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岩土工程专业翻译英文原文和译文

岩土工程专业翻译英文原文和译文
岩土工程专业翻译英文原文和译文

毕业设计---外文翻译

原作题目:Failure Properties of Fractured Rock Masses as

Anisotropic Homogenized Media

译作题目:均质各向异性裂隙岩体的破坏特性

专业:土木工程

姓名:吴雄

指导教师:吴雄志

河北工程大学土木工程学院

2012年5月21日

Failure Properties of Fractured Rock Masses as Anisotropic

Homogenized Media

Introduction

It is commonly acknowledged that rock masses always display discontinuous surfaces of various sizes and orientations, usually referred to as fractures or joints. Since the latter have much poorer mechanical characteristics than the rock material, they play a decisive role in the overall behavior of rock structures,whose deformation as well as failure patterns are mainly governed by those of the joints. It follows that, from a geomechanical engineering standpoint, design methods of structures involving jointed rock masses, must absolutely account for such ‘‘weakness’’ surfaces in their analysis.

The most straightforward way of dealing with this situation is to treat the jointed rock mass as an assemblage of pieces of intact rock material in mutual interaction through the separating joint interfaces. Many design-oriented methods relating to this kind of approach have been developed in the past decades, among them,the well-known ‘‘block theory,’’ which attempts to identify poten-

tially unstable lumps of rock from geometrical and kinematical considerations (Goodman and Shi 1985; Warburton 1987; Goodman 1995). One should also quote the widely used distinct element method, originating from the works of Cundall and coauthors (Cundall and S track 1979; Cundall 1988), which makes use of an explicit ?nite-difference numerical scheme for computing the displacements of the blocks considered as rigid or deformable bodies. In this context, attention is primarily focused on the formulation of realistic models for describing the joint behavior.

Since the previously mentioned direct approach is becoming highly complex, and then numerically untractable, as soon as a very large number of blocks is involved, it seems advisable to look for alternative methods such as those derived from the concept of homogenization. Actually, such a concept is already partially conveyed in an empirical fashion by the famous Hoek and Brown’s criterion (Hoek and Brown 1980; Hoek 1983). It stems from the intuitive idea that from a macroscopic point of view, a rock mass intersected by a regular network of joint surfaces, may be perceived as a homogeneous continuum. Furthermore, owing to the existence of joint preferential orientations, one should expect such a homogenized material to exhibit anisotropic properties.

The objective of the present paper is to derive a rigorous formulation for the failure criterion of a jointed rock mass as a homogenized medium, from the knowledge of the joints and rock material respective criteria. In the particular situation where twomutually orthogonal joint sets are considered, a closed-form expression is obtained, giving clear evidence of the related strength anisotropy. A comparison is performed on an illustrative example between the results produced by the homogenization method,making use of the previously determined criterion, and those obtained by means of a computer code based on the distinct element method. It is shown that, while both methods lead to almost identical results for a densely fr actured rock mass, a ‘‘size’’ or ‘‘scale effect’’ is observed in the case of a limited number of joints. The second part of the paper is then devoted to proposing a method which attempts to capture such a scale effect, while still taking advantage of a homogenization technique. This is

achieved by resorting to a micropolar or Cosserat continuum description of the fractured rock mass, through the derivation of a generalized macroscopic failure condition expressed in terms of stresses and couple stresses. The implementation of this model is ?nally illustrated on a simple example, showing how it may actually account for such a scale effect.

Problem Statement and Principle of Homogenization Approach

The problem under consideration is that of a foundation (bridge pier or abutment) resting upon a fractured bedrock (Fig. 1), whose bearing

capacity needs to be evaluated from the knowledge of the strength capacities of the rock matrix and the joint interfaces. The failure condition of the former will be expressed through

C and the the classical Mohr-Coulomb condition expressed by means of the cohesion

m

. Note that tensile stresses will be counted positive throughout the paper. friction angle

m

Likewise, the joints will be modeled as plane interfaces (represented by lines in the ?gure’s plane). Their strength properties are described by means of a condition involving the stress vector of components (σ, τ) acting at any point of those interfaces

According to the yield design (or limit analysis) reasoning, the above structure will remain safe under a given vertical load Q(force per unit length along the Oz axis), if one can exhibit throughout the rock mass a stress distribution which satis?es the equilibrium equations along with the stress boundary conditions,while complying with the strength requirement expressed at any point of the structure.

