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).     

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.     

含椭圆夹杂二维各向异性电磁弹性介质的耦合问题

研究了无限大二维各向异性电磁弹性固体的椭圆夹杂问题.基于广义Stroh方法、保角变换和扰动概念,得到了基体和夹杂内电场、磁场和弹性场的封闭解.本文结果可用于研究电磁弹性复合材料的有效性能.     

Winkler地基上四边自由正交各向异性矩形中厚板弯曲的有限积分变换解（英文）

本文应用有限积分变换法研究Winkler地基上四边自由正交各向异性矩形中厚板的弯曲问题.具体由正交各向异性矩形中厚板弯曲的基本方程组和边界条件出发,结合有限积分变换法及其对应的逆变换法推导出正交各向异性矩形中厚板弯曲问题的解析解.该解析解统一适用于计算各向同性/正交各向异性矩形薄板、中厚板和厚板的弯曲问题,并且通过具体算例验证了所得解析解的正确性.     

具有外磁场的Landau-Lifshitz方程

本文研究具有外磁场的Landau-Lifshitz方程的全局动力学,具体包括局部适定性、全局适定性、周期解的存在性.首先,利用移动标架法将LandauLifshitz方程转化为半线性Schr?dinger方程,从而利用色散方程的技巧得到任意维的局部适定性和一维的全局适定性.其次,通过使用Landau-Lifshitz方程的对称性将周期解的存在性转化为常微分方程,从而证明了具有非零常值外磁场的Landau-Lifshitz方程具有非平凡的周期解,同时对于时间相关的外磁场,我们构造了若干具有典型动力学意义的特解.     

Ginzburg-Landau方程极小能量解存在性的新证明

对R~2上带有外磁场或一般流源场的Ginzburg-Landau方程组,借助于Hardy型不等式,利用直接变分的方法重新证明了其极小能量解的存在性,且该解满足Coulomb规范.     

高速扩展平面应力裂纹尖端的各向异性塑性场

在裂纹尖端的应力分量都只是θ的函数的条件下,利用定常运动方程,Hill各向异性屈服条件及应力应变关系,我们得到高速扩展平面应力裂纹尖端的各向异性塑性场的一般解.将这个一般解用于四种各向异性特殊情形,我们就导出这四种特殊情形的一般解.最后,本文给出X=Y=Z情形的高速扩展平面应力Ⅰ型裂纹尖端的各向异性塑性场.     

高速扩展裂纹尖端的各向异性塑性场

在裂纹尖端的应力分量都只是θ的函数的条件下,利用定常运动方程,应力应变关系及Hill各向异性屈服条件,我们得到反平面应变和平面应变两者裂纹尖端的各向异性塑性场的一般解.将这些一般解用于具体裂纹,我们就求出了Ⅰ型和Ⅱ型裂纹的高速扩展尖端的各向异性塑性场,     

各向异性相态场模型的Gibbs—Thompson关系

本文利用奇异摄动的内、外解匹配方法,分析了各向异性时在相态场模型的边界层上表面张菌、法向速度、平均曲率和各向异性函数的影响,得到了各向异性时的Ｇｉｂｂｓ－Ｔｈｏｍｐｓｏｎ关系,以及边界层所满足的方程。     

渗透各向异性土层的平面应变固结

提出了一种有效的可供选择的分析方法,来研究渗透各向异性多孔弹性土层的平面应变固结问题.从饱和多孔弹性土体的控制方程出发,建立了在Laplace-Fourier变换域内,土层中地基表面(z=0)和深度z处基本变量之间的关系.结合边界条件,得到了变换域内渗透各向异性有限土层的平面应变Biot固结问题的精确解.通过Laplace-Fourier逆变换,得到了物理域内的真实解.平面应变Biot固结土层的数值分析结果显示:渗透各向异性对土层的固结行为,有比较显著的影响.     

Explicit piecewise smooth solutions of Landau-Lifshitz equation with discontinuous external field

In this paper, we shall construct some explicit piecewise smooth （global continuous） solutions as well as blow up solutions to the multidimensional Landau-Lifshitz equation, subject to the external magnetic fields being both discontinuous and unbounded. When the external magnetic field is continuous, some explicit exact smooth solutions and blow up solution are also constructed. We also establish some necessary and sufficient conditions to ensure that the solution of multidimensional Landau-Lifshitz equation with external magnetic field converges to the solution of equation without external magnetic field when the external magnetic field tends to zero.     

Some exact solutions to multidimensional Landau-Lifshitz equation with uprush external field and anisotropy field

In this paper we give a method that can construct some exact solutions to a multidimensional Landau-Lifshitz equation with uprush external field and anisotropy field.     

