变度量各向异性网格生成算法和各向异性椭圆偏微分方程匹配网格

对于各向异性问题而言,在进行数值求解时,一个相匹配的各向异性网格至关重要.本文针对二阶椭圆偏微分方程,当其系数矩阵为各向异性时,给出了系数矩阵的逆作为相匹配的各向异性度量,在此度量下生成的各向异性网格即为匹配网格.本文还提出了新的变度量各向异性网格生成算法,该算法通过在各向异性背景网格上结合各向异性Delaunay准则和基于力平衡的结点优化函数生成高质量的各向异性三角化网格.通过数值算例可知,在匹配的各向异性三角化网格上,不仅有条件数小的代数离散系统,还有高精度的数值解,更甚者,在匹配网格结点上的l2范数误差有超收敛现象.     

各向异性泛函与各向异性方程解的局部有界性

证明了各向异性泛函的极小点与各向异性方程     

各向异性Laplace算子的一个非线性Picone恒等式及其应用（英文）

本文针对各向异性Laplace算子,建立了一个非线性Picone恒等式.作为它的应用,得到了各向异性椭圆方程的Sturmian比较原理、各向异性椭圆系统的Liouville定理和广义的各向异性Hardy型不等式.     

磁场感生各向异性效应

用转矩法发现,在低温下,大于临界值的磁场能使自旋玻璃CuMn和AgMn感生出磁各向异性。它是由一个较大的单向各向异性和一个较小的单轴各向异性组成。本文介绍了这种感生各向异性的一些主要表现,并指出它与上述合金在磁场中冷却所感生的各向异性之间的密切关系。     

各向异性函数空间上的多线性算子的估计及其应用

设A是Rn上的各向异性伸缩, L是由各向异性Calderón-Zygmund算子生成的一般的多线性算子.本文得到L从加权Lebesgue空间Lwp(Rn)到无权的各向异性Hardy空间HAp (Rn)的有界性.另外,对各向异性Hardy空间H1(Rn)和加权各向异性BMO空间BMOAw(Rn)得到包含关系:BMOAw(Rn)■(H1A(Rn))*.作为应用,对加权各向异性BMO函数b和各向异性Calderón-Zygmund算子T生成的交换子[T, b],得到‖[T, b](f)‖Lwp(Rn)C‖b‖BMOwA(Rn)‖f‖Lpw(Rn).以上所有结果在经典的各向齐性情形下也是新的.     

太阳风粘性与各向异性压强的形成机制和数学描写方法

本文探讨了磁场、流场、各向异性热流和各向异性外热源以及库仑碰撞和内波粒相互作用对压强各向异性演化的影响.并根据定常太阳风这样的磁化等离子体中不存在与粘性应力无关的各向异性静压强的分析结论,证明了可用平行和垂直磁场压强场以及流场,来计算太阳风的粘性效应,而太阳风粘性模式实际上是包含质子热各向异性的太阳风模式.这种模式适于描写各类太阳风的粘性效应,包括能用经典理论描写的冕旒低速流;对于冕洞高速流,在能量方程中应包含各向异性质子热传导和各向异性外热源(如Alfven涨落加热).     

纳米晶软磁合金的结构对技术磁性的影响——Ⅰ.结构各向异性

考虑到现有理论的局限性,建立了界面非晶相的随机局域各向异性模型,对界面非晶相在合金结构各向异性中的作用进行了研究,结果表明由交换作用和局域磁晶各向异性决定的结构各向异性与界面非晶相的磁性和结构参数有着复杂的关系,晶化后期软磁性能的恶化可由界面非晶相的磁性能减弱来解释.     

各向异性非内积型网格下旋转Q1元的收敛性

主要研究非协调旋转Q₁元在各向异性非内积型网格,即各向异性平行四边形网格下的收敛性．该元的插值误差在各向异性网格剖分时是发散的,但是我们证明了它对于二阶椭圆问题的各向异性收敛性．为了克服该元插值误差的这个缺陷,构造了一个适当的算子来证明它的逼近性质．利用一定的分析技巧,在各向异性平行四边形网格剖分下,得到了旋转Q₁元的最优逼近误差和相容误差．该结果可以引发人们继续分析一些不满足各向异性插值性质单元的收敛性．文章的最后用一些算例来验证了理论分析的正确性．     

各向异性Sobolev及Besov类的平均单边宽度

给出了各向异性Sobolev类及各向异性Besov类的平均单边宽度,获得了相应的弱渐近估计.     

各向异性静态电磁场的本征理论

在物理表象的规范空间下研究了静电磁场方程,推导出了一阶模态形式的各向异性介质静电磁场的基本求解方程,从而得到了如下的理论结论:各向同性介质电或磁场为标量场;各向异性介质电或磁场则为失量场,其大小和方向与介质的异性子空间有关.以电各向异性介质为例,具体讨论了各向异性电场的规律.     

Anisotropic mesh generation methods based on ACVT and natural metric for anisotropic elliptic equation

Anisotropic meshes are known to be well-suited for problems which exhibit anisotropic solution features.Defning an appropriate metric tensor and designing an efcient algorithm for anisotropic mesh generation are two important aspects of the anisotropic mesh methodology.In this paper,we are concerned with the natural metric tensor for use in anisotropic mesh generation for anisotropic elliptic problems.We provide an algorithm to generate anisotropic meshes under the given metric tensor.We show that the inverse of the anisotropic difusion matrix of the anisotropic elliptic problem is a natural metric tensor for the anisotropic mesh generation in three aspects:better discrete algebraic systems,more accurate fnite element solution and superconvergence on the mesh nodes.Various numerical examples demonstrating the efectiveness are presented.     