This problem amounts to evaluating the ultimate load Q﹢beyond which failure will occur, or equivalently within which its stability is ensured. Due to the strong heterogeneity of the jointed rock mass, insurmountable dif?culties are likely to arise when trying to implement the above reasoning directly. As regards, for instance, the case where the strength properties of the joints are considerably lower than those of the rock matrix, the implementation of a kinematic approach would require the use of failure mechanisms involving velocity jumps

across the joints, since the latter would constitute preferential zones for the occurrence of

failure. Indeed, such a direct approach which is applied in most classical design methods, is becoming rapidly complex as the density of joints increases, that is as the typical joint spacing l is becoming small in comparison with a characteristic length of the structure such as the foundation width B.

In such a situation, the use of an alternative approach based on the idea of homogenization and related concept of macroscopic equivalent continuum for the jointed rock mass, may be appropriate for dealing with such a problem. More details about this theory, applied in the context of reinforced soil and rock mechanics, will be found in (de Buhan et al. 1989; de Buhan and Salenc ,on 1990; Bernaud et al. 1995).

Macroscopic Failure Condition for Jointed Rock Mass

The formulation of the macroscopic failure condition of a jointed rock mass may be obtained from the solution of an auxiliary yield design boundary-value problem attached to a unit representative cell of jointed rock (Bekaert and Maghous 1996; Maghous et al.1998). It will now be explicitly formulated in the particular situation of two mutually orthogonal sets of joints under plane strain conditions. Referring to an orthonormal frame O 21ξξwhose axes are placed along the joints directions, and introducing the following change of stress variables:

such a macroscopic failure condition simply becomes

where it will be assumed that

A convenient representation of the macroscopic criterion is to draw the strength envelope relating to an oriented facet of the homogenized material, whose unit normal n I is inclined by an angle a with respect to the joint direction. Denoting by n σ and n τthe normal and shear components of the stress vector acting upon such a facet, it is possible to determine for any value of a the set of admissible stresses (n σ , n τ) deduced from conditions (3) expressed in terms of (11σ,22σ , 12σ). The corresponding domain has been drawn in Fig. 2 in the

particular case where m ?α≤ .

Two comments are worth being made:

1. The decrease in strength of a rock material due to the presence of joints is clearly illustrated by Fig.

2. The usual strength envelope corresponding to the rock matrix failure condition is ‘‘truncated’’ by two orthogonal semilines as soon as condition m j H H is ful?lled.

2. The macroscopic anisotropy is also quite apparent, since for instance the strength envelope drawn in Fig. 2 is dependent on the facet orientation a. The usual notion of intrinsic curve should therefore be discarded, but also the concepts of anisotropic cohesion and friction angle as tentatively introduced by Jaeger (1960), or Mc Lamore and Gray (1967).

Nor can such an anisotropy be properly described by means of criteria based on an extension of the classical Mohr-Coulomb condition using the concept of anisotropy tensor(Boehler and Sawczuk 1977; Nova 1980; Allirot and Bochler1981).

Application to Stability of Jointed Rock Excavation

The closed-form expression (3) obtained for the macroscopic failure condition, makes it then possible to perform the failure design of any structure built in such a material, such as the excavation shown in Fig. 3,

where h and β denote the excavation height and the slope angle, respectively. Since no

surcharge is applied to the structure, the speci?c weight γ of the constituent material will obviously constitute the sole loading parameter of the system.Assessing the stability of this structure will amount to evaluating the maximum possible height h + beyond which failure will occur. A standard dimensional analysis of this problem shows that this critical height may be put in the form

where θ=joint orienta tion and K +=nondimensional factor governing the stability of the excavation. Upper-bound estimates of this factor will now be determined by means of the yield design kinematic approach, using two kinds of failure mechanisms shown in Fig. 4.

