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1.
????? 《力学与实践》1990,12(1):57-58
<正> 动量矩定理有多种形式,常用的形式可归纳如下:(1)对定矩心 o′的绝对动量矩定理(?)_0=L_0 (1)(2)在平动参考系 O′x′y′z′中对矩心 O′的相对  相似文献   

2.
This is a series of studies on Wu’s conjecture and on its resolution to be presented herein. Both are devoted to expound all the comprehensive properties of Cauchy’s function f(z) (z = x + iy) and its integral J[f(z) ] ≡(2πi) -1 C f(t)(t z) -1dt taken along the unit circle as contour C,inside which(the open domain D+) f(z) is regular but has singularities distributed in open domain Doutside C. Resolution is given to the inverse problem that the singularities of f(z) can be determined in analytical form in terms of the values f(t) of f(z) numerically prescribed on C(|t| = 1) ,as so enunciated by Wu’s conjecture. The case of a single singularity is solved using complex algebra and analysis to acquire the solution structure for a standard reference. Multiple singularities are resolved by reducing them to a single one by elimination in principle,for which purpose a general asymptotic method is developed here for resolution to the conjecture by induction,and essential singularities are treated with employing the generalized Hilbert transforms. These new methods are applicable to relevant problems in mathematics,engineering and technology in analogy with resolving the inverse problem presented here.  相似文献   

3.
We propose a theoretical model for spatial variations of the temperature variance σ~2( z, r)( z is the distance from the sample bottom and r the radial coordinate) in turbulent Rayleigh-Bénard convection(RBC).Adapting the "attached-eddy" model of shear flow to the plumes of RBC, we derived an equation for σ~2 which is based on the universal scaling of the normalized RBC temperature spectra. This equation includes both logarithmic and power-law dependences on z/λ_(th), where λ_(th) is the thermal boundary layer thickness. The equation parameters depend on r and the Prandtl number Pr, but have only an extremely weak dependence on the Rayleigh number Ra Thus our model provides a near-universal equation for the temperature variance profile in turbulent RBC.  相似文献   

4.
周衍柏编“理论力学教程”1986年第二版中增加了一个内容,讲用广义坐标及拉格朗日乘子来求约束反力(见该书p.279—280),笔者认为是错误的.为讨论方便起见,先将该段内容摘引如下,其中重点号为笔者所加.“首先,应当利用(5.1.8)式把(5.2.12)式中3n个x、y、z 改用S 个广义坐际q_(?)(α=1,2,…s)表出,则约束方程将变为(?)(q_1,q_2,…q_(?))=0(β=1,2,…k)(5.2.22)k 为体系所受到完整约束的数目,而虚位移δq。则应  相似文献   

5.
周衍柏编"理论力学教程"1986年第二版中增加了一个内容,讲用广义坐标及拉格朗日乘子来求约束反力(见该书p.279-280),笔者认为是错误的.为讨论方便起见,先将该段内容摘引如下,其中重点号为笔者所加."首先,应当利用(5.1.8)式把(5.2.12)式中3n个x、y、z 改用S 个广义坐际q_(?)(α=1,2,…s)表出,则约束方程将变为(?)(q_1,q_2,…q_(?))=0(β=1,2,…k)(5.2.22)k 为体系所受到完整约束的数目,而虚位移δq。则应 ...  相似文献   

6.
本文证明:对于薄壁杆件,偏心弯曲会引起约束扭转.假设翘曲位移w(z,s)=-θ(z)·Q(s),在开闭截面相接处,有θ_(?)(z)=αθ_l(z),并允许有相对刚体位移.在弥合翘曲差异时,局部应力系Δσ起了作用,从轴向力平衡、弯矩平衡、双力矩平衡决定待定常数α,使翘曲位移在连接处"有可能"连续.实例表明,与有限元法结果符合甚好.  相似文献   

7.
In this paper,we consider the vector nonlinear boundary value problem:εy~v=f(x,y,z,y′,ε),y(0)=A_1,y(1)=B_1εz~v=g(x,y,z,z′,ε),z(0)=A_2,z(1)=B_2whereε>0 is a small parameter,0≤x≤1 ,f and g are continuous functions in R~4,Under appropriate assumptions,by means of the differential inequalities,we demonstratethe existence and estimation,involving boundary and interior layers,of the solutions to theabove problem.  相似文献   

