23 resultados para Aguarelas (1926)

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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A new phenomenological deformation theory with strain gradient effects is proposed. This theory, which belongs to nonlinear elasticity, fits within the framework of general couple stress theory and involves a single material length scale l. In the present theory three rotational degrees of freedom omega(i) are introduced in addition to the conventional three translational degrees of freedom u(i). omega(i) has no direct dependence upon ui and is called the micro-rotation, i.e. the material rotation theta(i) plus the particle relative rotation. The strain energy density is assumed to only be a function of the strain tensor and the overall curvature tensor, which results in symmetric Cauchy stresses. Minimum potential principle is developed for the strain gradient deformation theory version. In the limit of vanishing 1, it reduces to the conventional counterparts: J(2) deformation theory. Equilibrium equations, constitutive relations and boundary conditions are given in details. Comparisons between the present theory and the theory proposed by Shizawa and Zbib (Shizawa, K., Zbib, H.M., 1999. A thermodynamical theory gradient elastoplasticity with dislocation density Censor: fundamentals. Int. J. Plast. 15, 899) are given. With the same hardening law as Fleck et al. (Fleck, N.A., Muller, G.H., Ashby, M.F., Hutchinson, JW., 1994 Strain gradient plasticity: theory and experiment. Acta Metall. Mater 42, 475), the new strain gradient deformation theory is used to investigate two typical examples, i.e. thin metallic wire torsion and ultra-thin metallic beam bend. The results are compared with those given by Fleck et al, 1994 and Stolken and Evans (Stolken, J.S., Evans, A.G., 1998. A microbend test method for measuring the plasticity length scale. Acta Mater. 46, 5109). In addition, it is explained for a unit cell that the overall curvature tensor produced by the overall rotation vector is the work conjugate of the overall couple stress tensor. (C) 2002 Elsevier Science Ltd. All rights reserved.

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An investigation has been made into the effect of microstructural parameters on the propensity for forming shear localization produced during high speed torsional testing by split Hopkinson bar with different average rates of 610, 650 and 1500 s(-1) in low carbon steels. These steels received the quenched, quenched and tempered as well as normalized treatments that provide wide microstructural parameters and mechanical properties. The results indicate that the occurrence of the shear localization is susceptible to the strength of the steels. In other words, the tendency of the quenched steel to form a shear band is higher than that of the other two steels. It is also found that there is a critical strain at which the shear localization occurs in the steels. The critical strain value is strongly dependent on the strength of the steels. Before arriving at this point, the material undergoes a slow work-hardening. After this point, the material suffers work-softening, corresponding to a process during which the deformation is gradually localized and eventually becomes spatially correlated to form a macroscopic shear band. Examinations by SEM reveal that the shear localization within the band involves a series of sequential crystallographic and non-crystallographic events including the change in crystal orientation, misorientation, generation and even perhaps damage in microstructures such as the initiation, growth and coalescence of the microcracks. It is expected that the sharp drop in the load-carrying capacity is associated with the growth and coalescence of the microcracks rather than the occurrence of the shear localization, but the shear localization is seen to accelerate the growth and coalescence of the microcracks. The thin foil observations by TEM reveal that the density of dislocations in the band is extremely high and the tangled arrangement and cell structure of dislocations tends to align along the shear direction. The multiplication and interaction of dislocations seems to be responsible for work-hardening of the steels. The avalanche of the dislocation cells corresponds to the sharp drop in shear stress at which the deformed specimen is broken. Double shear bands and kink bands are also observed in the present study. The principal band develops first and its width is narrower than that of the secondary band.