Rotational Failure Mechanism [Fig. 4(a)]

The ?rst class of failure mechanisms considered in the analysis is a direct transposition of those usually employed for homogeneous and isotropic soil or rock slopes. In such a mechanism a volume of homogenized jointed rock mass is rotating about a point Ω with an angular velocity ω. The curve separating this volume from the rest of the structure which is kept motionless is a velocity jump line. Since it is an arc of the log spiral of angle m and focus Ω the v elocity discontinuity at any point of this line is inclined at angle wm with respect to the tangent at the same point.

The work done by the external forces and the maximum resisting work developed in such a mechanism may be written as (see Chen and Liu 1990; Maghous et al. 1998)

where e w and me w =dimensionless functions, and μ1 and μ2=angles specifying the

position of the center of rotation Ω.Since the kinematic approach of yield design states that a necessary condition for the structure to be stable writes

it follows from Eqs. (5) and (6) that the best upper-bound estimate derived from this ?rst class of mechanism is obtained by minimization with respect to μ1 and μ2

which may be determined numerically.

Piecewise Rigid-Block Failure Mechanism [Fig. 4(b)]

The second class of failure mechanisms involves two translating blocks of homogenized material. It is de?ned by ?ve angular parameters. In order to avoid any misinterpretation, it should be speci?ed that the termino logy of block does not refer here to the lumps of rock matrix in the initial structure, but merely means that, in the framework of the yield design kinematic approach, a wedge of homogenized jointed rock mass is given a (virtual) rigid-body motion.

The implementation of the upper-bound kinematic approach,making use of of this second class of failure mechanism, leads to the following results.

where U represents the norm of the velocity of the lower block. Hence, the following upper-bound estimate for K+:

Results and Comparison with Direct Calculation

The optimal bound has been computed numerically for the following set of parameters:

The result obtained from the homogenization approach can then be compared with that derived from a direct calculation, using the UDEC computer software (Hart et al. 1988). Since the latter can handle situations where the position of each individual joint is speci?ed, a series of calculations has been performed varying the number n of regularly spaced joints, inclined at th e same angleθ=10° with the horizontal, and intersecting the facing of the excavation, as sketched in Fig. 5. The

corresponding estimates of the stability factor have been plotted against n in the same ?gure. It can be observed that these numerical estimates decrease with the number of intersecting joints down to the estimate produced by the homogenization approach. The observed discrepancy between homogenization and direct approaches, could be regarded as a ‘‘size’’ or ‘‘scale effect’’ which is not inclu ded in the classical

homogenization model. A possible way to overcome such a limitation of the latter, while still taking advantage of the homogenization concept as a computational time-saving alternative for design purposes, could be to resort to a description of the fractured rock medium as a Cosserat or micropolar continuum, as advocated for instance by Biot (1967); Besdo(1985); Adhikary and Dyskin (1997); and Sulem and Mulhaus (1997) for strati?ed or block structures. The second part of this paper is devoted to applying such a model to describing the failure properties of jointed rock media.

均质各向异性裂隙岩体的破坏特性

概述

由于岩体表面的裂隙或节理大小与倾向不同,人们通常把岩体看做是非连续的。尽管裂隙或节理表现出的力学性质要远远低于岩体本身,但是它们在岩体结构性质方面起着重要的作用,岩体本身的变形和破坏模式也主要是由这些节理所决定的。从地质力学工程角度而言,在涉及到节理岩体结构的设计方法中,软弱表面是一个很重要的考虑因素。

解决这种问题最简单的方法就是把岩体看作是许多完整岩块的集合,这些岩块之间有很多相交的节理面。这种方法在过去的几十年中被设计者们广泛采用,其中比较著名的是“块体理论”,该理论试图从几何学和运动学的角度用来判别潜在的不稳定岩块(Goodman & 石根华1985;Warburton 1987;Goodman 1995);另外一种广泛使用的方法是特殊单元法,它是由Cundall及其合作者(Cundall & Strack 1979;Cundall 1988)提出来的,其目的是用来求解显式有限差分数值问题,计算刚性块体或柔性块体的位移。本文的重点是阐述如何利用公式来描述实际的节理模型。

既然直接求解的方法很复杂,数值分析方法也很难驾驭,同时由于涉及到了数目如此之多的块体,所以寻求利用均质化的方法是一个明智的选择。事实上,这个概念早在Hoek-Brown准则(Hoek & Brown 1980;Hoek 1983)得出的一个经验公式中就有所涉及,它来自于宏观上的一个直觉,被一个规则的表面节理网络所分割的岩体,可以看做是一个均质的连续体,由于节理倾向的不同,这样的一个均质材料显示出了各向异性的性质。

