120 resultados para MSC Diagram


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The dynamic behaviour for nanoscale electrostatic actuators is studied. A two Parameter mass-spring model is shown to exhibit a bifurcation from the case excluding an equilibrium point to the case including two equilibrium points as the geometrical dimensions of the device are altered. Stability analysis shows that one is a stable Hopf bifurcation point and the other is an unstable saddle point. In addition, we plot the diagram phases, which have periodic orbits around the Hopf point and a homoclinic orbit passing though the unstable saddle point.

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针对固体火箭发动机柔性接头中的橡胶材料,研究了在进行这种橡胶结构有限元计算中橡胶材料的力学行为的表征。进行了单轴拉伸与简单剪切材料力学性能试验,根据不同材料模型对试验曲线进行了拟合,并用MSC/Marc软件模拟了超弹性材料的单轴拉伸与简单剪切变形过程。结果表明:采用单轴拉伸试验数据预测材料剪切性能会造成明显误差,而简单剪切试验得到的模型可以比较准确描述材料的拉伸和剪切变形,针对柔性接头这种以剪切变形为主的结构,应选取剪切试验数据;当应变大于150%时,不同材料模型与试验数据的选用范围对计算结果具有明显影响。

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A linear stability analysis is applied to determine the onset of oscillatory thermocapillary convection in cylindrical liquid bridges of large Prandtl numbers (4 <= Pr <= 50). We focus on the relationships between the critical Reynolds number Re-c, the azimuthal wave number m, the aspect ratio F and the Prandtl number Pr. A detailed Re-c-Pr stability diagram is given for liquid bridges with various Gamma. In the region of Pr > 1, which has been less studied previously and where Re, has been usually believed to decrease with the increase of Pr, we found Re-c exhibits an early increase for liquid bridges with Gamma around one. From the computed surface temperature gradient, it is concluded that the boundary layers developed at both solid ends of liquid bridges strengthen the stability of basic axisymmetric thermocapillary convection at large Prandtl number, and that the stability property of the basic flow is determined by the "effective" part of liquid bridge. (c) 2008 Published by Elsevier Ltd on behalf of COSPAR.

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Three types of streamline topology in a Karman vortex street flow are shown under the variation of spatial parameters. For the motion of dilute particles in the Karman vortex street flow, there exist a route of bifurcation to a chaotic orbit and more attractors in a bifurcation diagram for the proportion of particle density to fluid density. Along with the increase of spatial parameters in the flow field, the bifurcation process is suspended, as well as more and more attractors emerge. In the motion of dilute particles, a drag term and gravity term dominate and result in the bifurcation phenomenon.

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In the present paper, we endeavor to accomplish a diagram, which demarcates the validity ranges for interfacial wave theories in a two-layer system, to meet the needs of design in ocean engineering. On the basis of the available solutions of periodic and solitary waves, we propose a guideline as principle to identify the validity regions of the interfacial wave theories in terms of wave period T, wave height H, upper layer thickness d(1), and lower layer thickness d(2), instead of only one parameter-water depth d as in the water surface wave circumstance. The diagram proposed here happens to be Le Mehautes plot for free surface waves if water depth ratio r = d(1)/d(2) approaches to infinity and the upper layer water density rho(1) to zero. On the contrary, the diagram for water surface waves can be used for two-layer interfacial waves if gravity acceleration g in it is replaced by the reduced gravity defined in this study under the condition of sigma = (rho(2) - rho(1))/rho(2) -> 1.0 and r > 1.0. In the end, several figures of the validity ranges for various interfacial wave theories in the two-layer fluid are given and compared with the results for surface waves.

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Flow fields around a rotating circular cylinder in a uniform stream are computed using a low dimensional Galerkin method. Results show that the formation of a Fopple vortex pair behind a stationary circular cylinder is caused by the structural instability in the vicinity of the saddle located at the rear of the cylinder. For rotating cylinder a bifurcation diagram with the consideration of two parameters, Reynolds number Re and rotation parameter a, is built by a kinematic analysis of the steady flow fields.