Stresses in elastic conical tubes of transversely isotropic materials with spherical anisotropies under temperature and force loadings

Analytic solutions are proposed for a number of new problems on determining the state of stress of a transversely-isotropic hollow cone with spherical anisotropy. An exact solution of the problem of the axisymmetric deformation of a long conical tube (or continuous cone) from an elastic transversely-isotropic material with spherical anisotropy subjected to an axial force is obtained in a spherical coordinate system R, , θ, the material axis of symmetry is directed along the spherical radius R. A rigorous solution is given of the problem of the uniform heating of a conical tube of transversely-isotropic material with spherical anisotropy for particular values of Poisson's ratios; the material axis of symmetry is directed along the θ-axis. For arbitrary Poisson's ratios an asymptotic solution is found for the temperature problem for a tube with small conicity.     

Adiabatic approximations for Landau-Lifshitz equations

The asymptotics with respect to a small parameter for solutions of a system of Landau-Lifshitz equations with slowly varying coefficients and small dissipative terms is investigated. These equations are a mathematical model of a uniaxial ferromagnet in a time-dependent magnetic field. The asymptotics constructed make it possible to describe the magnetization reversal effect and to reveal the influence of the parameters of the external magnetic field and dissipation on the stability of this process.     

On in‐out splitting of incident fields and the far‐field behaviour of Herglotz wavefunctions

It is easy to write down entire solutions of the Helmholtz equation: Examples are plane waves and Herglotz wavefunctions. We are interested in the far‐field behaviour of these solutions motivated by the following question: When is it legitimate to split the far field of such an entire solution into the sum of an incoming spherical wave and an outgoing spherical wave? We review the relevant literature (there are disjoint physical and mathematical threads), and then we answer the question for Herglotz wavefunctions, using a combination of the 2‐dimensional method of stationary phase and some explicit examples.     

Motion of magnetic domain walls

We consider the dynamics of one-dimensional micromagnetic domain walls in layers of uniaxial anisotropy. In the regime of bulk materials, i.e. when the thickness is assumed to be infinite, and the magnetostatic interaction terms appear as local quantities, explicit traveling wave solutions for the corresponding Landau-Lifshitz equation, known asWalker exact solutions, can be constructed. A natural question is whether this construction can be perturbed to the non-local regime of layers of finite thickness. Our stability analysis gives an affirmative answer. (© 2005 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)     

BUBBLES OF LANDAU-LIFSHITZ EQUATIONS WITH APPLIED FIELDS

In this paper, we discuss the Landau-Lifshitz equations with applied magnetic fields. The equations describing the bubbles in the ferromagnets and the behaviors of the solutions near the singularities are given. We found that the applied fields do not affect the bubbles and we have the same conclusions as in reference [1].     

Neutral Fermion with a Magnetic Moment in External Electromagnetic Fields

The interaction between a massive neutral fermion with a static (spin) magnetic dipole moment and an external electromagnetic field is described by the Dirac–Pauli equation. Exact solutions of this equation are obtained along with the corresponding energy spectrum for an axially symmetric external magnetic field and for some centrally symmetric electric fields. It is shown that the spin–orbital interaction of a neutral fermion with a magnetic moment determines both the characteristic properties of the quantum states and the fermion energy spectrum. It is found that (1) the discrete energy spectrum of a neutral fermion depends on the projection of the fermion spin on a certain quantization axis, (2) the ground energy level of a fermion in these electric fields as well as the energy levels of all bound states with a fixed value of the quantum number characterizing the projection of the fermion spin in the electric field E = er is degenerate and the degeneration order is countably infinite, and (3) the energy spectra of neutral fermions and antifermions with spin magnetic moments are symmetric in centrally symmetric fields. Bound states of a neutral fermion with a magnetic moment in an external electric field do exist even if the Dirac–Pauli equation does not explicitly contain the term with the fermion mass. In addition, in centrally symmetric electric fields, there exist a countably infinite set of pairs of isolated charge-conjugate zero-energy solutions of the Dirac–Pauli equation.     

Initial-boundary value problems for anisotropic Landau-Lifshitz equations in three or four space dimensions

In this paper, we will show the existence of partially regular solutions to the initial-boundary value problem for Landau-Lifshitz equations with nonpositive anisotropy constants in three or four space dimensions. The partial regularity is proved up to the boundary both for the Dirichlet problem and for the Neumann problem. In addition, for the Neumann case, a generalized stability condition which ensures the partial regularity is given. For equations with positive or negative anisotropy coefficients, we will give two results of existence and uniqueness for the solutions corresponding to ground states.     

Interaction of a breather with a magnetization wave in a ferromagnet with light-axis anisotropy

We use the dressing method to find exact solutions of the Landau-Lifshitz equation for a ferromagnet with light-axis anisotropy. These solutions describe the interaction of a nonlinear precession wave of arbitrary amplitude with solitons. We analyze the change of the internal structure and the physical parameters of the solitons as a result of their interaction with the magnetization wave. We find an infinite series of integrals of motion that stabilize the soliton on the background of the pumping wave.