本文的目的就是:从节理和岩体各自准则出发,推求出一个严格准确的公式,来描述作为均匀介质的节理岩体的破坏准则。先考查特殊情况,从两组相互正交的节理着手,得到一个封闭的表达式,清楚的证明了强度的各向异性。我们进行了一项试验:把利用均质化方法得到的结果和以前普遍使用的准则得到的结果以及基于计算机编程的特殊单元法(DEM)得到的结果进行了对比,结果表明:对于密集裂隙的岩体,结果基本一致;对于节理数目较少的岩体,存在一个尺寸效应(或者称为比例效应)。本文的第二部分就是在保证均质化方法优点的前提下,致力于提出一个新的方法来解决这种尺寸效应,基于应力和应力耦合的宏观破坏条件,提出利用微极模型或者Cosserat连续模型来描述节理岩体;最后将会用一个简单的例子来演示如何应用这个模型来解决比例效应的问题。

问题的陈述和均质化方法的原理

考虑这样一个问题:一个基础(桥墩或者其邻接处)建立在一个有裂隙的岩床上

(Fig.1),岩床的承载能力通过岩基和节理交界面的强度

估算出来。岩基的破坏条件使用传统的莫尔-库伦条件,可以用粘聚力C 1和内摩擦角? m 来表示(本文中张应力采用正值计算)。同样,用接触平面代替节理(图示平面中用直线表示)。强度特性采用接触面上任意点的应力向量(σ,τ)表示:

根据屈服设计(或极限分析)推断,如果沿着应力边界条件,岩体应力分布满足平

衡方程和结构任意点的强度要求,那么在一个给定的竖向荷载Q(沿着OZ 轴方向)作

用下,上部结构仍然安全。

这个问题可以归结为求解破坏发生处的极限承载力Q+,或者是多大外力作用下结构能确保稳定。由于节理岩体强度的各向异性,若试图使用上述直接推求的方法,难度就会增大很多。比如,由于节理强度特性远远低于岩基,从运动学角度出发的方法要求考虑到破坏机理,这就牵涉到了节理上的速度突跃,而节理处将会是首先发生破坏的区域。

这种应用在大多数传统设计中的直接方法,随着节理密度的增加越来越复杂。确切

地说,这是因为相比较结构的长度(如基础宽B)而言,典型节理间距L变得更小,加

大了问题的难度。在这种情况下,对节理岩体使用均质化方法和宏观等效连续的相关概

念来处理可能就会比较妥当。关于这个理论的更多细节,在有关于加固岩土力学的文章

中可以查到(de Buhan等1989;de Buhan & Salenc 1990;Bernaud等1995)。

节理岩体的宏观破坏条件

节理岩体的宏观破坏条件公式可以从对节理岩体典型晶胞单元的辅助屈服设计边值问题中得到(Bekaert & Maghous 1996; Maghous 等 1998)。现在可以精确地表示平面应变条件下,两组相互正交节理的特殊情况,建立沿节理方向的正交坐标系O 21ξξ ,并引入下列应力变量:

观破坏条件可简化为:

其中,假定

宏观准则的一种简便表示方法是画出均质材料倾向面上的强度包络线,其单位法线n 的倾角α 为节理的方向,分别用σn 和τn 表示这个面上的正应力和切应力,用(11σ,22σ , 12σ) 表示条件(3),推求出一组许可应力(σn ,τn ),然后求解出倾角α 。当α ≥? m 时,相应的区域表示如图2所示,并对此做出两个注解如下:

1. 从图2中可以清楚的看出,节理的存在导致了岩体强度的降低。通常当m j H H <时,强度包络线和岩基破坏条件相一致,其前半部分被两个正交的半条线切去。

2. 宏观各向异性很显著。比如,图2中的强度包络线决定于方位角α 。应该抛弃

固有曲线和各向异性粘聚力与摩擦角的概念,其中后一个概念是由Jaeger(1960)或Mc Lamore & Gray(1967)所引入的。通过莫尔-库伦条件进行扩展,利用各向异性张量的方法来描述各向异性也是不妥当的(Boehler & Sawczuk 1977;Nova 1980;Allirot & Bochler 1981) 。

