A closure relation for moments equations in kinetic theory was recently introduced in [38], based on the study of the geometry of the set of moments. This relation was constructed from a projection of a moment vector toward the boundary of the set of moments and corresponds to approximating the underlying kinetic distribution as a sum of a chosen equilibrium distribution plus a sum of purely anisotropic Dirac distributions.The present work generalizes this construction for kinetic equations involving unbounded velocities, i.e. to the Hamburger problem, and provides a deeper analysis of the resulting moment system. Especially, we provide representation results for moment vectors along the boundary of the moment set that implies the well-definition of the model. And the resulting moment model is shown to be weakly hyperbolic with peculiar properties of hyperbolicity and entropy of two subsystems, corresponding respectively to the equilibrium and to the purely anisotropic parts of the underlying kinetic distribution.
{"title":"A moment closure based on a projection on the boundary of the realizability domain: Extension and analysis","authors":"T. Pichard","doi":"10.3934/krm.2022014","DOIUrl":"https://doi.org/10.3934/krm.2022014","url":null,"abstract":"A closure relation for moments equations in kinetic theory was recently introduced in [38], based on the study of the geometry of the set of moments. This relation was constructed from a projection of a moment vector toward the boundary of the set of moments and corresponds to approximating the underlying kinetic distribution as a sum of a chosen equilibrium distribution plus a sum of purely anisotropic Dirac distributions.The present work generalizes this construction for kinetic equations involving unbounded velocities, i.e. to the Hamburger problem, and provides a deeper analysis of the resulting moment system. Especially, we provide representation results for moment vectors along the boundary of the moment set that implies the well-definition of the model. And the resulting moment model is shown to be weakly hyperbolic with peculiar properties of hyperbolicity and entropy of two subsystems, corresponding respectively to the equilibrium and to the purely anisotropic parts of the underlying kinetic distribution.","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"25 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2022-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79764078","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this paper, we investigate existence of global-in-time strong solutions to the Cauchy problem of the kinetic Cucker–Smale model coupled with the incompressible Navier–Stokes equations in the two dimensional space. By introducing a weighted Sobolev space and using the maximal regularity estimate on the linear non-stationary Stokes equations, we present a complete analysis on existence of global-in-time strong solutions to the coupled model, without any smallness assumptions on initial data.
{"title":"Global existence of strong solutions to the kinetic Cucker-Smale model coupled with the two dimensional incompressible Navier-Stokes equations","authors":"Chunyin Jin","doi":"10.3934/krm.2022023","DOIUrl":"https://doi.org/10.3934/krm.2022023","url":null,"abstract":"In this paper, we investigate existence of global-in-time strong solutions to the Cauchy problem of the kinetic Cucker–Smale model coupled with the incompressible Navier–Stokes equations in the two dimensional space. By introducing a weighted Sobolev space and using the maximal regularity estimate on the linear non-stationary Stokes equations, we present a complete analysis on existence of global-in-time strong solutions to the coupled model, without any smallness assumptions on initial data.","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"285 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2022-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75422347","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We study a variant of the Cucker-Smale model where information between agents propagates with a finite speed begin{document}$ {{mathfrak{c}}}>0 $end{document}. This leads to a system of functional differential equations with state-dependent delay. We prove that, if initially the agents travel slower than begin{document}$ {{mathfrak{c}}} $end{document}, then the discrete model admits unique global solutions. Moreover, under a generic assumption on the influence function, we show that there exists a critical information propagation speed begin{document}$ {{{{mathfrak{c}}}^ast}}>0 $end{document} such that if begin{document}$ {{mathfrak{c}}}geq{{{{mathfrak{c}}}^ast}} $end{document}, the system exhibits asymptotic flocking in the sense of the classical definition of Cucker and Smale. For constant initial datum the value of begin{document}$ {{{{mathfrak{c}}}^ast}} $end{document} is explicitly calculable. Finally, we derive a mean-field limit of the discrete system, which is formulated in terms of probability measures on the space of time-dependent trajectories. We show global well-posedness of the mean-field problem and argue that it does not admit a description in terms of the classical Fokker-Planck equation.
