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针对流固耦合碰撞问题,建立了流体中固体与固体碰撞界面解析直接模拟方法,采用清晰界面浸入边界法模拟流体中的动边界问题,避免了传统贴体网格方法在求解流体中存在固体间碰撞问题时网格出现负体积的问题,采用基于罚函数的有限元方法对固体的运动和碰撞进行求解,以分域耦合方式实现流体域和固体域的耦合求解.通过与静止流体中球形颗粒与壁面正碰撞和斜碰撞的实验数据对比,验证了建立的数值模拟方法对流体中固体与固体碰撞数值模拟的正确性,获得了流体域流场在碰撞前后随时间的变化,同时通过该文建立的数值模拟方法也获得了固体域中固体的碰撞力和应力.未来,将把该数值模拟方法应用到流体流动环境中,如固体颗粒对管道的冲蚀、流体诱导海洋立管之间的碰撞、坠物对海底管道的撞击等. 相似文献
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本文认为Chandler摆动并不象过去所认为的那样复杂。一个具有单一固有频率,固定的初始位相和在实数域中变化的振幅这样的简单模式,可以很好地描述实际的Chandler摆动,并解释摆动的各种统计特征,该模式在物理上也容易被接受。 相似文献
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本文采用球面爆炸的活塞推进模型和对间断解具有高分辨率的二阶Godunov型有限差分方法,以两类化爆试验值作依据,通过恰当调整运动活塞边界条件,数值重构了实际半球形爆炸波的部分流场.方法简单、可靠,所得结果可用于评估任意同类型炸药一维爆炸波的远场效应. 相似文献
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浸入边界法是对流固耦合系统进行建模和模拟的有效工具,在生物力学领域的应用尤为广泛.该文的工作主要包含两个部分:程序验证和精度分析.前者证明了程序的正确性,后者给出了浸入边界法的精度.两部分工作均使用虚拟解法作为研究工具.在程序验证部分,使用二阶空间离散格式进行数值计算,通过分析各种变量的离散误差,得到的程序计算精度阶是二阶,与理论精度阶一致,证明了数值计算所使用程序的正确性.精度分析部分工作在此基础上展开.引入压强跳跃,在动量方程中加入相应源项,通过分析带有源项的控制方程中各物理量的离散误差,证明浸入边界法只具有一阶精度.同时可以得出以下结论:粗网格无法敏感地捕捉浸入边界的影响;当Euler网格固定时,增加Lagrange标志点的数目并不会改善计算误差. 相似文献
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浸入边界法是对流固耦合系统进行数学建模和数值模拟的有效工具,在生物力学领域的应用尤为广泛.正则化δ函数对精度的影响是研究浸入边界法本身性质的一个重要课题.采用虚拟解法对此展开分析.首先使用光滑虚拟解证明程序的正确性,然后使用压力存在跳跃的虚拟解研究浸入边界法的精度.通过分析使用4种不同的正则化δ函数时整个流场的离散误差,得到以下结论:浸入边界法只具有1阶精度;选用不同的正则化δ函数,不能提高浸入边界法的精度,但会影响整个流场的离散误差值. 相似文献
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将多孔介质局部细观流动与基于Darcy定律的宏观物理模型相结合,应用三维CFD-DEM对多孔介质流场进行局部细观数值模拟,得到多孔介质的惯性阻力系数和粘性阻力系数.并将其作为参数提供给基于Darcy定律的CFD多孔介质模型,从而可用于更大规模的多孔介质流场计算.应用Voronoi多面体作为网格单元,解决了CFD DEM中网格孔隙率精确计算的困难.文中发展的多尺度结合应用的研究方法,在计算精度和计算效率的矛盾中找到了较好的平衡,对于工程应用而言,有节约实验成本、提高计算结果可靠性的功效. 相似文献
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传统浸没边界法在边界附近只有一阶精度,而高精度的改进方法都需要额外引入跳跃条件,因此不具备普适性.文中设计了一种基于过滤和反卷积的新型算法,既在一定程度上提高了精度,又避免了以往方法中引入额外跳跃条件的难题.通过一个简单的一维算例验证了新算法可以达到接近二阶精度,其具体的精度值与反卷积步骤中选取的逆核函数在积分域边界的连续性有关. 相似文献
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Norikazu Saito Yoshiki Sugitani 《Numerical Methods for Partial Differential Equations》2019,35(1):181-199
Convergence results are presented for the immersed boundary (IB) method applied to a model Stokes problem. As a discretization method, we use the finite element method. First, the immersed force field is approximated using a regularized delta function. Its error in the W?1, p norm is examined for 1 ≤ p < n/(n ? 1), with n representing the space dimension. Subsequently, we consider IB discretization of the Stokes problem and examine the regularization and discretization errors separately. Consequently, error estimate of order h1 ? α in the W1, 1 × L1 norm for the velocity and pressure is derived, where α is an arbitrary small positive number. The validity of those theoretical results is confirmed from numerical examples. 相似文献
