正交变换在曲线,曲面积分计算中的应用

正交变换在曲线、曲面积分计算中的应用林元重（江西萍乡高等专科学校３３７０５５）对于三维空间的曲线积分与曲面积分，如果知道其积分曲线或积分曲面的参数形式，一般可按数学分析教材所介绍的公式计算．但是，对于某些曲线、曲面积分，要把积分曲线或曲面用适当的参数...     

正交变换在图像压缩中的应用

用矩阵表示图像,构造正交均值差分变换矩阵,对原始图像进行正交变换,进一步取阈值,仅存储绝对值大于阈值的系数,获得数据压缩.解压缩过程只需作逆均值差分变换.最后将该算法分别应用于灰度和彩色图像的压缩处理,结果验证了算法的有效性.由于算法中所有变换都通过矩阵运算处理,且意义直观明了,故该算法是大学线性代数教学中一个非常好的应用案例.     

论二次型与正交变换在重积分中的某些应用

二次型与正交变换是代数学的基本内容，其用途十分广泛，而重积分的计算往往存在技术性的困难，若利用“二次型”与“正交变换”的有关理论去解决某些重积分的计算问题是颇有功效的。本文将以“二型”与“正交变换”为工具，乘法的处理了一大批重积分的问题。     

论二次型与正交变换在重积分中的某些应用

二次型与正交变换是代数学的基本内容 ,其用途十分广泛 .而重积分的计算往往存在技术性的困难 ,若利用“二次型”与“正交变换”的有关理论去解决某些重积分的计算问题是颇有功效的 .本文将以“二次型”与“正交变换”为工具 ,简洁的处理了一大批重积分的问题     

带有局部源的非局部扩散方程组的Fujita现象

本文研究了一类带有局部源的非局部扩散系统$u_t=J*u-u+a(x)v^{p}$, $v_t=J*v-v+a(x)u^q$的柯西问题,首先根据是否存在全局解建立了Fujita曲线$(pq)_c=1+\max \{p+1,q+1\}$,也即证明了:如果$1(pq)_c$时,则既存在全局解,也存在非全局解.然后我还根据初始值在无穷远处的衰减率建立了第二临界曲线.     

非局部平面曲线流

本文首先综述近年来关于平面曲线流(尤其是非局部平面凸曲线流)的一系列研究进展.之后研究平面凸曲线的一个广义保面积流,并证明在演化过程中,演化曲线始终保持凸性,并且长度递减,最终当时间趋于无穷时,演化曲线光滑收敛到一个圆周.     

关于曲线上稳定秩2局部自由层在基变换下拉回的稳定性

本文主要给出稳定秩２局部自由层在基变换下其拉回层不稳定的例。     

对称性与局部支集样条函数构造

1引言令D为二维串连通区域,用不可约代数曲线对D进行剖分西,得胞腔。,i—l,…,N．D上n次广阶光滑的样条函数空间定义为S：（D,凸）一｛f6or（D）,f。一片;6尺｝在两相邻胞腔。和个上,SESZ（D,凸）满足其中l。为人与4的公共内网线,q。称为S在l。上的光滑余因子．进而分片多项式S6s：（,凸）,当且仅当在任一内网线上存在光滑余因子,且在任一内网点A处满足协调条件Zc／xx。一。其中求和对所有以A为一端点的内网线进行［”‘j．以上定义和基本结果是文1中给出的．这种方法称为光滑余因子协条法．此外在多元样条函数的研究…     

局部对称黎曼流形中的超曲面

研究了局部对称黎曼流形中具有常平均曲率超曲面的几何性质,得到了关于其第二基本形式模长平方的拼挤定理.     

Hamilton体系辛半解析法及在非均匀电磁波导中的应用

力学中的Hamilton体系需用对偶变量来描述,而电磁场正好有电场和磁场这一对对偶变量．尝试将力学中的Hamilton体系理论应用于电磁波导的分析,以横向电场和磁场作为对偶变量,将电磁波导的基本方程导向辛几何的形式．基于Hamilton变分原理, 导出横向离散的半解析系统方程, 保持体系的辛结构．以非均匀波导为例, 求解了方程的辛本征值问题, 计算结果与解析解相当吻合．     

LOCAL ORTHOGONAL TRANSFORMATION FOR ACOUSTIC WAVEGUIDE

§ 1　IntroductionLarge scale wave propagation problems in acoustics,electro-magnetism,seismic mi-gration and other applications often require the solution ofa variable coefficient Helmholtzequation in a domain with a very large length,as compared with the typical wavelength.Standard mumerical methods,such as the finite difference and finite element methods,give rise to very large linear systems,because a few grid points(or basis functions) are al-ways required for each wavelength to resolve t…     

A perturbative method for the spectral analysis of an acoustic multistratified strip