We study a variant of the Cucker-Smale model where information between agents propagates with a finite speed begin{document}$ {{mathfrak{c}}}>0 $end{document}. This leads to a system of functional differential equations with state-dependent delay. We prove that, if initially the agents travel slower than begin{document}$ {{mathfrak{c}}} $end{document}, then the discrete model admits unique global solutions. Moreover, under a generic assumption on the influence function, we show that there exists a critical information propagation speed begin{document}$ {{{{mathfrak{c}}}^ast}}>0 $end{document} such that if begin{document}$ {{mathfrak{c}}}geq{{{{mathfrak{c}}}^ast}} $end{document}, the system exhibits asymptotic flocking in the sense of the classical definition of Cucker and Smale. For constant initial datum the value of begin{document}$ {{{{mathfrak{c}}}^ast}} $end{document} is explicitly calculable. Finally, we derive a mean-field limit of the discrete system, which is formulated in terms of probability measures on the space of time-dependent trajectories. We show global well-posedness of the mean-field problem and argue that it does not admit a description in terms of the classical Fokker-Planck equation.
{"title":"Cucker-Smale model with finite speed of information propagation: Well-posedness, flocking and mean-field limit","authors":"J. Haskovec","doi":"10.3934/krm.2022033","DOIUrl":"https://doi.org/10.3934/krm.2022033","url":null,"abstract":"<p style='text-indent:20px;'>We study a variant of the Cucker-Smale model where information between agents propagates with a finite speed <inline-formula><tex-math id=\"M1\">begin{document}$ {{mathfrak{c}}}>0 $end{document}</tex-math></inline-formula>. This leads to a system of functional differential equations with state-dependent delay. We prove that, if initially the agents travel slower than <inline-formula><tex-math id=\"M2\">begin{document}$ {{mathfrak{c}}} $end{document}</tex-math></inline-formula>, then the discrete model admits unique global solutions. Moreover, under a generic assumption on the influence function, we show that there exists a critical information propagation speed <inline-formula><tex-math id=\"M3\">begin{document}$ {{{{mathfrak{c}}}^ast}}>0 $end{document}</tex-math></inline-formula> such that if <inline-formula><tex-math id=\"M4\">begin{document}$ {{mathfrak{c}}}geq{{{{mathfrak{c}}}^ast}} $end{document}</tex-math></inline-formula>, the system exhibits asymptotic flocking in the sense of the classical definition of Cucker and Smale. For constant initial datum the value of <inline-formula><tex-math id=\"M5\">begin{document}$ {{{{mathfrak{c}}}^ast}} $end{document}</tex-math></inline-formula> is explicitly calculable. Finally, we derive a mean-field limit of the discrete system, which is formulated in terms of probability measures on the space of time-dependent trajectories. We show global well-posedness of the mean-field problem and argue that it does not admit a description in terms of the classical Fokker-Planck equation.</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"116 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"77972240","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The free transport operator of probability density function begin{document}$ f(t, x, v) $end{document} is one the most fundamental operator which is widely used in many areas of PDE theory including kinetic theory, in particular. When it comes to general boundary problems in kinetic theory, however, it is well-known that high order regularity is very hard to obtain in general. In this paper, we study the free transport equation in a disk with the specular reflection boundary condition. We obtain initial-boundary compatibility conditions for begin{document}$ C^{1}_{t, x, v} $end{document} and begin{document}$ C^{2}_{t, x, v} $end{document} regularity of the solution. We also provide regularity estimates.
The free transport operator of probability density function begin{document}$ f(t, x, v) $end{document} is one the most fundamental operator which is widely used in many areas of PDE theory including kinetic theory, in particular. When it comes to general boundary problems in kinetic theory, however, it is well-known that high order regularity is very hard to obtain in general. In this paper, we study the free transport equation in a disk with the specular reflection boundary condition. We obtain initial-boundary compatibility conditions for begin{document}$ C^{1}_{t, x, v} $end{document} and begin{document}$ C^{2}_{t, x, v} $end{document} regularity of the solution. We also provide regularity estimates.
{"title":"On $ C^{2} $ solution of the free-transport equation in a disk","authors":"G. Ko, Donghyung Lee","doi":"10.3934/krm.2022031","DOIUrl":"https://doi.org/10.3934/krm.2022031","url":null,"abstract":"<p style='text-indent:20px;'>The free transport operator of probability density function <inline-formula><tex-math id=\"M2\">begin{document}$ f(t, x, v) $end{document}</tex-math></inline-formula> is one the most fundamental operator which is widely used in many areas of PDE theory including kinetic theory, in particular. When it comes to general boundary problems in kinetic theory, however, it is well-known that high order regularity is very hard to obtain in general. In this paper, we study the free transport equation in a disk with the specular reflection boundary condition. We obtain initial-boundary compatibility conditions for <inline-formula><tex-math id=\"M3\">begin{document}$ C^{1}_{t, x, v} $end{document}</tex-math></inline-formula> and <inline-formula><tex-math id=\"M4\">begin{document}$ C^{2}_{t, x, v} $end{document}</tex-math></inline-formula> regularity of the solution. We also provide regularity estimates.</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"74 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-12-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"77111579","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this note, we propose a slightly different proof of Gallavotti's theorem ["Statistical Mechanics: A Short Treatise", Springer, 1999, pp. 48-55] on the derivation of the linear Boltzmann equation for the Lorentz gas with a Poisson distribution of obstacles in the Boltzmann-Grad limit.
