轴拉杆随机分析的域外奇点法

采用随机域外奇点法对轴拉杆件进行了分析．考虑杨氏模量的不确定性，得到了不同相关类型、不同相关长度下的解析解，并分析了相关类型、相关长度以及随机场中点离散法对位移方差的影响．     

气体催化裂解法制备高纯碳纳米管的研究

利用有机气体化学裂解技术 ,用二甲苯作碳源 ,二茂铁作催化剂 ,噻吩作助长剂 ,氢气作载气 ,对碳纳米管的制备进行了研究 .研究结果表明 ,二甲苯流量、氢气流量及有机气体裂解温度等工艺参数对碳纳米管的产量及形态有很大的影响 ;在反应温度为 10 0 0～ 110 0℃ ,氢气流量为 15 0mL·min- 1,二甲苯的流量为 0 .12 1mL·min- 1时 ,能获得直径为 4 0～ 10 0nm的碳纳米管 ,碳纳米管的纯度可达 95 %以上 .     

4ФFDPSK高频调制解调器的MAP准则同步方案

本文提出了利用MAP准则实现短波数字调制、解调器的同步方案,导出了提取同步信息的表达式。最后,对此方案进行了计算机模拟,根据模拟结果对方案的性能进行了分析。从理论上实践上证实了方案的可行性。     

成本在心中效益在手中--山西汾西矿业(集团)水峪煤矿有限责任公司成本管理浅析

从材料的消耗，电力的消耗，管理费用的控制3个方面阐述了成功的成本管理给企业带来的经济效益，指出降低成本是企业力求发展的重要途径，管理是企业永恒的主题。     

Fibulin-5/DANCE is essential for elastogenesis in vivo.

The elastic fibre system has a principal role in the structure and function of various types of organs that require elasticity, such as large arteries, lung and skin. Although elastic fibres are known to be composed of microfibril proteins (for example, fibrillins and latent transforming growth factor (TGF)-beta-binding proteins) and polymerized elastin, the mechanism of their assembly and development is not well understood. Here we report that fibulin-5 (also known as DANCE), a recently discovered integrin ligand, is an essential determinant of elastic fibre organization. fibulin-5-/- mice generated by gene targeting exhibit a severely disorganized elastic fibre system throughout the body. fibulin-5-/- mice survive to adulthood, but have a tortuous aorta with loss of compliance, severe emphysema, and loose skin (cutis laxa). These tissues contain fragmented elastin without an increase of elastase activity, indicating defective development of elastic fibres. Fibulin-5 interacts directly with elastic fibres in vitro, and serves as a ligand for cell surface integrins alphavbeta3, alphavbeta5 and alpha9beta1 through its amino-terminal domain. Thus, fibulin-5 may provide anchorage of elastic fibres to cells, thereby acting to stabilize and organize elastic fibres in the skin, lung and vasculature.     

Ruin Probability with Variable Premium Rate and Disturbed by Diffusion in a Markovian Environment

We consider a risk model with a premium rate which varies with the level of free reserves. In this model, the occurrence of claims is described by a Cox process with Markov intensity process, and the influence of stochastic factors is considered by adding a diffusion process. The integro-differential equation for the ruin probability is derived by a infinitesimal method.     

Newton's Easy Quadratures ``Omitted for the Sake of Brevity'

In the 1687 Principia, Newton gave a solution to the direct problem (given the orbit and center of force, find the central force) for a conic-section with a focal center of force (answer: a reciprocal square force) and for a spiral orbit with a polar center of force (answer: a reciprocal cube force). He did not, however, give solutions for the two corresponding inverse problems (given the force and center of force, find the orbit). He gave a cryptic solution to the inverse problem of a reciprocal cube force, but offered no solution for the reciprocal square force. Some take this omission as an indication that Newton could not solve the reciprocal square, for, they ask, why else would he not select this important problem? Others claim that ``it is child's play' for him, as evidenced by his 1671 catalogue of quadratures (tables of integrals). The answer to that question is obscured for all who attempt to work through Newton's published solution of the reciprocal cube force because it is done in the synthetic geometric style of the 1687 Principia rather than in the analytic algebraic style that Newton employed until 1671. In response to a request from David Gregory in 1694, however, Newton produced an analytic version of the body of the proof, but one which still had a geometric conclusion. Newton's charge is to find both ``the orbit' and ``the time in orbit.' In the determination of the dependence of the time on orbital position, t(r), Newton evaluated an integral of the form ∫dx/x <sup>n</sup> to calculate a finite algebraic equation for the area swept out as a function of the radius, but he did not write out the analytic expression for time t = t(r), even though he knew that the time t is proportional to that area. In the determination of the orbit, θ (r), Newton obtained an integral of the form ∫dx/√(1−x<sup>2</sup>) for the area that is proportional to the angle θ, an integral he had shown in his 1669 On Analysis by Infinite Equations to be equal to the arcsin(x). Since the solution must therefore contain a transcendental function, he knew that a finite algebraic solution for θ=θ(r) did not exist for ``the orbit' as it had for ``the time in orbit.' In contrast to these two solutions for the inverse cube force, however, it is not possible in the inverse square solution to generate a finite algebraic expression for either ``the orbit' or ``the time in orbit.' In fact, in Lemma 28, Newton offers a demonstration that the area of an ellipse cannot be given by a finite equation. I claim that the limitation of Lemma 28 forces Newton to reject the inverse square force as an example and to choose instead the reciprocal cube force as his example in Proposition 41. (Received August 14, 2002) Published online March 26, 2003 Communicated by G. Smith     

英汉交际语差异及其原因初探

文章就日常生活中一些较为典型的交际情景，对英汉交际语的差异及其潜在原因作了探讨。