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自从1926年Chanman和Wheeler率先开创有障碍物管道中的火焰传播研究工作以来,管道中障碍物扰动引起的火焰加速现象引起了广泛的关注。由于这类现象在燃烧科学上的学术意义及其在生产中诸如安全问题等方面的实际意义,人们相继进行了一系列的研究工作。归纳起来,可以分为两大类:1)封闭管道的火焰传播。人们在不同形状的管道或容器中研究了障碍物对火焰加速的影响,在理论分析和数值计算方面也作了一些有益的工作;2)开口管道的火焰传播。相对于闭口管道,开口管道中的火焰传播研究则逊色得多。这方面尚缺乏系统的实验数据,理论方面的分析也欠缺得多。但当前在实际中,并不乏开口体系的应用,如,现已广泛应用于电力系统的一种燃气除灰装置,是一燃烧气体燃料的半开口系统。因此,研究半开口管道中非稳态燃烧的加速机制具有重要意义。在本论文工作中,通过大量的实验研究,比较系统地研究了障碍物的扰动对预混火焰传播特性的影响。实验在一长L=5m、内径D=80mm的一端封闭、一端开口的火焰传播管内进行,管内均匀布置障碍物,通过改变障碍物的形状、间距、阻塞比大小,同时选用五种不同的可燃气体,探索了障碍物结构对预混湍流火焰加速和管内压力上升的影响。实验表明,对于敏感气体如氢气和乙炔,由于障碍物扰动产生的影响,火焰不断加速,并最终达到一准稳定状态;在适当的条件下,火焰传播状态可由爆燃向爆轰转变,此时火焰速度发生跃变;而对干不敏感气体如甲烷,则爆燃转爆轰现象不容易发生。在不同的火焰传播状态,障碍物结构特性对火焰速度和压力产生的影响各不相同。在缓燃态,随着阻塞比的变化,最大火焰速度先上升后下降,在BR=0.3~0.4之间存在一最大值;在銮塞态,最大火焰速度受阻塞比变化的影响不明显,略低于燃烧产物的声速;在阻塞比BR=0.5附近,压力达到最大值。而在爆轰态,随着阻塞比的增加,最大火焰速度和压力逐渐降低,爆燃转爆轰的浓度范围变小。由于在有障碍物的管道中,火焰速度很容易达到声速(变塞态)或超声速(爆轰态),必须考虑流体的马赫数效应。本文在前人研究成果的基础上,给出了湍流马赫数修正的可压缩性两方程湍流模型,模拟了半开口狭长管道中重复布置的障碍物引起的湍流火焰加速现象。最大火焰速度和管内压力的计算结果与实验测量值吻合良好,这表明用修正后的湍流模型能够比较真实地模拟障碍物管内预混火焰的发展过程。通过对管道内障碍物扰动引起的燃烧波加速的机理和技术研究,对流场扰动对燃烧波产生和发展的影响规律有了比较全面的了解,研究结果对气脉冲除灰技术的完善具有直接的指导意义。

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High-order harmonics and single attosecond pulse generation by using an infrared laser pulse combined with attosecond pulse trains (APT) interacting with He+ have been investigated. We show that the ionization for different instant time intervals can be controlled by altering the time delay between the APT and the infrared pulse. Consequently, APT can be used as a tool to control the efficiency of high-order harmonics emitted at different times. By choosing appropriate APT and time delay, the driving pulse width for single attosecond pulse generation can be extended up to six optical cycles. (c) 2007 Optical Society of America.

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用Ansys软件模拟了大功率半导体激光器阵列的稳态温度分布,并对自行研制的半导体激光器阵列的温度变化进行了测试,结果表明理论计算与实验结果基本吻合。该模拟结果对大功率半导体激光器阵列的封装设计具有现实的指导意义。

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树鼩是一种新开发的小型实验动物. 研究树鼩的寄生虫对保护树鼩群体, 保证准确的实验结果, 以及寻找人类疾病的动物模型等方面都有着重要的实用意义和理论意义. 关于缅甸、越南、婆罗洲、马来西亚、马来亚、印度、和印度尼西亚树鼩的体内外寄生虫研究, 国外学者已作过许多研究(Dunn, 1963, 1964; Van Peenen等, 1967;Durette-Desset等, 1975, 1981; File, 1974; Quentin等, 1975, 1977; Chabaud等, 1975;Ohbayashi等, 1983; Betteron等, 1977; Betterton, 1979, 1980; Myers, 1960; Orihel, 1966; Nandi, 1982; Manning等, 1972; Mallin等, 1972; Schmidt等, 1977; Houdemer, 1938; Heyneman 等, 1965; Jordan,1926; Durden 等, 1984)。

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在渔业资源和可养殖水面有限的情况下,必然要在水产养殖上寻求渔业的可持续发展,如增加养殖密度,提高单位水体产量。养殖密度的增加,对养殖系统及排放废水的附近水域都会产生负面影响。由于鱼类排泄物和残饵直接进入水体,导致氨氮浓度升高,已成为制约鱼类生产、造成水体富营养化的主要环境因素。对治理氨氮污染这一世界性的课题,笔者就去除养殖水体氨氮的微生物种群、固定化技术、生物强化技术以及人工湿地生态工程技术等做一综述,以期把握研究热点,推进水产养殖的可持续发展。

