对非线性椭圆边值问题解的存在性的研究

利用非线性增生映射值域的扰动定理 ,研究了非线性椭圆边值问题 ( @)在 L2 (Ω )中解的存在性 .( @) -△pu +g( x,u) =f a.e.在Ω中-〈v,| u|p- 2 u〉∈βx( u( x) ) a.e.在Γ上其中 f∈ L2 (Ω )给定 ,Ω RN,N 1 ,△ pu=div( | u|p- 2 u)为 P拉普拉斯算子 ,1 2 NN +1 ,v为 Γ的外法向导数 ,g:Ω× R→ R满足 Caratheodory条件 ,对 x∈ Γ,βx是正常、凸、下半连续函数 φx=φ( x,· )的次微分 ,其中 φ:Γ×R→ R.     

W.Janous猜测的再推广

W .Janous猜测 :设x ,y,z >0 ,则x2 -z2y+z + y2 -x2z+x + z2 -y2x+y ≥ 0 ( 1 )贵刊文 [1 ]将 ( 1 )式推广为 :设xi>0 (i =1 ,2 ,… ,n) ,n≥ 3,记S=x1 +x2 +… +xn,t =x21+x22 +… +x2 n,则nx21 -ts-x1 + nx22 -ts-x2 +… + nx2 n-ts-xn ≥ 0 ( 2 )当n =3时 ,由 ( 2 )式可得 ( 1 )式 .本文将把 ( 2 )式作进一步推广 ,并回答文 [1 ]中提出的一个问题 .我们得到如下结果 :设xi>0 (i=1 ,2 ,… ,n) ,n≥ 3,α ,β,γ∈R ,T =xα1 +xα2 +… +xαn,A>max{xγ1 ,xγ2 ,… ,xγn},则当αβγ >0时 ,有nxα1 -T(A-xγ1 )β+ nxα2 -T(A-xγ2 )…     

一类新的二次p元Bent函数的构造

设m为正整数,n=2m,p为一奇素数,令d=pm+1/2,e|m,其中a∈F*pn,γ是Fpn中的一非平方元.本文研究了有限域Fpn上的函数F(x)=Tr1n(axpm+e+1-γdxpm+1),利用有限域上的二次型理论,证明了在m/e为奇数的条件下或m/e为偶数但a(pn-1)/(pe+1)≠1的条件下,F(x)为p元弱正则Bent函数.     

关于非线性椭圆边值问题解的存在性的注

利用非线性增生映射值域的扰动理论,本文研究了与P拉普拉斯算子△p相关的非线性椭圆边值问题@在Ls(Ω)空间中解的存在性,其中2>sp>2nn+1且n1.@-Δpu+|u(x)|p-2u(x)+g(x,u(x))=fa.e.x∈Ω-〈υ,|u|p-2u〉=0a.e.x∈Γ其中f∈Ls(Ω)给定,ΩRn,n1,Δpu=div(|u|p-2u)为P拉普拉斯算子,υ为Γ的外法向导数,g∶Ω×R→R满足Caratheodory条件.本文所讨论的方程及所用的方法是对以往一些工作的补充和延续.     

有界线性算子的摄动定理

本文研究了正则算子的摄动理论.考虑Banach空间X上的正则算子T,假设dim[K(T)∩N(T)]<∞且K(T)闭,则当S∈B(X)可逆,ST=TS,‖S‖充分小时,证明了T—S为上半Fredholm算子.在以上条件下,若K(T)+N(T)或者R(T)+N(T)在X中有有限维的补子空间,这时T—S为Fredholm算子.     

S-内射模及S-内射包络

设R是环.设S是一个左R-模簇,E是左R-模.若对任何N∈S,有Ext_R~1(N,E)=0,则E称为S-内射模.本文证明了若S是Baer模簇,则关于S-内射模的Baer准则成立;若S是完备模簇,则每个模有S-内射包络;若对任何单模N,Ext_R~1(N,E)=0,则E称为极大性内射模;若R是交换环,且对任何挠模N,Ext_R~1(N,E)=0,则E称为正则性内射模.作为应用,证明了每个模有极大性内射包络.也证明了交换环R是SM环当且仅当T/R的正则性内射包e(T/R)是∑-正则性内射模,其中T=T(R)表示R的完全分式环,当且仅当每一GV-无挠的正则性内射模是∑-正则性内射模.     