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采用MSC.Marc非线性有限元软件,对薄板激光变曲过程中的温度场进行了数值模拟,得到了引起薄板激光弯曲形的温度场的变化规律。通过温度传感器测量与激光扫描线相对应的薄板下表面温度变化的规律来验证数值模拟的结果。模拟值与实测值基本吻合,表明数值模拟结果可作为激光加工工艺参数选择的依据。

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采用MSC.Marc非线性有限元软件,对试件在激光点热源作用下动态微变形过程进行了数值模拟。通过激光反射放大系统测量了试件在激光点热源作用下的动态微变形过程。模拟值与实测值的结果表明:热应力和相变应力的共同作用使得试件产生微变形,最终试件的变形方向取决于热应变和相变共同作用的结果,朝向激光束或背向激光束。比较实验值和模拟值,发现变形的最大值相近,变形过程却略有不同。考虑到激光点热源作用下有限厚度的试件内,温度场分布出现的反常效应,即内部的温度大于边界温度,提出采用波动理论修正经典的热传导计算模型,可望有效地提高模拟过程的计算精度。结论为进一步研究薄板激光弯曲的变形机理及变形过程莫定了基础。

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利用MSC.Dytran中的具有强度的多材料欧拉网格模拟水滴和有限长连续射流对靶板(岩石)的高速冲击作用,研究了靶板破坏深度、破坏宽度与水滴初压力、速度、入射方向、板厚以及连续射流的密度等的关系及其物理意义.用应力波理论来解释靶板的层裂现象,试图多角度分析射流破岩机理.

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采用MSC.Mare非线性有限元软件,对激光强化过程中的温度场进行数值模拟,分析了能量密度的变化对激光强化效果的影响。通过温度传感器测量激光强化时材料表面温度的变化来验证数值模拟的结果。模拟值与实测值基本吻合。结果表明,数值模拟结果可作为激光加II艺参数选择的依据。

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根据转动壳体的动力学方程,在利用DMAP对大型有限元软件MSC/NASTRAN二次开发的基础上,呆用有限元方法对复合材料层合壳体转动状态下的动力特性进行了研究,分析了科氏力、离心力和横向剪力对固有频率的影响,并与实验结果进行了比较.结果显示由于科氏力的作用,即使在动坐标系下,层合壳体也会出现频率不等的前后行波,横向剪力使壳体的固有频率降低,且随着壳体厚径比的增加其影响显著增加.

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Fuzzy reliability methods are used to study the corrosion of pipelines. Three methods are used. They consist of using fracture failure modes, failure assessment diagram (FAD) and residual strength for establishing fuzzy reliability. Calculations are made by application of JC, improved GA-JC and Mente-carlo methods. Examples for oilfield injecting water pipeline show the residual strength well agree with field data. Mente-carlo methods appear to yield results that have better agreement with field data.

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采用MSC.Marc非线性有限元软件,对板料激光弯曲过程进行了数值模拟.试验与数值模拟的相互印证表明:数值模拟的模型正确,计算过程可靠,计算结果可为板料激光弯曲工艺参数的选择提供依据.通过模拟多道次直线照射的过程可知,变形效果受照射路径次序的影响很大,应选择从固定端向自由端方向交替的双向照射路径,以保证板料在宽度方向上变形的均匀.模拟结果可为带筋结构壁板激光弯曲成形提供实用方案.

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采用三种不同的双光记录方案进行了LiNbO3:Fe:Ni晶体全息存储实验.详细研究了饱和衍射效率、固定衍射效率、动态范围和记录灵敏度,以及退火条件对记录的影响。结果表明,氧化LiNbO3:Fe:Ni晶体的饱和衍射效率、固定衍射效率和记录灵敏度比其他报道的双掺杂LiNbO3晶体高。结合掺杂能级图,理论分析了LiNbO3双掺杂晶体深陷阱中心能级的相对位置及其微观光学参量对全息记录性能的影响。LiNbO3:Fe:Ni晶体有望成为一种新的高效率非挥发全息存储材料。

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The near-IR emission spectra of Er3+-Tm3+ codoped 70GeS(2)-20In(2)S(3)-10CsI chalcohalide glasses were studied with an 808 nm laser as an excitation source. A broad emission extending from 1.35 to 1.7 mu m with a FWHM of similar to 160 nm was recorded in a 0.1 mol.% Er2S3, 0.5 mol.% Tm2S3 codoped chalcohalide glass. The fluorescence decay curves of glasses were measured by monitoring the emissions of Tm3+ at 1460 nm and Er3+ at 1540 nm, and the lifetimes were obtained from the first-order exponential fit. The luminescence mechanism and the possible energy-transfer processes are discussed with respect to the energy-level diagram of Er3+ and Tm3+ ions. (C) 2008 Optical Society of America