共查询到18条相似文献,搜索用时 46 毫秒
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在空气动力学、水动力学和生物流体力学领域中,大变形柔性结构的流固耦合现象是一个重要的非线性力学问题.对该系统的数值模拟是分析这一问题的有效手段.将近年提出的一种Descartes流场求解器,即浸润边界-格子Boltzmann通量求解器(immersed boundary-lattice Boltzmann flux solver,IB-LBFS)作为流场求解方法,并引入绝对节点坐标法(absolute nodal coordinate formulation,ANCF)作为大变形结构分析手段,构建了流固耦合求解器以模拟三维流场中的大变形柔性体运动.使用三维来流中的旗帜摆动算例对该流固耦合求解器进行了验证计算.基于该流固耦合求解器对三维不可压流场中的矩形降落伞和十字形降落伞的展开过程进行了非定常流固耦合数值模拟. 相似文献
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具有大范围运动和非线性变形的空间柔性梁的精确动力学建模 总被引:1,自引:0,他引:1
研究具有大范围运动和非线性变形的空间柔性梁的有限元动力学建模.首先在精确描述空间柔性梁的非线性变形的基础上,采用有限元方法对梁结构进行离散,导出其动能、势能及外力对应的广义力,然后利用Lagrange方程建立了空间柔性梁的精确动力学方程.该方程在原有一次耦合模型的基础上,增加了新的表征纵向、横向、侧向弯曲变形,以及扭转变形的耦合项,同时包含了变形运动与大范围运动之间的相互耦合项.本建模方法和所得结论可为以后空间柔性梁的动力学特性分析作以参考. 相似文献
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针对平面干涉检测技术的检测精度受限于参考面面形精度的问题,提出使用基于奇偶函数的高精度绝对检测方法消除干涉系统中参考面面形误差的影响。对旋转角度误差与旋转偏心误差对绝对检测方法测量精度的影响进行了仿真分析。利用商用菲索干涉仪,设计和分析了绝对检测精度实验及重复性实验。仿真结果显示:旋转角度误差在达到0.13°时,测量误差PV值为0.000 1λ;旋转偏心误差达到3 pixel时,测量误差PV值为0.005λ。实验结果显示:测得实际样品的绝对检测精度PV10值为0.041 5 λ,RMS值为0.008 7 λ,小于常规干涉检测所得结果;对同一平面两次独立的绝对检测结果进行点对点作差处理,从而获得残差图,其残差图PV10值为0.004 λRMS值为0.000 5 λ。实验结果表明了该方法的高重复性和有效性。 相似文献
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对二维剪切梁单元进行研究,利用平面旋转场理论推导了精确曲率模型.采用几何精确梁理论构建了剪切梁单元弹性力矩阵.通过绝对节点坐标方法建立了系统的非线性动力学方程,提出基于旋转场曲率的二维剪切梁单元,并分别引入经典二维剪切梁单元和基于位移场曲率的二维剪切梁单元进行比较研究.首先,静力学分析证明了所提模型的正确性;其次,特征频率分析验证了模型可与理论解符合,收敛精度高,并且能准确地预测单元固有频率对应的振型;最后,在非线性动力学问题上,通过与ANSYS结果对比分析,证明了该模型可有效处理柔性大变形问题,并且与经典二维剪切梁单元相比具有缓解剪切闭锁的优势.因此,本文提出的基于旋转场曲率的二维剪切梁单元在处理几何非线性问题中具有较大的应用潜力. 相似文献
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数字图像相关中基于可靠变形初值估计的大变形测量 总被引:7,自引:0,他引:7
为使数字图像相关方法适用于大变形测量,提出一种变形初值估计方法.通过在变形前图像中第一个计算点附近选择三个或更多特征点并在变形后图像中选择其对应点,利用坐标对应关系获得该点可靠的变形估计值作为Newton-Rapshon方法的迭代初值.该方法可对被测物体存在任意刚体转动或大变形情况下的表面变形进行准确测量,克服了通常的基于整像素位移相关搜索再进行亚像素位移测量的数字图像相关方法在被测物面存在稍大转角或大变形情况下即不能使用的缺点.对存在相对刚体转动图像的位移场和聚丙烯泡沫塑料压缩实验的大变形进行了测量,结果充分显示本文方法的有效性. 相似文献
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The spaces of tensor densities over a manifold M are modules over the Lie algebra Vect(M) of vector fields over the manifold. When M is a contact manifold, one can consider the algebra C(M) of vector fields which preserves the contact structure. If the manifold is endowed with a contact projective structure, there is an embedding of the linear symplectic algebra sp(2n+2, ) in C(M). In this Letter, we determine the C(M)- and the sp(2n+2, )-invariant bidifferential operators on tensor densities. 相似文献
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This paper obtains Lagrange equations of nonholonomic systems with fractional derivatives. First, the exchanging relationships between the isochronous variation and the fractional derivatives are derived. Secondly, based on these exchanging relationships, the Hamilton's principle is presented for non-conservative systems with fractional derivatives. Thirdly, Lagrange equations of the systems are obtained. Furthermore, the d'Alembert–Lagrange principle with fractional derivatives is presented,and the Lagrange equations of nonholonomic systems with fractional derivatives are studied. An example is designed to illustrate these results. 相似文献
