REPRESENTATION THEOREM AND ONE-ITERATION THEOREM FOR FREDHOLM INTEGRAL EQUATION OF THE FIRST KIND Ax=y

In this paper,two theorems are presented.The representation theorem states:if the Fredholm integral equation of the first kind Ax=y,with bounded L_2 kernel,has a uniquesolution(?),then(?),whereThe one-iteration theorem states:(?)can be achieved in one iteration by(?)=x_0 g_0 A*(y-Ax_0)iff one of the following conditions is satisfied.     

Singularly perturbed nonlinear second order elliptic equation

In this paper, we study singular perturbation problems of some semi-linear second order elliptic equations with nonlinear boundary value conditions: where ε is a small positive parameter and u/ l is a directional derivative, which lies on an oblique vector (x,ε). We have given a construction of the asymptotic solutions and proof of their asymptotic correctness, which is based on the principle of contraction mapping.     

Multiplicity results for a fourth-order boundary value problem

ＭＵＬＴＩＰＬＩＣＩＴＹＲＥＳＵＬＴＳＦＯＲＡＦＯＵＲＴＨ－ＯＲＤＥＲＢＯＵＮＤＡＲＹＶＡＬＵＥＰＲＯＢＬＥＭＭａＲｕｙｕｎ（马如云）ＭａＱｉｎｓｈｅｎｇ（马勤生）（ＲｅｃｅｉｖｅｄＯｃｔ．５．１９９４：ＣｏｍｍｕｎｉｃａｔｅｄｂｙＬｉｎＺｏｎｇｃｈ...     

Necessary and sufficient conditions for the absolute stability of discrete type lurie control system

ＮＥＣＥＳＳＡＲＹＡＮＤＳＵＦＦＩＣＩＥＮＴＣＯＮＤＩＴＩＯＮＳＦＯＲＴＨＥＡＢＳＯＬＵＴＥＳＴＡＢＩＬＩＴＹＯＦＤＩＳＣＲＥＴＥＴＹＰＥＬＵＲＩＥＣＯＮＴＲＯＬＳＹＳＴＥＭＺｈａｎｇＪｉｙｅ（张继业）（ＲｅｃｅｉｘｅｄＯｃｔ．５．１９９４Ｃｏｍｍｕ...     

THE HLDER CONTINUITY FOR THE GRADIENT OF SOLUTIONS TO ONE-SIDED OBSTACLE PROBLEMS

The Hölder continuity is proved for the gradient of the solution Jo the one-sided obstacle problem of the following variational inequality in the case 1相似文献   

Extended graphical representation of rational fractions with applications to cybernetics

In this paper,we discuss the extended graphical representation ofthe fraction of a complex variable sWhere K is confined to be real.Three figures of the above fraction canbe used in feedback systems as well as to study the properties of figuresfor any one coefficient of a characteristic equation as a real parameter.It is easy to prove the following theorem:K_1=f(n)(s)/F(d)(s)and K_2=F(d)(s)/f(n)(s)have the same root locus.By this graphical theory,we find out that if the zeros and polesof a fraction are alternatively placed on the axis x,then there is nocomplex root locus of this fraction,therefore the state of such a sys-tem is always non-oscillatory.Using these figures of this,fraction,wecan discuss its stable interval systematically.     

The traction problem in elastodynamics

In continuum mechanics, Cauchy's six equations are incomplete, and the famous Cauchy's laws of motion where ρ(?), ρb, T and divT are continuous are also incomplete. The first six equations are incomplete because the geometrical representation of deformation at a given point is as yet incomplete, and the last two laws are incomplete because b,T and divT are frame-indifferent, but ρ(?) is not, and T is a symmetric, as Cauchy interpreted himself. Therefore, we say, the last two laws can't accommodate to the asymmetric tensor. The purpose of this paper is to complete Cauchy's laws of motion by postulating an asymmetric tensor for the underlying traction field of 3-dimensional space on a general framing.     

On the global asymptotic stability of periodic solutions of a class of ecological system

In this paper, we have made reaearches on the mathematical models which have three populations of mutual action: We have obtained the sufficient conditions respectively for the systems(*)and(**)for existence and uniqueness of single positive periodic solutions which are globally asymptotically stable.     

The floquet theory for quasi-periodic linear systems

In this paper we establish the Floquet theory for the quasi-perio-dic systemwhere A(u_1,u_2,…,u_m)is an n×n periodic matrix function of u_1,u_2.…,u_mwith period 2π,and it is of C~τ,τ=(N 1)τ_0,τ_0=2(m 1).N=(1/2)n(n 1).Meanwhile,we define the characteristic exponential roots β_1,β_2,…,β_nof(0.1),and assume thatwhere K(ω),K(ω,β)>0.k_μ,j_v.are integers,all the integers k_1,k_2,…,k_m.are not zero,i~2=-1,Then there exists aquasi-periodic linear transformation,which carries(0.1)into a li-near system with constant coefficients.     

Singular perturbation of boundary value problems for second order nonlinear ordinary differential equations on infinite interval (I)

In this paper existence, uniqueness and asymptotic estimations of solutions of the boundary value problems on infinite interval for the second order nonlinear equation depending singularly on a small parameter ε>0 are examined, where α_i, β are constants, and i=0,1.     

Doubly Curved Shallow Shells with the Rectangular Base Elastically Supported by Edge Arched Beams and Tie-Rods (Ⅱ)

In order to study the boundary conditions of integrated form(91a,d),firstlywe make use of trigonometrical series to express N_ξη(0,η),Q_ξ^*(0,η)of(97C,D).Suppose .     