8.
??? 《力学与实践》1990,12(4):50-52
<正> 1.两类基本应力函数束众所周知,空间轴对称问题的基本应力函数(?)(r,(?))由双调和方程确定.本文采用变换(?)(r,z)=r~2f(r,z)或(?)(r,z)=(?)~2g(r,z)将方程(1)化为 f(r,z)或 g(r,z)的新方程,再利用[2]提出的变换-分离变量法求解此新方程,从而得到空间轴对称问题的两类基本应力函数.  相似文献   

9.
1.两类基本应力函数束众所周知,空间轴对称问题的基本应力函数(?)(r,(?))由双调和方程确定.本文采用变换(?)(r,z)=r~2f(r,z)或(?)(r,z)=(?)~2g(r,z)将方程(1)化为 f(r,z)或 g(r,z)的新方程,再利用[2]提出的变换-分离变量法求解此新方程,从而得到空间轴对称问题的两类基本应力函数.  相似文献   

10.
This article studies on Cauchy’s function f (z) and its integral, (2πi)J[ f (z)] ≡■C f (t)dt/(t z) taken along a closed simple contour C, in regard to their comprehensive properties over the entire z = x + iy plane consisted of the simply connected open domain D + bounded by C and the open domain D outside C. (1) With f (z) assumed to be C n (n < ∞-times continuously differentiable) z ∈ D + and in a neighborhood of C, f (z) and its derivatives f (n) (z) are proved uniformly continuous in the closed domain D + = [D + + C]. (2) Cauchy’s integral formulas and their derivatives z ∈ D + (or z ∈ D ) are proved to converge uniformly in D + (or in D = [D +C]), respectively, thereby rendering the integral formulas valid over the entire z-plane. (3) The same claims (as for f (z) and J[ f (z)]) are shown extended to hold for the complement function F(z), defined to be C n z ∈ D and about C. (4) The uniform convergence theorems for f (z) and F(z) shown for arbitrary contour C are adapted to find special domains in the upper or lower half z-planes and those inside and outside the unit circle |z| = 1 such that the four general- ized Hilbert-type integral transforms are proved. (5) Further, the singularity distribution of f (z) in D is elucidated by considering the direct problem exemplified with several typ- ical singularities prescribed in D . (6) A comparative study is made between generalized integral formulas and Plemelj’s formulas on their differing basic properties. (7) Physical sig- nificances of these formulas are illustrated with applicationsto nonlinear airfoil theory. (8) Finally, an unsolved inverse problem to determine all the singularities of Cauchy function f (z) in domain D , based on the continuous numerical value of f (z) z ∈ D + = [D + + C], is presented for resolution as a conjecture.  相似文献   

11.
1 相移技术场移云纹:一种绝对值测量的新技术(A.J.Boehnlein等,美国工业技术研究所)。正弦位相调制的激光二极管干涉仪(带有能抑制外部干扰的反馈控制系统)(O.Sasaki等,日本Niigata大学)。动态条纹投影非接触式测量(M.M.Shaw等,英国Liverpool工学院)。用杨氏条纹鉴相器的高精度延迟测量(S.Nakadate,日本东京工业大学)。六闪光(Hexflash)位相分析实例(L.N.Mertz,美国Lockheed研究实验室)。  相似文献   

12.
考虑矩形截面环形管道(图1):0≤z′≤L,r′_1≤r′≤r′_2.上下壁为绝缘壁,在 z 轴方向加匀强磁场 B_0.内外壁为理想导体,用作电极,在径向通以电流 I.管道内导电流体就在电磁力作用下旋转起来(单极机).设导电率σ及粘性系数η都是常数.设 ...  相似文献   

13.
Two simple integral equation methods are proposed for the analysisof vertical loaded pile.One of them is:let the axisymmetrical loads formedby Mindlin’s horizontal point forces be distributed along the axis z in[0,L]of the elastic half-space,and composed with the Boussinesq’s pointforce.The other is:in addition to the above fictitious loads,the Mind-lin’s vertical forces are distributed along the axis z in[0,L].The form-er reduces the problem of a vertical loaded pile embedded in a half-spacewith the following boundary conditions.  相似文献   