在节理岩体开挖稳定性中的应用

式(3)的封闭形式是从宏观破坏条件中得到的,该式可以用来对此种材料的结构体进行破坏设计,如图3所示的开挖,h 和β分别表示开挖高度和边坡

角。由于结构上没有其他荷载,材料比重γ就成为系统唯一的加载参数。该结构的稳定性评价需要在破坏发生的部位算出最大可能高度h+,通过标准量纲分析表明,这个临界高度表示为:

其中θ为节理方位角,K +为表示开挖部位稳定性的一个无量纲因子,该因子的上界估计值可以分别使用图4所示的两种类型的破坏机制,通过屈服设计的运动学方法来确定。

转动破坏机理[Fig. 4(a)]

第一种类型的破坏机制,通常把分析对象直接转换为均匀各向同性的岩坡(或土坡)。若采用这种破坏机制,各向同性的节理岩体围绕点Ω产生角速度为ω的旋转,把静止的部分和运动的部分分开的曲线即为速度突跃线,在这条角度为?m、圆心为Ω的滑弧上的任意一点上,速度都不是连续的,速度方向与该点处的切线成倾角?m。

在这种破坏机制下,外力所做的功和最大抵抗功可以表示为下列形式(Chen & Liu 1990;Maghous 等。

w e和w mr为无量纲函数,

μ1和μ2为滑移体的圆心角,由于屈服设计状态的动力学方法是结构稳固的一个必要条件,故有:

联立(5)式和(6)式,取μ1和μ2的最小值进行计算,可以得到第一种类型破坏机制的最佳上界估计:

分段刚性块体破坏机理[Fig. 4(b)]

第二种类型的破坏机制涉及到了两种均匀材料块体的转换,由五个角度参数定义。为了避免误解,应该具体指出,“块体”并不是指代初始状态下的岩基块体,在屈服设计运动学方法的框架下,它代表的不仅仅这个意思,一块均质节理岩体的运动可以近似看做是刚体运动。

对于第二种类型的破坏机制,运用上界运动学方法,可以得出以下结果:(在Fréard (2000)的文中可以找到详细的计算过程)

其中U 表示下盘块体的速度(如图4-b所示)。因此,K +

上界估计值为:

计算结果以及与直接计算结果之间的对比

经过计算,选定最优上界参数值为:

屈服时有

利用UDEC软件(Hart等1988)对均质化方法的计算结果和直接计算方法的结果进行对比发现,当每一个节理的位置都已知时,利用后一种方法就可以求解这个问题,当节理间隙很规则,且倾角保持在与水平成10 °的方向切割开挖平面时,随着节理数n的变化,计算出一系列的结果,点绘于图5中,与n相应的稳定性因子的估计值也在图5中表示出来,容易看出,随着分割节理数目的降低,这些估计值

的大小降低到了均质化方法的估计值。均质化方法和直接计算法的差异可以看成是由于“尺寸效应”而引起的,而均质化方法并没有尺寸效应的问题。为了设计上计算的省时高效,克服直接计算法的局限,同时要运用均质化的概念,考虑对裂隙岩体介质采用一种新的描述方法——Cosserat 或者是微极连续,Biot (1967),Besdo (1985),Adhikary & Dyskin (1997),以及Sulem & Mulhaus (1997) 对于分层岩体或者是块体结构都有所描述。本文的第二部分就是致力于应用这个模型来描述节理岩体介质的破坏特性。