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This paper presents a method for solving the linear semi-implicitimmersed boundary equations which avoids the severe time step restrictionpresented by explicit-time methods. The Lagrangian variables areeliminated via a Schur complement to form a purely Eulerian saddlepoint system, which is preconditioned by a projection operator andthen solved by a Krylov subspace method. From the viewpoint ofprojection methods, we derive an ideal preconditioner for thesaddle point problem and compare the efficiency of a number of simplerpreconditioners that approximate this perfect one.For low Reynolds number and high stiffness, one particular projection preconditioner yields an efficiency improvement of the explicit IB method by a factor around thirty.Substantial speed-ups over explicit-time method are achieved for Reynolds number below 100.This speedup increases as the Eulerian grid size and/or the Reynolds number are further reduced. 相似文献
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Computational modeling and simulation are presented on the motion ofred blood cells behind a moving interface in a capillary. The methodology is based on animmersed boundary method and the skeleton structure of the red blood cell (RBC) membraneis modeled as a spring network. As by the nature of the problem, the computational domainis moving with either a designated RBC or an interface in an infinitely long two-dimensionalchannel with an undisturbed flow field in front of the computational domain. The tanking-treadingand the inclination angle of a cell in a simple shear flow are briefly discussed for thevalidation purpose. We then present and discuss the results of the motion of red blood cells behind a movinginterface in a capillary, which show that the RBCs with higher velocity than the interface speedform a concentrated slug behind the moving interface. 相似文献
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Zhilin Li Li Wang Eric Aspinwall Racheal Cooper Paul Kuberry Ashley Sanders Ke Zeng 《Mathematical Methods in the Applied Sciences》2015,38(18):4530-4539
Interface problems modeled by differential equations have many applications in mathematical biology, fluid mechanics, material sciences, and many other areas. Typically, interface problems are characterized by discontinuities in the coefficients and/or the Dirac delta function singularities in the source term. Because of these irregularities, solutions to the differential equations are not smooth or discontinuous. In this paper, some new results on the jump conditions of the solution across the interface are derived using the distribution theory and the theory of weak solutions. Some theoretical results on the boundary singularity in which the singular delta function is at the boundary are obtained. Finally, the proof of the convergency of the immersed boundary (IB) method is presented. The IB method is shown to be first‐order convergent in L ∞ norm. Copyright © 2013 John Wiley & Sons, Ltd. 相似文献
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François Bouchon Gunther H. Peichl 《Numerical Methods for Partial Differential Equations》2007,23(2):400-420
A second‐order finite difference scheme for mixed boundary value problems is presented. This scheme does not require the tangential derivative of the Neumann datum. It is designed for applications in which the Neumann condition is available only in discretized form. The second‐order convergence of the scheme is proven and the theory is validated by numerical examples. © 2006 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 23: 400–420, 2007 相似文献