Toward anisotropic mesh construction and error estimation in the finite element method

Directional, anisotropic features like layers in the solution of partial differential equations can be resolved favorably by using anisotropic finite element meshes. An adaptive algorithm for such meshes includes the ingredients Error estimation and Information extraction/Mesh refinement. Related articles on a posteriori error estimation on anisotropic meshes revealed that reliable error estimation requires an anisotropic mesh that is aligned with the anisotropic solution. To obtain anisotropic meshes the so‐called Hessian strategy is used, which provides information such as the stretching direction and stretching ratio of the anisotropic elements. This article combines the analysis of anisotropic information extraction/mesh refinement and error estimation (for several estimators). It shows that the Hessian strategy leads to well‐aligned anisotropic meshes and, consequently, reliable error estimation. The underlying heuristic assumptions are given in a stringent yet general form. Numerical examples strengthen the exposition. Hence the analysis provides further insight into a particular aspect of anisotropic error estimation. © 2002 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 18: 625–648, 2002; DOI 10.1002/num.10023     

The mathematical modeling of the electric field in the media with anisotropic objects

We present a numerical scheme for modeling the electric field in the media with tensor conductivity. This scheme is based on vector finite element method in frequency domain. The numerical computations of the electric field in the anisotropic medium are done. The conductivity of the anisotropic medium is positive defined dense tensor in general case. We consider the electric field from anisotropic layer, inclined anisotropic layer and some anisotropic objects in isotropic half-space.     

Nonconforming rotated Q_1 element on non-tensor product anisotropic meshes

In this paper, we consider the nonconforming rotated Q1 element for the second order elliptic problem on the non-tensor product anisotropic meshes, i.e. the anisotropic affine quadrilateral meshes. Though the interpolation error is divergent on the anisotropic meshes, we overcome this difficulty by constructing another proper operator. Then we give the optimal approximation error and the consistency error estimates under the anisotropic affine quadrilateral meshes. The results of this paper provide some hints to derive the anisotropic error of some finite elements whose interpolations do not satisfy the anisotropic interpolation properties. Lastly, a numerical test is carried out, which coincides with our theoretical analysis.     

Nonconforming rotated Q 1 element on non-tensor product anisotropic meshes

In this paper, we consider the nonconforming rotated Q ₁ element for the second order elliptic problem on the non-tensor product anisotropic meshes, i.e. the anisotropic affine quadrilateral meshes. Though the interpolation error is divergent on the anisotropic meshes, we overcome this difficulty by constructing another proper operator. Then we give the optimal approximation error and the consistency error estimates under the anisotropic affine quadrilateral meshes. The results of this paper provide some hints to derive the anisotropic error of some finite elements whose interpolations do not satisfy the anisotropic interpolation properties. Lastly, a numerical test is carried out, which coincides with our theoretical analysis.     

A Survey on Some Anisotropic Hardy-Type Function Spaces

Let $A$ be a general expansive matrix on $\mathbb{R}^n$. The aims of this article are twofold. The first one is to give a survey on the recent developments of anisotropic Hardy-type function spaces on $\mathbb{R}^n$, including anisotropic Hardy–Lorentz spaces, anisotropic variable Hardy spaces and anisotropic variable Hardy–Lorentz spaces as well as anisotropic Musielak–Orlicz Hardy spaces. The second one is to correct some errors and seal some gaps existing in the known articles. Some unsolved problems are also presented.     

Nonconforming rotated Q 1 element on non-tensor product anisotropic meshes

In this paper, we consider the nonconforming rotated Q ₁ element for the second order elliptic problem on the non-tensor product anisotropic meshes, i.e. the anisotropic affine quadrilateral meshes. Though the interpolation error is divergent on the anisotropic meshes, we overcome this difficulty by constructing another proper operator. Then we give the optimal approximation error and the consistency error estimates under the anisotropic affine quadrilateral meshes. The results of this paper provide some hints to derive the anisotropic error of some finite elements whose interpolations do not satisfy the anisotropic interpolation properties. Lastly, a numerical test is carried out, which coincides with our theoretical analysis.     

The anisotropic p-capacity and the anisotropic Minkowski inequality

In this paper,we prove a sharp anisotropic L;Minkowski inequality involving the total L^panisotropic mean curvature and the anisotropic p-capacity for any bounded domains with smooth boundary in Rⁿ.As consequences,we obtain an anisotropic Willmore inequality,a sharp anisotropic Minkowski inequality for outward F-minimising sets and a sharp volumetric anisotropic Minkowski inequality.For the proof,we utilize a nonlinear potential theoretic approach which has been recently developed by Agostiniani et al.(2019).     

Analyses and simulation of anisotropic fractal surfaces

The spectral densities for an anisotropic fractal surfaces are investigated. Since there is no general definition for anisotropic fractal surface, the profiles of anisotropic fractal surfaces are assumed to be fractal in two main axes. Then, the possible forms of the surface spectral densities are proposed. By using the inverse Fast Fourier Transform, anisotropic fractal surfaces can be simulated from the spectral densities.