We consider the acoustic propagator A=−∇·c²∇ in the strip Ω={(x, z)∈ℝ²∣0<z<H} with finite width H>0. The celerity c depends for large ∣x∣ only on the variable z and describes the stratification of Ω: it is assumed to be in L^∞(Ω), bounded from below by c_min>0, such that there exists M>0 with c(x, z)=c₁(z) if x< −M and c(x, z)=c₂(z) if x>M. We look at the propagator A as a ‘perturbation’ of the free propagators A_j in Ω associated to the velocities c_j, j=1, 2, and implement a ‘perturbative’ method, adapting ideas of Majda and Vainberg. The spectrum of A is defined in section 2, a limiting absorption principle is proved in section 3 outside of a countable set Γ(A). The points of Γ(A) can only accumulate at the left of the thresholds of the free propagators. The needed material about A_j, j=1, 2, and some technical estimates for A are given in Appendix. © 1998 B. G. Teubner Stuttgart—John Wiley & Sons, Ltd.     

A decomposition scheme for acoustic obstacle scattering in a multilayered medium

We consider the acoustic wave scattering by an impenetrable obstacle embedded in a multilayered background medium, which is modelled by a linear system constituted by the Helmholtz equations with different wave numbers and the transmission conditions across the interfaces. The aim of this article is to construct an efficient computing scheme for the scattered waves for this complex scattering process, with a rigorous mathematical analysis. First, we construct a set of functions by a series of coupled transmission problems, which are proven to be well-defined. Then, the solution to our complex scattering in each layer is decomposed as the summation in terms of these functions, which are essentially the contributions from two interfaces enclosing this layer. These contributions physically correspond to the scattered fields for simple scattering problems, which do not involve the multiple scattering and are coupled via the boundary conditions. Finally, we propose an iteration scheme to compute the wave field in each layer decoupling the multiple scattering effects, with the advantage that only the solvers for the well-known transmission problems and an obstacle scattering problem in a homogeneous background medium are applied. The convergence property of this iteration scheme is proven.     

Orthogonality of eigenwaves in a semi-open elastic waveguide

We consider a two-layer elastic waveguide structure such that its one layer is unbounded in the lateral direction, and the standard boundary conditions are stated on the boundary of another one. We study several kinds of eigenwaves for this structure. In general, they have a complex-valued longitudinal propagation constant (the spectral parameter). On the base of the Green formula we introduce the scalar product of two waves and prove that the system of eigenwaves of the semiopen elastic waveguide is orthogonal. We construct families of waves which belong to discrete and continuous parts of the spectrum.     

Inverse problem for structural acoustic interaction

We consider an inverse problem of determining a source term for a structural acoustic partial differential equation (PDE) model that is comprised of a two- or a three-dimensional interior acoustic wave equation coupled to an elastic plate equation. The coupling takes place across a boundary interface. For this PDE system, we obtain uniqueness and stability estimates for the source term from a single measurement of boundary values of the “structure” (acceleration of the elastic plate). The proof of uniqueness is based on a Carleman estimate (first version) of the wave problem within the chamber. The proof of stability relies on three main points: (i) a more refined Carleman estimate (second version) and its resulting implication, a continuous observability-type estimate; (ii) a compactness/uniqueness argument; (iii) an operator theoretic approach for obtaining the needed regularity in terms of the initial conditions.     

632.8-nm visible region waveguide polarizer fabricated by proton exchange

Optical waveguide polarizer at 632.8 nm was fabricated for the first time using proton exchange Ti:LiNbO₃. The setup measuring the characteristic parameters of the polarizer was given. The extinction ratio of the polarizer was theoretically analyzed and calculated by means of physical optics and dispersion theory for waveguide. Various factors affecting the device performance are analyzed. Theoretical calculations are in good agreement with the experimental results.     

反演声波阻尼系数的另一种方法

提出了一种方法,利用正则化方法和积分方程,由散射波的近场数据反演时间调和声波阻尼系数.给出了该方法收敛性的证明及数值例子,算法与数值例子表明这种方法不仅简单而且很有效.     

Detection of multilayered media in the acoustic waveguide

This work is concerned with the inverse problem for ocean acoustics modeled by a multilayered waveguide with a finite depth. We provide explicit formulae to locate the layers, including the seabed, and reconstruct the speed of sound and the densities in each layer from measurements collected on the surface of the waveguide. We proceed in two steps. First, we use Gaussian type excitations on the upper surface of the waveguide and then from the corresponding scattered fields, collected on the same surface, we recover the boundary spectral data of the related 1D spectral problem. Second, from these spectral data, we reconstruct the values of the normal derivatives of the singular solutions, of the original waveguide problem, on that upper surface. Finally, we derive formulae to reconstruct the layers from these values based on the asymptotic expansion of these singular solutions in terms of the source points.