14.
1.弯曲问题的数学提法 本文讨论有同心圆弧裂缝的圆柱和圆管的线弹性弯曲。直角坐标系z轴平行于柱轴;x,y轴是截面的惯性主轴;原点在柱体的端面;力W在另一端面z=l沿x方向作用,则受弯曲柱体的应力分布为:  相似文献   

15.
I.Intr0ductionForflndingallzerosofacomplexpolynomialofdegree;Ip(z)=zu olz'-l ..' a.-1z a.(l.l)whenzerosareal1simple,manymethodsareavailable.AmongthemaretheDurand-Kerneralgorithm,theAberthalgorithm,thesquarerootingaIg0rithmandtheirvarietiesI3'[1'141.Thecom…  相似文献   

16.
The response of turbulent enstrophy to a sudden implementation of spanwise wall oscillation(SWO) is studied in a turbulent channel flow via direct numerical simulation. In the beginning of the application of SWO, a significant correlation is formed between ω′yand ω′z. A transient growth of turbulent enstrophy occurs, which directly enhances turbulent dissipation and drifts the turbulent flow towards a new lower-drag condition. Afterwards, the terms related to the stretching of vorticity(ωx, ω′y, and ωz),the inclination of ω′yby ?w/?y, the turn of z by ?v′/?z, and the horizontal shear of z by ?w′/?x are suppressed due to the presence of SWO, leading to attenuation of the turbulent enstrophy.  相似文献   

17.
IntroductionIn 1 7thcenturyIsaacNewton[1]gavesuchabinomialexpressionforfractionalandnegativeexponents(1 +t) α,i.e.,(1 +t) α =1 + +∞k=1α(α-1 ) (α-2 )… (α -k+ 1 )k !tk   (α≠ 0 ,1 ,2 ,… ) ,(1 )whoseconvergenceradiusisone.Furthermore ,theclassicalTaylorseries (seeRef.[2 ] )limm→+∞ mk=0f(k) (z0 )k !(z-z0 ) k (2 )ofacomplexfunctionf(z)atz=z0 isvalidmostlyinarestrictedconvergenceregion|z-z0 |相似文献   

18.
IntroductionLetX ,YbetwotopologicalspacesandZbeanonemptyset.LetF∶X×X→ 2 Z,A∶X→ 2 XandC∶X→ 2 Zbeset_valuedmappingswhere2 ZdenotesthefamilyofallsubsetsofZ .  Thegeneralizedvectorquasi_equilibriumproblemofType (Ⅰ ) (inshort,GVQEP(Ⅰ ) )istofind ^x∈Xsuchthat^x∈A( ^x)andF( ^x ,z) C( ^x) ,   z∈A( ^x) . ( 1 )  Thegeneralizedvectorquasi_equilibriumproblemofType (Ⅱ ) (inshort,GVQEP(Ⅱ ) )istofind ^x∈Xsuchthat^x∈A( ^x)andF( ^x ,z) C( ^x) ,   z∈A( ^x) . ( 2 )  …  相似文献   

19.
采用准连续介质多尺度方法模拟了纳米尺度单晶铝的剪切变形.分别采用三种不同晶体取向(分别为x[1-10],y[001],z[-1-10]; x[-1-12],y[111],z[-110]; x[-110],y[-1-12],z[111])和三种不同长宽比的几何模型(分别为1:1,2:1,4:1)进行模拟,得出各模型应力一应变响应曲线.加载过程中,对晶体内部变形比较剧烈的部分画出原子图,并从微观角度分析了产生剧烈变形的原因;讨论了三种晶体取向下的尺寸效应:单晶铝的剪切屈服应力随模型几何尺寸的增加而降低,并且随晶体取向的不同变化很大.最后,使用指数法则来描述模型的尺寸效应,提出了针对不同取向的指数法则参数,表明了晶体不同取向对剪切屈服应力的大小有影响.  相似文献   

20.
1.IntroductionWeconsiderthequadraticdifferentialsystemoftype(II)and(ill):.z~~y sx IXZ mxg g','~x(l ox)(1.1)f~~g 6x lx' mxy ny','~x(l ax by)(1.2)Asacontributionofsolvingbifurcationproblemofquadraticsystems,westudyinthispaperbifurcationofcriticalpoints(CPs)…  相似文献   

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