{"title":"The Boltzmann-Grad limit for the Lorentz gas with a Poisson distribution of obstacles","authors":"F. Golse","doi":"10.3934/krm.2022001","DOIUrl":"https://doi.org/10.3934/krm.2022001","url":null,"abstract":"<p style='text-indent:20px;'>In this note, we propose a slightly different proof of Gallavotti's theorem [\"Statistical Mechanics: A Short Treatise\", Springer, 1999, pp. 48-55] on the derivation of the linear Boltzmann equation for the Lorentz gas with a Poisson distribution of obstacles in the Boltzmann-Grad limit.</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"95 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-11-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79548176","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
C. Bardos, Trinh T. Nguyen, Toan T. Nguyen, E. Titi
We prove the inviscid limit for the incompressible Navier-Stokes equations for data that are analytic only near the boundary in a general two-dimensional bounded domain. Our proof is direct, using the vorticity formulation with a nonlocal boundary condition, the explicit semigroup of the linear Stokes problem near the flatten boundary, and the standard wellposedness theory of Navier-Stokes equations in Sobolev spaces away from the boundary.
{"title":"The inviscid limit for the 2D Navier-Stokes equations in bounded domains","authors":"C. Bardos, Trinh T. Nguyen, Toan T. Nguyen, E. Titi","doi":"10.3934/krm.2022004","DOIUrl":"https://doi.org/10.3934/krm.2022004","url":null,"abstract":"We prove the inviscid limit for the incompressible Navier-Stokes equations for data that are analytic only near the boundary in a general two-dimensional bounded domain. Our proof is direct, using the vorticity formulation with a nonlocal boundary condition, the explicit semigroup of the linear Stokes problem near the flatten boundary, and the standard wellposedness theory of Navier-Stokes equations in Sobolev spaces away from the boundary.","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"175 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-11-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76964311","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We establish existence of finite energy weak solutions to the kinetic Fokker-Planck equation and the linear Landau equation near Maxwellian, in the presence of specular reflection boundary condition for general domains. Moreover, by using a method of reflection and the begin{document}$ S_p $end{document} estimate of [7], we prove regularity in the kinetic Sobolev spaces begin{document}$ S_p $end{document} and anisotropic Hölder spaces for such weak solutions. Such begin{document}$ S_p $end{document} regularity leads to the uniqueness of weak solutions.
We establish existence of finite energy weak solutions to the kinetic Fokker-Planck equation and the linear Landau equation near Maxwellian, in the presence of specular reflection boundary condition for general domains. Moreover, by using a method of reflection and the begin{document}$ S_p $end{document} estimate of [7], we prove regularity in the kinetic Sobolev spaces begin{document}$ S_p $end{document} and anisotropic Hölder spaces for such weak solutions. Such begin{document}$ S_p $end{document} regularity leads to the uniqueness of weak solutions.
{"title":"Kinetic Fokker-Planck and Landau equations with specular reflection boundary condition","authors":"Hongjie Dong, Yan Guo, Timur Yastrzhembskiy","doi":"10.3934/krm.2022003","DOIUrl":"https://doi.org/10.3934/krm.2022003","url":null,"abstract":"<p style='text-indent:20px;'>We establish existence of finite energy weak solutions to the kinetic Fokker-Planck equation and the linear Landau equation near Maxwellian, in the presence of specular reflection boundary condition for general domains. Moreover, by using a method of reflection and the <inline-formula><tex-math id=\"M1\">begin{document}$ S_p $end{document}</tex-math></inline-formula> estimate of [<xref ref-type=\"bibr\" rid=\"b7\">7</xref>], we prove regularity in the kinetic Sobolev spaces <inline-formula><tex-math id=\"M2\">begin{document}$ S_p $end{document}</tex-math></inline-formula> and anisotropic Hölder spaces for such weak solutions. Such <inline-formula><tex-math id=\"M3\">begin{document}$ S_p $end{document}</tex-math></inline-formula> regularity leads to the uniqueness of weak solutions.</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"24 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-11-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82769968","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
By employing the Fourier transform to derive key a priori estimates for the temporal gradient of the chemical signal, we establish the existence of global solutions and hydrodynamic limit of a chemotactic kinetic model with internal states and temporal gradient in one dimension, which is a system of two transport equations coupled to a parabolic equation proposed in [4].