英语原文及其翻译

Exploring Filipino School Counselors’ Beliefs about Learning Allan B. I. Bernardo [Abstract] School reform efforts that focus on student learning require school counselors to take on important new roles as advocates of student learning and achievement.But how do school counselors understand the process of learning? In this study, we explore the learning beliefs of 115 Filipino school counselors who indicated their degree of agreementwith 42 statements about the process of learning and the factors thatinfluence this process.A principal components analysis of the responses to the 42 statements suggested three factors:(F1)social-cognitive constructivist beliefs, (F2) teacher-curriculum-centered behaviorist beliefs,and (F3) individual difference factors.The preliminary results are briefly discussed in terms of issues related to how Filipino school counselors’ conceptions of learning may guide their strategies for promoting student learning and achievement. [Key words]beliefs about learning, conceptions of learning, school counselors, student learning, Philippines School reform efforts in different parts of the world have focusedon students’learning. In particular,most school improvement programsnow aim to ensure that students acquire the high-level knowledge and skills that help them to thrive in today’s highly competitive globaleconomy (e.g., Lee & Williams, 2006). I n this regard, school reform programs draw from various contemporary theories and research on learning (e.g.,Bransford,Brown, & Cocking, 1999; Lambert & McCombs, 1998).The basic idea is that all school improvement efforts should be directed at ensuring students achieve high levels of learning or attainment of well-defined curricular objectives and standards.For example, textbooks (Chien & Young, 2007), computers and educational technology (Gravoso, 2002; Haertnel & Means, 2003;Technology in Schools Task Force, 2003), and educational assessment systems (Black & Wiliam2004; Cheung & Ng, 2007; Clark, 2001; Stiggins, 2005) are being reconsidered as regards how they can effectively provide scaffolds and resources for advancing student learning. Likewise,the allocation and management of a school’s financial resources are assessed in terms ofwhether these are effectively mobilized and utilized towards improving student learning (Bolam, 2006; Chung & Hung, 2006; Retna, 2007). In this regard, some advocates have also called for an examination of the role of school counselors in these reform efforts (Herr, 2002). Inthe United States, House and Hayes (2002) challenged school counselors to take proactive leadership roles in advocating for the success of all

蓝梅主编 给排水科学与工程专业英语部分课文翻译中文版

第四单元给水系统 一般来说,供水系统可划分为四个主要组成部分:(1)水源和取水工程(2)水处理和存储(3)输水干管和配水管网。常见的未处理的水或者说是原水的来源是像河流、湖泊、泉水、人造水库之类的地表水源以及像岩洞和水井之类的地下水源。修建取水构筑物和泵站是为了从这些水源中取水。原水通过输水干管输送到自来水厂进行处理并且处理后的出水储存到清水池。处理的程度取决于原水的水质和出水水质要求。有时候,地下水的水质是如此的好以至于在供给给用户之前只需消毒即可。由于自来水厂一般是根据平均日需求流量设计的,所以,清水池为水需求日变化量提供了一个缓冲区。 水通过输水干管长距离输送。如果输水干管中的水流是通过泵所产生的压力水头维持的,那么我们称这个干管为增压管。另外,如果输水干管中的水流是靠由于高差产生的可获得的重力势能维持的,那么我们称这个干管为重力管。在输水干管中没有中间取水。与输水干管类似,在配水管网中水流的维持要么靠泵增压,要么靠重力势能。一般来说,在平坦地区,大的配水管网中的水压是靠泵提供的,然而,在不平坦的地区,配水管网中的压力水头是靠重力势能维持的。 一个配水管网通过引入管连接配水给用户。这样的配水管网可能有不同的形状,并且这些形状取决于这个地区的布局。一般地,配水管网有环状或枝状的管道结构,但是,根据当地城市道路和街区总体布局计划,有时候环状和枝状结构合用。城市配水管网大多上是环状形式,然而,乡村地区的管网是枝状形式。由于供水服务可靠性要求高,环状管网优于枝状管网。 配水管网的成本取决于对管网的几何形状合适的选择。城市计划采用的街道布局的选择对提供一个最小成本的供水系统来说是重要的。环状管网最常见的两个供水结构是方格状、环状和辐射状;然而,我们不可能找到一个最佳的几何形状而使得成本最低。 一般地,城镇供水系统是单入口环状管系统。如上所说,环状系统有一些通过系统相互连接的管道使得通过这些连接接的管道,可以供水到同一个需水点。与枝状系统不同,在环状系统中,由于需水量在空间和时间上的变化,管道中的水流方向并非不变。 环状管网可为系统提供余量,提高系统应对局部变化的能力,并且保证管道故障时为用户供水。从水质方面来说,环状形状可减少水龄,因此被推广。管道的尺寸和配水系统的设计对减少水龄来说是重要的因素。由于多方向水流模式和系统中流动模式随时间的变化,水不会停留在一个地方,这样减少了水龄。环状配水系统的优缺点如表4.1所述。 优点:1.Minimize loss of services.as main breaks can be isolated due to multidirectional flow to demand points.2.Reliability for fire protection is higher due to redundancy in the system.3.Likely to meet increase in water demand -higher capacity and lower velocities.4.Better residual chlorine due to in line mixing and fewer dead ends. 5.Reduced water age. 在文献中曾记载过,只考虑最低成本设计的环状管网系统会转化成树状似的结构,这一做法导致在最终的设计中失去最初的几何形状。环状保证了系统的可靠性。因此,一个只考虑最低成本为依据的设计打败了在环状管网中所提供的基本功能。有文献记载设计环状管网系统的方法。尽管这个方法也是仅以考虑最低成本为基础,它通过对管网中所有管道最优化规划从而保持了管网的环状结构。