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Susumu Onaka 《哲学杂志》2013,93(18):2264-2271
Onaka has shown (2010) that the Hencky equivalent strain is the appropriate quantity to represent the degree of severe plastic deformation based on simple-shear deformation. In a recent paper, Shrivastava et al. have criticized (2011) the Onaka paper and stated that the Hencky formulation does not apply to large simple-shear deformation. In this response, it is shown that this claim of Shrivastava et al. is not consistent with recent accepted knowledge on the Hencky strain. 相似文献
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本文将地球介质看作是弹性介质, 从弹性体的Navier方程出发, 建立均匀弹性介质和非均匀弹性介质的分析动力学方程——Lagrange方程, 利用弹性介质的Lagrange方程导出匀弹性介质和非均匀弹性介质的地震波方程, 为用Lagrange分析动力学研究地球介质中地震波传播规律和解决地震勘探中的有关问题提供基础.关键词:地震勘探弹性介质Lagrange 方程地震波方程 相似文献
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We present a spring-defect model in 3-dimensions to describe the connection between elastic distortion and interstitial carbon
ordering associated with phase transition from a body centred cubic (BCC) to body centered tetragonal (BCT) structure in BCC
metals such as α-iron. The presence or the absence of the carbon is modelled in terms of a pseudo spinŝ=+1or -l.An Ising interaction between carbon atoms is recovered after eliminating the lattice degrees of freedom, which is
longranged. The coupling between the spin and lattice degrees of freedom allows for a systematic study of ferroelasticity
and the variation of the lattice parameter with carbon concentration. The mean field results for the paraelastic to ferroelastic
transition, lattice parameter and static compliance are presented. The significant feature of this calculation is not only
a derivation of the defect-defect interaction, but also an explicit calculation of the strain dipole tensor associated with
each defect, from a microscopic model. 相似文献
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A single particle obeys the Dirac equation in spatial dimensions and is bound by an attractive central monotone potential that vanishes at infinity. In one dimension, the potential is even, and monotone for The asymptotic behavior of the wave functions near the origin and at infinity are discussed. Nodal theorems are proven for the cases and , which specify the relationship between the numbers of nodes n1 and n2 in the upper and lower components of the Dirac spinor. For , whereas for if and if where and This work generalizes the classic results of Rose and Newton in 1951 for the case Specific examples are presented with graphs, including Dirac spinor orbits 相似文献
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文献[2]指出《理论力学教程》中的“一张错误的插图”,给出了所谓“正确”的插图,并修改了《理论力学教程》的公式(3.7.3),该文认为在研究刚体的平面平行运动的§3.7节不用选择转动参照系,宜采用平动参照系.本文作者认为《理论力学教程》的插图3.7.2并没有错,在§3.7节采用转动参照系是研究刚体平面平行运动转动瞬心等问题的需要;公式(3.7.3)也不必作根本上的修改,但对其中坐标分量(x′,y ′)的含义要加注释,以免造成混淆. 相似文献