{"title":"A kinetic chemotaxis model with internal states and temporal sensing","authors":"Zhian Wang","doi":"10.3934/krm.2021043","DOIUrl":"https://doi.org/10.3934/krm.2021043","url":null,"abstract":"<p style='text-indent:20px;'>By employing the Fourier transform to derive key <i>a priori</i> estimates for the temporal gradient of the chemical signal, we establish the existence of global solutions and hydrodynamic limit of a chemotactic kinetic model with internal states and temporal gradient in one dimension, which is a system of two transport equations coupled to a parabolic equation proposed in [<xref ref-type=\"bibr\" rid=\"b4\">4</xref>].</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"23 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-11-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74833194","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Although the nuclear fusion process has received a great deal of attention in recent years, the amount of mathematical analysis that supports the stability of the system seems to be relatively insufficient. This paper deals with the mathematical analysis of the magnetic confinement of the plasma via kinetic equations. We prove the global wellposedness of the Vlasov-Maxwell system in a two-dimensional annulus when a huge (but finite-in-time) external magnetic potential is imposed near the boundary. We assume that the solution is axisymmetric. The authors hope that this work is a step towards a more generalized work on the three-dimensional Tokamak structure. The highlight of this work is the physical assumptions on the external magnetic potential well which remains finite within a finite time interval and from that, we prove that the plasma never touches the boundary. In addition, we provide a sufficient condition on the magnitude of the external magnetic potential to guarantee that the plasma is confined in an annulus of the desired thickness which is slightly larger than the initial support. Our method uses the cylindrical coordinate forms of the Vlasov-Maxwell system.
{"title":"Magnetic confinement for the 2D axisymmetric relativistic Vlasov-Maxwell system in an annulus","authors":"Jin Woo Jang, Robert M. Strain, T. Wong","doi":"10.3934/krm.2021039","DOIUrl":"https://doi.org/10.3934/krm.2021039","url":null,"abstract":"Although the nuclear fusion process has received a great deal of attention in recent years, the amount of mathematical analysis that supports the stability of the system seems to be relatively insufficient. This paper deals with the mathematical analysis of the magnetic confinement of the plasma via kinetic equations. We prove the global wellposedness of the Vlasov-Maxwell system in a two-dimensional annulus when a huge (but finite-in-time) external magnetic potential is imposed near the boundary. We assume that the solution is axisymmetric. The authors hope that this work is a step towards a more generalized work on the three-dimensional Tokamak structure. The highlight of this work is the physical assumptions on the external magnetic potential well which remains finite within a finite time interval and from that, we prove that the plasma never touches the boundary. In addition, we provide a sufficient condition on the magnitude of the external magnetic potential to guarantee that the plasma is confined in an annulus of the desired thickness which is slightly larger than the initial support. Our method uses the cylindrical coordinate forms of the Vlasov-Maxwell system.","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"14 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-11-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82411038","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Following closely the classical works [5]-[7] by Glassey, Strauss, and Schaeffer, we present a version of the Glassey-Strauss representation for the Vlasov-Maxwell systems in a 3D half space when the boundary is the perfect conductor.
{"title":"Glassey-Strauss representation of Vlasov-Maxwell systems in a Half Space","authors":"Yunbai Cao, Chanwoo Kim","doi":"10.3934/krm.2021034","DOIUrl":"https://doi.org/10.3934/krm.2021034","url":null,"abstract":"<p style='text-indent:20px;'>Following closely the classical works [<xref ref-type=\"bibr\" rid=\"b5\">5</xref>]-[<xref ref-type=\"bibr\" rid=\"b7\">7</xref>] by Glassey, Strauss, and Schaeffer, we present a version of the Glassey-Strauss representation for the Vlasov-Maxwell systems in a 3D half space when the boundary is the perfect conductor.</p>","PeriodicalId":49942,"journal":{"name":"Kinetic and Related Models","volume":"383 1","pages":""},"PeriodicalIF":1.0,"publicationDate":"2021-10-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76445350","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}