文献翻译英文原文

https://www.sodocs.net/doc/4312179314.html,/finance/company/consumer.html Consumer finance company The consumer finance division of the SG group of France has become highly active within India. They plan to offer finance for vehicles and two-wheelers to consumers, aiming to provide close to Rs. 400 billion in India in the next few years of its operations. The SG group is also dealing in stock broking, asset management, investment banking, private banking, information technology and business processing. SG group has ventured into the rapidly growing consumer credit market in India, and have plans to construct a headquarters at Kolkata. The AIG Group has been approved by the RBI to set up a non-banking finance company (NBFC). AIG seeks to introduce its consumer finance and asset management businesses in India. AIG Capital India plans to emphasize credit cards, mortgage financing, consumer durable financing and personal loans. Leading Indian and international concerns like the HSBC, Deutsche Bank, Goldman Sachs, Barclays and HDFC Bank are also waiting to be approved by the Reserve Bank of India to initiate similar operations. AIG is presently involved in insurance and financial services in more than one hundred countries. The affiliates of the AIG Group also provide retirement and asset management services all over the world. Many international companies have been looking at NBFC business because of the growing consumer finance market. Unlike foreign banks, there are no strictures on branch openings for the NBFCs. GE Consumer Finance is a section of General Electric. It is responsible for looking after the retail finance operations. GE Consumer Finance also governs the GE Capital Asia. Outside the United States, GE Consumer Finance performs its operations under the GE Money brand. GE Consumer Finance currently offers financial services in more than fifty countries. The company deals in credit cards, personal finance, mortgages and automobile solutions. It has a client base of more than 118 million customers throughout the world

建筑工程及给排水专业中英文对照翻译

Laminar and Turbulent Flow Observation shows that two entirely different types of fluid flow exist. This was demon- strated by Osborne Reynolds in 1883 through an experiment in which water was discharged from a tank through a glass tube. The rate of flow could be controlled by a valve at the outlet, and a fine filament of dye injected at the entrance to the tube. At low velocities, it was found that the dye filament remained intact throughout the length of the tube, showing that the particles of water moved in parallel lines. This type of flow is known as laminar, viscous or streamline, the particles of fluid moving in an orderly manner and retaining the same relative positions in successive cross- sections. As the velocity in the tube was increased by opening the outlet valve, a point was eventually reached at which the dye filament at first began to oscillate and then broke up so that the colour was diffused over the whole cross-section, showing that the particles of fluid no longer moved in an orderly manner but occupied different relative position in successive cross-sections. This type of flow is known as turbulent and is characterized by continuous small fluctuations in the magnitude and direction of the velocity of the fluid particles, which are accompanied by corresponding small fluctuations of pressure. When the motion of a fluid particle in a stream is disturbed, its inertia

英文翻译(原文)