SINGULAR PERTURBATION OF NONLINEAR BOUNDARY VALUE PROBLEMS

In this paper we consider the boundary value problem where ε.μ are two positive parameters. Under f_y≤-k<0 and other suitable restrictions, there exists a solution and it satisfied where y_(0,0)(x) is solution of reduced problem while y_i-j,j(x)(j=0,1,...,i;i=1,2,...,m) can be obtained successively from certain linear equations.     

The application of the asymptotic method to a clas of strongly nonlinear systems

In this paper, according to the form of the asymptotic solution of papers [1, 2], the asymptotic method is extended to the following a class of more general strong nonlinear vibration systems where g and f are the nonlinear analytical-functions of x and x, and ε>0 is a small parameter. We assume that the derivative system corresponding to ε=0 has periodic solution. The recurrence equations of the asymptotic solution for the system(0.1)are deduced in this paper, and they are applied to practical examples.     

Note on the critical variational state in elasticity theory

Recently Prof. Chien Wei-zang pointed out that in certain cases, by means of ordinary Lagrange multiplier method, some of undetermined Lagrange multipliers may turn out to be zero during variation. This is a critical state of variation. In this critical state, the corresponding variational constraint can not be eliminated by means of simple Lagrange multiplier method. This is indeed the case when one tries to eliminate the constraint condition of strain-stress relation in variational principle of minimum complementary energy by the method of Lagrange multiplier.By means of Lagrange multiplier method, one can only derive, from minimum complementary energy principle, the Hellinger-Reissner Principle, in which only two type of in-dependent variables, stresses and displacements, exist in the new functional. Hence Prof. Chien introduced the high-order Lagrang multiplier method bu adding the quadratic terms.to original functions. The purpose of this paper is to show that by adding to original functionals one     

On singular perturbation boundary-value problem of coupling type system of convection-diffusion equations

In this paper we consider the singular perturbation boundary-value problem of thefollowing coupling type system of convection-diffusion equationsWe advance two methods:the first one is the initial value solving method,by which theoriginal boundary-value problem is changed into a series of unperturbed initial-valueproblems of the first order ordinary differential equation or system so that an asymptoticexpansion is obtained;the second one is the boundary-value solving method,by which theoriginal problem is changed into a few boundary-value problems having no phenomenon ofboundary-layer so that the exact solution can be obtained and any classical numericalmethods can be used to obtain the numerical solution of consismethods can be used to obtainthe numerical solution of consistant high accuracy with respect to the perturbationparameterε     

Theory of pressure swirl atomisation and study on the characteristic of droplet size in atomisation

Based on the observation of the working condition in pressure swirl atomisationexperiments,this article tries to suggest a model of the mechanism of pressure swirlatomisation—the atomisation theory of pressure swirl spray of conical film.Under somebasic assumptions,the formula for the characteristic of droplet size of pressure swirlatomisation is derived:The above theory agrees basically with the actual working conditions in atomisation,andgives the latter a compratively good interpretation.In this article,theoretical calculations are worked out for the characteristic ofatomised droplet size of some Oil atomising nozzles used in power plants in our country(thePeople＇s Republic of China)and are compared with actual test data.The results show thatthe theory is of some value to preactice,and it is recommended to those concerned forreference.     

The criterion algorithm of relation of implication between periodic orbits (I)

In recent years, there is a wide interest in Sarkovskii’s theorem ami the related study. According to Sarkovskii’s theoren if the continuous self-mapf of the closed interval has a 3-pcriodic orbit, then fmust has an n-pcriodic orbit for any positive integer n. But f can not has all n-periodic orbits for some n.For example, let Evidently, f has only one kind of 3-periodic orbit in the two kinds of 3-periodic orbits. This explains that it isn’t far enough to uncover the relation between periodic orbits by information which Sarkovskii’s theorem has offered. In this paper, we raise the concept of type of periodic orbits, and give a feasible algorithm which decides the relation of implication between two periodic orbits.     

The global structural stability and application of the toroidal differntial equations\left\{ {\begin{array}{*{20}c} {\dot x = a_1 [\sin (x - y) - \sin x] - \Delta \omega } \\ {\dot y = a_2 [\sin (y - x) - \sin y] - \Delta \omega } \\ \end{array} } \right.

In this paper, the global structural stability of the toroidal differential equationshas been obtained, and applied to the cross-coupled phase - locked loop, where Δω≥0     

The boundedness and asymptotic behavior of solutions of differential system of second-order with variable coefficients

In this paper, the differential system of second-order withvariable coefficients is studied. and some criteria of theboundedness and asymptotic behavior for solutions are given.Consider a system of differential equationsdx_1/dt=p_(11)(t)x_1 p_(12)(t)x_2dx_2/dt=p_(21)(t)x_1 p_(22)(t)x_2Now we studg the boundedness and asymptotic behavior of its so-lutions. In the case of Pij(t)being periodic functions. it wasinvestigated by Burdina; in the case of Pij(t) being arbitraryfunctions. it has not been investigated yet. Besides. the me-thod used by Burdina is only oppropriate for the former but notfor the latter case. In this paper we shall give a method whichis appropriate for both cases.     

Nonstationary random vibration of one-degree and multidegree of freedom systems

In ref.[1]for nonstationary random processes such aswe defined the spectral densityS_ξ(t,ω)=|f(t,ω)|~2S(ω)where Z(A)is an orthogonal random measure,S(ω)is the spectral density of thestationary random processf(t,ω)is a complex function with two real variables,it is called modulation functionand it is satisfied byIn ref[1]we obtained the main results:for the linear dynamic systems which isdescribed by such equationswe obtained under certain conditions thatwherehere W(t,τ)is the response function of the systems to the unit pulse.This paper is continued on ref.[1].We obtain some results for the one-degree andmultidegree of freedom systems.