 359(2):733–763, 2018. https://doi.org/10.1007/s00220-017-3078-4; Majda in Am Math Soc 43(281):93, 1983. https://doi.org/10.1090/memo/0281) and by recent constructions of dissipative incompressible Euler solutions (Brue and De Lellis in Commun Math Phys 400(3):1507–1533, 2023. https://doi.org/10.1007/s00220-022-04626-0 624; Brue et al. in Commun Pure App Anal, 2023), as well as passive scalars (Colombo et al. in Ann PDE 9(2):21–48, 2023. https://doi.org/10.1007/s40818-023-00162-9; Drivas et al. in Arch Ration Mech Anal 243(3):1151–1180, 2022. https://doi.org/10.1007/s00205-021-01736-2). For <span>(L^q_tL^r_x)</span> suitable Leray–Hopf solutions of the <span>(d-)</span>dimensional Navier–Stokes equation we prove a bound of the dissipation in terms of the Parabolic Hausdorff measure <span>(mathcal {P}^{s})</span>, which gives <span>(s=d-2)</span> as soon as the solution lies in the Prodi–Serrin class. In the three-dimensional case, this matches with the Caffarelli–Kohn–Nirenberg partial regularity.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142180272","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-21DOI: 10.1007/s00021-024-00890-3
Adam Larios, Vincent R. Martinez
In this article, some elementary observations are is made regarding the behavior of solutions to the two-dimensional curl-free Burgers equation which suggests the distinguished role played by the scalar divergence field in determining the dynamics of the solution. These observations inspire a new divergence-based regularity condition for the two-dimensional Kuramoto–Sivashinsky equation (KSE) that provides conceptual clarity to the nature of the potential blow-up mechanism for this system. The relation of this regularity criterion to the Ladyzhenskaya–Prodi–Serrin-type criterion for the KSE is also established, thus providing the basis for the development of an alternative framework of regularity criterion for this equation based solely on the low-mode behavior of its solutions. The article concludes by applying these ideas to identify a conceptually simple modification of KSE that yields globally regular solutions, as well as providing a straightforward verification of this regularity criterion to establish global regularity of solutions to the 2D Burgers–Sivashinsky equation. The proofs are direct, elementary, and concise.
{"title":"Remarks on the Stabilization of Large-Scale Growth in the 2D Kuramoto–Sivashinsky Equation","authors":"Adam Larios, Vincent R. Martinez","doi":"10.1007/s00021-024-00890-3","DOIUrl":"https://doi.org/10.1007/s00021-024-00890-3","url":null,"abstract":"<p>In this article, some elementary observations are is made regarding the behavior of solutions to the two-dimensional curl-free Burgers equation which suggests the distinguished role played by the scalar divergence field in determining the dynamics of the solution. These observations inspire a new divergence-based regularity condition for the two-dimensional Kuramoto–Sivashinsky equation (KSE) that provides conceptual clarity to the nature of the potential blow-up mechanism for this system. The relation of this regularity criterion to the Ladyzhenskaya–Prodi–Serrin-type criterion for the KSE is also established, thus providing the basis for the development of an alternative framework of regularity criterion for this equation based solely on the low-mode behavior of its solutions. The article concludes by applying these ideas to identify a conceptually simple modification of KSE that yields globally regular solutions, as well as providing a straightforward verification of this regularity criterion to establish global regularity of solutions to the 2D Burgers–Sivashinsky equation. The proofs are direct, elementary, and concise.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142180273","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The present paper studies an asymptotic behavior of a spherically symmetric solution on the exterior domain of an unit ball for the compressible Navier–Stokes equation, describing a motion of viscous barotropic gas. Especially we study outflow problem, that is, the fluid blows out through boundary. Precisely we show an asymptotic stability of a spherically symmetric stationary solutions provided that an initial disturbance of the stationary solution is sufficiently small in the Sobolev space.