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研究了盐泽螺旋藻的形态、生理生化特性和在不同条件下的生长状况,并与其他螺旋藻进行了比较。盐泽螺旋藻、极大螺旋藻和钝顶螺旋藻在蛋白质的含量、氨基酸组分以及可见光吸收光谱等方面差别不大。盐泽螺旋藻的生长速度最快(世代时间为8.4h)。极大螺旋藻、钝顶螺旋藻1926和钝顶螺旋藻2340的世代时间分别为11、11.8和14.8h。盐泽螺旋藻的光合作用和呼吸作用强度亦大于极大螺旋藻和钝顶螺旋藻。此外,这种藻对盐分和温度还具有较宽的适应范围,在形态上也和其他3种螺旋藻有较大之差异。

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水印检测是数字水印技术的一个关键步骤,但是目前所提出的绝大多数水印检测算法既不具备赖以支撑的理论基础,其检测性能也不是优化的.利用数字水印的不可感知特性,应用弱信号检测理论进行水印检测的研究.首先从图像小波变换系数的统计特性出发,利用广义高斯分布(GGD)来建立小波细节子带系数的统计分布模型;然后针对水印嵌入强度未知的情况,将水印检测问题转化为非高斯噪声中具有未知参数的确定性信号的检测,在弱信号条件下提出一种离散小波变换(DWT)域图像水印的优化盲检测算法.检测性能分析表明,该检测算法能够实现恒虚警率水印检测.实验结果验证了检测性能理论分析的有效性和实际性能的优越性.

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将前向安全的概念引入到基于双线性映射的门限签名方案中,提出了一个基于双线性映射的前向安全的门限签名方案.该方案将签名密钥分散到签名成员集合中,采用各成员部分密钥前向更新的方式实现了签名密钥的前向更新,增强了签名密钥的安全性,使得签名方案具有前向安全性.另外,由于部分密钥具有前向更新的特性,从而方案有效防止了移动攻击.对该方案的安全性进行了分析,分析表明,该方案是安全、有效的.

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一、前言海洋热能转换(Ocean Thermal Energy Conversion OTEC)这一概念早在1881年法国物理学家 D~1 Arsonval 就提出来了。他设想在热带海洋表面温海水与深层冷海水之间,设置闭式朗肯循环,把海洋中所储存的太阳热能转换为电能。为实现这一设想,D~1Arsonval 的学生,法国工程师 G.Claude 于1926年在一个海水温差发电的模拟装置上使

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By extending our microscopic model on optical-phonon modes in quantum wells to one-dimensional (1D) quantum-well wires (QWW), the optical displacements and associated electrostatic potentials of optical-phonon modes in 1D QWW are calculated. The modes can be clearly divided into confined LO bulklike, TO bulklike modes, and extended interfacelike modes provided the bulk phonon dispersion is ignored. The character of each type of mode is illustrated with special attention to the interfacelike modes, which are hybrids of longitudinal- and transverse-optical waves from the corresponding bulk materials. Based on the numerical results, approximate analytical formulas for bulklike modes are presented. As in 2D wells, both the optical displacements and Frohlich potentials for the bulklike modes vanish at the interfaces. The finite dispersion of bulk phonons has a more pronounced effect on the 1D phonon modes because interfacelike modes show mixed characteristics of 2D interface and bulklike modes.

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利用电化学沉积方法在重离子径迹模板中制备出直径从45nm到200nm,长径比达700的金纳米线阵列,利用扫描电子显微镜(SEM)和X射线衍射(XRD)对所制备金纳米线的形貌及晶体结构进行分析,结果表明,在1.5V(无参比电极)沉积电压下所制备出的直径为200nm金纳米线沿[100]晶向具有较好择优取向.利用紫外-可见光谱(UV-Vis)对镶嵌在透明模板中平行排列的金纳米线阵列光学特性进行研究,发现金纳米线直径为45nm时,其紫外可见光谱在539nm处有强烈吸收峰,随着金纳米线直径增加,吸收峰红移,当金纳米线直径达到200nm时,其吸收峰峰位移至700nm.结合金纳米颗粒相关表面等离子体共振吸收效应对实验结果进行了讨论.