应力、强度均服从瑞利（Rayleigh）分布的可靠性分析

在应力—强度干涉模型中,当应力、强度均服从瑞利(Rayleigh)分布:R(x│β)={2βxexp[(-xβ2)],x00x<0,参数未知的情况下,讨论了在给定验前分布情况下的可靠性R=P(Y相似文献   

偏线性模型的核——最小二乘估计法的渐近性质

设有偏线性模型 Y=X′β+g(T)+e,其中(X,T)为取值于 R~p×[0,1]上的随机向量,β为 p×1未知参数向量,g是定义于[0,1]上的未知函数,e 为随机误差,均值是0,方差σ~2>0未知,且 e 与(X,T)独立.本文综合核和最小二乘的方法定义了β,g和σ~2的估计量和,在十分自然合理的条件下证明了和的渐近正态性,并得到了g_n~*的最优收敛速度.     

2007年普通高等学校招生全国统一考试(海南宁夏卷)

数学(理科)参考公式:样本数据x1,x2,…,xn的标准差S=1n[(x1-x)2 (x2-x)2 … (xn-x)2]其中x为样本平均数.柱体体积公式V=Sh其中S为底面面积,h为高.锥体体积公式V=31Sh,其中S为底面面积,h为高.球的表面积、体积公式S=4πR2,V=34πR3其中R为球的半径.第Ⅰ卷一、选择题:本大题共12小题,每小题5分,在每小题给出的四个选项中,只有一项是符合题目要求的.1·已知命题p∶x∈R,sinx≤1,则A·┒p∶x∈R,sinx≥1B·┒p∶x∈R,sinx≥1C·┒p∶x∈R,sinx>1D·┒p∶x∈R,sinx>12·已知平面向量a=(1,1),b=(1,-1)则向量12a-23b=A·(-2,-1)B·(-2,1)…     

多目标数学规划的对偶性

<正> R.R.Egudo 和M.A.Hanson 在文[2]中讨论了如下一类多目标数学规划的对偶性其中f:R~n→R~k,g:R~n→R~m 是向量值函数,e=(1,1,…,1)~T ∈R~k,λ∈W~(++)={ω|ω_i>0,sum from i=1 to k ω_i=1}。文[2]对多目标非凸规划(VP)和(VD)关于真有效解给出了弱对偶和强对偶定理。本文将(VP)和(VD)推广为如下一类常闭凸锥约束的多目标数学规划问题     

Stability of the Riemann solutions for a nonstrictly hyperbolic system of conservation laws

We prove that the Riemann solutions are stable for a nonstrictly hyperbolic system of conservation laws under local small perturbations of the Riemann initial data. The proof is based on the detailed analysis of the interactions of delta shock waves with shock waves and rarefaction waves. During the interaction process of the delta shock wave with the rarefaction wave, a new kind of nonclassical wave, namely a delta contact discontinuity, is discovered here, which is a Dirac delta function supported on a contact discontinuity and has already appeared in the interaction process for the magnetohydrodynamics equations [M. Nedeljkov and M. Oberguggenberger, Interactions of delta shock waves in a strictly hyperbolic system of conservation laws, J. Math. Anal. Appl. 344 (2008) 1143-1157]. Moreover, the global structures and large time asymptotic behaviors of the solutions are constructed and analyzed case by case.     

The Riemann problem for the pressure-gradient system in three pieces

The Riemann problem for a two-dimensional pressure-gradient system is considered. The initial data are three constants in three fan domains forming different angles. Under the assumption that only a rarefaction wave, shock wave or contact discontinuity connects two neighboring constant initial states, it is proved that the cases involving three rarefaction waves are impossible. For the cases involving one shock (rarefaction) wave and two rarefaction (shock) waves, only the combinations when the three elementary waves have the same sign are possible (impossible).     

On the Riemann problem for 2D compressible Euler equations in three pieces

The Riemann problem for two-dimensional isentropic Euler equations is considered. The initial data are three constants in three fan domains forming different angles. Under the assumption that only a rarefaction wave, shock wave or contact discontinuity connects two neighboring constant initial states, it is proved that the cases involving three shock or rarefaction waves are impossible. For the cases involving one rarefaction (shock) wave and two shock (rarefaction) waves, only the combinations when the three elementary waves have the same sign are possible (impossible).     