GRA VITY RETAINING?WALL 1. INTRODUCTION Retaining walls are structures used to provide stability for earth or other material where conditions disallow the mass to assume its natural slope, and are commonly used to hold back or support soilbanks,coal or ore piles, and water. Retaining walls are classified, based on the method of achieving stability, into six principal types (Fig.1). The gravity-wall depends upon its weight, as the name implies, for stability. The cantilever wall is a reinforced-concrete wall that utilizes cantilever action to retain the mass behind the wall from assuming a natural slope. Stability of this wall is partially achieved from the weight of soil on the heel portion of the base slab. A counterfort retaining wall is similar to a cantilever retaining wall, except that it is used where the cantilever is long or for very high pressures behind wall and has counterforts, which tie the wall and base together, built at intervals along the wall to reduce the bending moments and sheers. As indicated in Fig.1c, the counterfort is behind the wall and subjected to tensile forces. A buttressed retaining wall is similar to a counterfort wall, except that the bracing is in front of the wall and is in compression instead of tension. Two other types of walls not considered further are crib walls, which are built-up members of pieces of precast concrete, metal, or timber and are supported by anchor pieces embedded in the soil for stability, and semigravity walls, which are walls intermediate between a true gravity and a cantilever wall. (a)(b)(e)

英语原文及翻译

高速视频处理系统中的信号完整性分析 摘要:结合高速DSP图像处理系统讨论了高速数字电路中的信号完整性问题,分析了系统中信号反射、串扰、地弹等现象破坏信号完整性的原因,通过先进IS工具的辅助设计,找出了确保系统信号完整性的具体方法。 关键词:高速电路设计信号完整性 DSP系统 深亚微米工艺在IC设计中的使用使得芯片的集成规模更大、体积越来越小、引脚数越来越多;由于近年来IC工艺的发展,使得其速度越来越高。从而,使得信号完整性问题引起电子设计者广泛关注。 在视频处理系统中,多维并行输入输出信号的频率一般都在百兆赫兹以上,而且对时序的要求也非常严格。本文以DSP图像处理系统为背景,对信号完整性进行准确的理论分析,对信号完整性涉及的典型问题[1]——不确定状态、传输线效应、反射、串扰、地弹等进行深入研究,并且从实际系统入手,利用IS仿真软件寻找有效的途径,解决系统的信号完整性问题。 1 系统简介 为了提高算法效率,实时处理图像信息,本图像处理系统是基于DSP+FPGA结构设计的。系统由SAA7111A视频解码器、TI公司的TMS320C6701 DSP、Altera公司的EPlK50QC208 FPGA、PCI9054 PCI接口控制器以及SBRAM、SDRAM、FIFO、FLASH等构成。FPGA是整个系统的时序控制中心和数据交换的桥梁,而且能够对图像数据实现快速底层处理。DSP是整个系统实时处理高级算法的核心器件。系统结构框图如图1所示。 在整个系统中,PCB电路板的面积仅为15cm×l5cm,系统时钟频率高达167MHz,时钟沿时间为0.6ns。由于系统具有快斜率瞬变和极高的工作频率以及很大的电路密度,使得如何处理高速信号问题成为一个制约设计成功的关键因素。 2 系统中信号完整性问题及解决方案 2.1 信号完整性问题产生机理 信号的完整性是指信号通过物理电路传输后,信号接收端看到的波形与信号发送端发送的波形在容许的误差范围内保持一致,并且空间邻近的传输信号间的相互影响也在容许的范围之内。因此,信号完整性分析的主要目标是保证高速数字信号可靠的传输。实际信号总是存在电压的波动,如图2所示。在A、B两点由于过冲和振铃[2]的存在使信号振幅落入阴影部分的不确定区,可能会导致错误的逻辑电平发生。总线信号传输的情况更加复杂,任何一个信号发生相位上的超前或滞后都可能使总线上数据出错,如图3所示。图中,CLK为时钟信号,D0、D1、D2、D3是数据总线上的信号,系统允许信号最大的建立时间[1]为△t。在正常情况下,D0、D1、D2、D3信号建立时间△t1<△t,在△t时刻之后数据总线的数据已稳定,系统可以从总线上采样到正确的数据,如图3(a)所示。相反,当信号D1、D2、D3受过冲和振铃等信号完整问题干扰时,总线信号就发生

水文与水资源专业英语文章翻译

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如果你已经看到了这里,那么说明你应该是英文爱好者哦。 下面有一些非常实用,我精心整理的英文资料,你一定用得到!快去看看吧! 一,最常用英语翻译政治文体句型总结大全完美版 二,英文合同翻译最常用句型总结专业版 三,英语毕业论文提纲模板优秀完整详细无敌版

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