{"title":"Asymptotic Behavior of Spherically Symmetric Solutions to the Compressible Navier–Stokes Equation Towards Stationary Waves","authors":"Itsuko Hashimoto, Shinya Nishibata, Souhei Sugizaki","doi":"10.1007/s00021-024-00885-0","DOIUrl":"https://doi.org/10.1007/s00021-024-00885-0","url":null,"abstract":"<p>The present paper studies an asymptotic behavior of a spherically symmetric solution on the exterior domain of an unit ball for the compressible Navier–Stokes equation, describing a motion of viscous barotropic gas. Especially we study outflow problem, that is, the fluid blows out through boundary. Precisely we show an asymptotic stability of a spherically symmetric stationary solutions provided that an initial disturbance of the stationary solution is sufficiently small in the Sobolev space.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141942838","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-27DOI: 10.1007/s00021-024-00888-x
Zoran Grujić, Liaosha Xu
The problem of global-in-time regularity for the 3D Navier-Stokes equations, i.e., the question of whether a smooth flow can exhibit spontaneous formation of singularities, is a fundamental open problem in mathematical physics. Due to the super-criticality of the equations, the problem has been super-critical in the sense that there has been a ‘scaling gap’ between any regularity criterion and the corresponding a priori bound (regardless of the functional setup utilized). The purpose of this work is to present a mathematical framework-based on a suitably defined ‘scale of sparseness’ of the super-level sets of the positive and negative parts of the components of the higher-order spatial derivatives of the velocity field—in which the scaling gap between the regularity class and the corresponding a priori bound vanishes as the order of the derivative goes to infinity.
{"title":"Asymptotic Criticality of the Navier–Stokes Regularity Problem","authors":"Zoran Grujić, Liaosha Xu","doi":"10.1007/s00021-024-00888-x","DOIUrl":"https://doi.org/10.1007/s00021-024-00888-x","url":null,"abstract":"<p>The problem of global-in-time regularity for the 3D Navier-Stokes equations, i.e., the question of whether a smooth flow can exhibit spontaneous formation of singularities, is a fundamental open problem in mathematical physics. Due to the super-criticality of the equations, the problem has been super-critical in the sense that there has been a ‘scaling gap’ between any regularity criterion and the corresponding a priori bound (regardless of the functional setup utilized). The purpose of this work is to present a mathematical framework-based on a suitably defined ‘scale of sparseness’ of the super-level sets of the positive and negative parts of the components of the higher-order spatial derivatives of the velocity field—in which the scaling gap between the regularity class and the corresponding a priori bound vanishes as the order of the derivative goes to infinity.\u0000</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141782422","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-20DOI: 10.1007/s00021-024-00889-w
Lv Cai, Ning-An Lai
In this paper we study the compressible magnetohydrodynamics equations in three dimensions, which offer a good model for plasmas. Formation of singularity for (C^1)-solution in finite time is proved with axisymmetric initial data. The key observation is that the magnetic force term admits a good structure with axisymmetric assumption.
{"title":"Formation of Finite Time Singularity for Axially Symmetric Magnetohydrodynamic Waves in 3-D","authors":"Lv Cai, Ning-An Lai","doi":"10.1007/s00021-024-00889-w","DOIUrl":"https://doi.org/10.1007/s00021-024-00889-w","url":null,"abstract":"<p>In this paper we study the compressible magnetohydrodynamics equations in three dimensions, which offer a good model for plasmas. Formation of singularity for <span>(C^1)</span>-solution in finite time is proved with axisymmetric initial data. The key observation is that the magnetic force term admits a good structure with axisymmetric assumption.</p>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.3,"publicationDate":"2024-07-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141739008","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-15DOI: 10.1007/s00021-024-00887-y
Yongfu Wang
{"title":"Blowup Criterion for Viscous Non-baratropic Flows with Zero Heat Conduction Involving Velocity Divergence","authors":"Yongfu Wang","doi":"10.1007/s00021-024-00887-y","DOIUrl":"https://doi.org/10.1007/s00021-024-00887-y","url":null,"abstract":"","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":null,"pages":null},"PeriodicalIF":1.2,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141646262","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}