Global entropy solutions to the relativistic Euler equations for a class of large initial data

We are concerned with global entropy solutions to the relativistic Euler equations for a class of large initial data which involve the interaction of shock waves and rarefaction waves. We first carefully analyze the global behavior of the shock curves, the rarefaction wave curves, and their corresponding inverse curves in the phase plane. Based on these analyses, we use the Glimm scheme to construct global entropy solutions to the relativistic Euler equations for the class of large discontinuous initial data.     

Global entropy solutions to the relativistic Euler equations for a class of large initial data

We are concerned with global entropy solutions to the relativistic Euler equations for a class of large initial data which involve the interaction of shock waves and rarefaction waves. We first carefully analyze the global behavior of the shock curves, the rarefaction wave curves, and their corresponding inverse curves in the phase plane. Based on these analyses, we use the Glimm scheme to construct global entropy solutions to the relativistic Euler equations for the class of large discontinuous initial data.Received: May 23, 2004     

Interactions of delta shock waves for a class of nonstrictly hyperbolic system of conservation laws

In this paper, we study the perturbed Riemann problem for a class of nonstrictly hyperbolic system of conservation laws, and focuse on the interactions of delta shock waves with the shock waves and the rarefaction waves. The global solutions are constructed completely with the method of splitting delta function. In solutions, we find a new kind of nonclassical wave, which is called delta contact discontinuity with Dirac delta function in both components. It is quite different from the previous ones on which only one state variable contains the Dirac delta function. Moreover, by letting perturbed parameter $\varepsilon$ tend to zero, we analyze the stability of Riemann solutions.     

绝热流Chaplygin气体的Riemann问题

本文研究了绝热流Chaplygin气体动力学方程组,利用特征分析方法,在得到所有基本波的基础上,构造出Riemann问题的所有解.Riemann解由前向疏散波(激波)、后向疏散波(激波)、接触间断以及δ波构成.     

The singular solutions to a nonsymmetric system of Keyfitz-Kranzer type with initial data of Riemann type

The solutions to the Riemann problem for a nonsymmetric system of Keyfitz-Kranzer type are constructed explicitly when the initial data are located in the quarter phase plane. In particular, some singular hyperbolic waves are discovered when one of the Riemann initial data is located on the boundary of the quarter phase plane, such as the delta shock wave and some composite waves in which the contact discontinuity coincides with the shock wave or the wave back of rarefaction wave. The double Riemann problem for this system with three piecewise constant states is also considered when the delta shock wave is involved. Furthermore, the global solutions to the double Riemann problem are constructed through studying the interaction between the delta shock wave and the other elementary waves by using the method of characteristics. Some interesting nonlinear phenomena are discovered during the process of constructing solutions; for example, a delta shock wave is decomposed into a delta contact discontinuity and a shock wave.     

一维Chaplygin气体欧拉方程组中波的相互作用

研究一维Chaplygin气体欧拉方程组中波的相互作用.方程组的波包含接触间断和在密度变量以及内能变量上同时具有狄拉克函数的狄拉克激波.根据这些波的不同组合,问题被分成了7种情形.通过详细地构造每种情形的整体解,获得了各种波相互作用的完整结果.特别地,对于一类初值,两个接触间断相互作用后,产生了一个狄拉克激波;然而,对于另外一类初值,一个狄拉克激波与一个接触间断相互作用后,狄拉克激波消失.这些都是波相互作用中非常特别的现象.     

ZERO DISSIPATION LIMIT TO A RIEMANN SOLUTION FOR THE COMPRESSIBLE NAVIER-STOKES SYSTEM OF GENERAL GAS

For the general gas including ideal polytropic gas, we study the zero dissipation limit problem of the full 1-D compressible Navier-Stokes equations toward the superposition of contact discontinuity and two rarefaction waves. In the case of both smooth and Riemann initial data, we show that if the solutions to the corresponding Euler system consist of the composite wave of two rarefaction wave and contact discontinuity, then there exist solutions to Navier-Stokes equations which converge to the Riemman solutions away from the initial layer with a decay rate in any fixed time interval as the viscosity and the heat-conductivity coefficients tend to zero. The proof is based on scaling arguments, the construction of the approximate profiles and delicate energy estimates. Notice that we have no need to restrict the strengths of the contact discontinuity and rarefaction waves to be small.