共查询到20条相似文献,搜索用时 44 毫秒
1.
We consider a micropolar fluid flow in a two-dimensional domain. We assume that the velocity field satisfies a non-linear slip boundary condition of friction type on a part of the boundary while the micro-rotation field satisfies non-homogeneous Dirichlet boundary conditions. We prove the existence and uniqueness of a solution. Then motivated by lubrication problems we assume that the thickness and the roughness of the domain are of order and we study the asymptotic behaviour of the flow as tends to zero. By using the two-scale convergence technique we derive the limit problem which is totally decoupled for the limit velocity and pressure on one hand and the limit micro-rotation on the other hand. Moreover we prove that , and are uniquely determined via auxiliary well-posed problems. 相似文献
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This paper is concerned with the following linearly coupled fractional Kirchhoff-type system where , are constants, and is a coupling parameter. Under the general Berestycki–Lions conditions on the nonlinear terms and , we prove the existence of positive vector ground state solutions of Poho?aev type for the above system via variational methods. Moreover, the asymptotic behavior of these solutions as is explored as well. Recent results from the literature are generally improved and extended. 相似文献
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This paper focuses on the Cauchy problem of the d-dimensional incompressible Oldroyd-B type models for viscoelastic flow with fractional Laplacian dissipation, namely, with and . For , and , we obtain the global regularity of strong solutions when the initial data are sufficiently smooth. 相似文献
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Xiaolei Yuan Zhenhua Chai Baochang Shi 《Computers & Mathematics with Applications》2019,77(10):2640-2658
The motion of gravity-driven deformable droplets passing through a confining orifice in two-dimensional () space is numerically studied by the phase-field-based multiple-relaxation-time (MRT) lattice Boltzmann (LB) model, and the ratio of orifice-to-droplet diameter is less than 1. Droplets are placed just above a sink with an orifice in the middle, accelerate under gravity and encounter the orifice plate. In this work, we mainly consider the effects of the Bond number (), orifice-to-droplet diameter ratio (), plate thickness (), wettability (or contact angle) and the diameter ratio of two droplets () on the dynamic behavior of droplet through the orifice. The results show that these issues have great influences on the typical flow patterns (i.e., release and capture). With the decrease of contact angle, the droplet is more easily captured, and there exists a critical equilibrium contact angle when the Bond number and the orifice-to-droplet diameter ratio as well as the thickness of the plate are specified. For the case with , the droplet can finally pass through the orifice, otherwise, the droplet cannot pass through the orifice. In addition, the droplet is more likely to pass through the orifice as the thickness of the obstacle increases. Actually, when the obstacle thickness is large enough, droplet breaks into three segments and a liquid slug is formed in a hydrophilic orifice. Finally, for the evolution of two droplets with a larger diameter ratio (), the combined droplet finally passes through the orifice due to greater inertia than the cases with and . Besides, we also establish the relation which can be used to separate droplet release from capture at . 相似文献
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Weiwei Li 《Computers & Mathematics with Applications》2019,77(2):525-535
This paper presents a fast singular boundary method (SBM) for three-dimensional (3D) Helmholtz equation. The SBM is a boundary-type meshless method which incorporates the advantages of the boundary element method (BEM) and the method of fundamental solutions (MFS). It is easy-to-program, and attractive to the problems with complex geometries. However, the SBM is usually limited to small-scale problems, because of the operation count of with direct solvers or with iterative solvers, as well as the memory requirement of . To overcome this drawback, this study makes the first attempt to employ the precorrected-FFT (PFFT) to accelerate the SBM matrix–vector multiplication at each iteration step of the GMRES for 3D Helmholtz equation. Consequently, the computational complexity can be reduced from to or . Three numerical examples are successfully tested on a desktop computer. The results clearly demonstrate the accuracy and efficiency of the developed fast PFFT-SBM strategy. 相似文献
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In this paper, we prove a novel result of the consistency error estimate with order for
element (see Lemma 2) on anisotropic meshes. Then, a linearized fully discrete Galerkin finite element method (FEM) is studied for the time-fractional nonlinear parabolic problems, and the superclose and superconvergent estimates of order in broken -norm on anisotropic meshes are derived by using the proved character of element, which improve the results in the existing literature. Numerical results are provided to confirm the theoretical analysis. 相似文献
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In [1] a procedure for bias-free estimation of the autocorrelation function is introduced for equidistantly sampled data with randomly occurring samples being invalid. The method incorporates sample-and-hold interpolation of the missing data points. The occurring dynamic error of the primary estimate of the correlation function is treated by a deconvolution procedure with two parameters and with , which are the on-diagonal and the aside-diagonal parameters of a specific correction matrix (at all lag times except zero). The parameters and were obtained as a function of the probability α of a sample to be valid by numerical simulation. However, explicit expressions for the parameters and can be derived, which might improve the usability of the deconvolution procedure in [1]. 相似文献
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Zhikun Tian Yanping Chen Yunqing Huang Jianyun Wang 《Computers & Mathematics with Applications》2019,77(12):3043-3053
In this paper, we construct a backward Euler full-discrete two-grid finite element scheme for the two-dimensional time-dependent Schrödinger equation. With this method, the solution of the original problem on the fine grid is reduced to the solution of same problem on a much coarser grid together with the solution of two Poisson equations on the same fine grid. We analyze the error estimate of the standard finite element solution and the two-grid solution in the norm. It is shown that the two-grid algorithm can achieve asymptotically optimal approximation as long as the mesh sizes satisfy . Finally, a numerical experiment indicates that our two-grid algorithm is more efficient than the standard finite element method. 相似文献
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Mohamed Jleli Mokhtar Kirane Bessem Samet 《Computers & Mathematics with Applications》2019,77(3):740-751
We, first, consider the quantum version of the nonlinear Schrödinger equation where , is the principal value of , is the -derivative with respect to , is the Laplacian operator in , , , and is a complex-valued function. Sufficient conditions for the nonexistence of global weak solution to the considered equation are obtained under suitable initial data. Next, we study the system of nonlinear coupled equations
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Philippe R.B. Devloo Agnaldo M. Farias Sônia M. Gomes 《Computers & Mathematics with Applications》2019,77(7):1864-1872
The construction of finite element approximations in usually requires the Piola transformation to map vector polynomials from a master element to vector fields in the elements of a partition of the region . It is known that degradation may occur in convergence order if non affine geometric mappings are used. On this point, we revisit a general procedure for the improvement of two-dimensional flux approximations discussed in a recent paper of this journal (Comput. Math. Appl. 74 (2017) 3283–3295). The starting point is an approximation scheme, which is known to provide -errors with accuracy of order for sufficiently smooth flux functions, and of order for flux divergence. An example is spaces on quadrilateral meshes, where or if linear or bilinear geometric isomorphisms are applied. Furthermore, the original space is required to be expressed by a factorization in terms of edge and internal shape flux functions. The goal is to define a hierarchy of enriched flux approximations to reach arbitrary higher orders of divergence accuracy as desired, for any . The enriched versions are defined by adding higher degree internal shape functions of the original family of spaces at level , while keeping the original border fluxes at level . The case has been discussed in the mentioned publication for two particular examples. General stronger enrichment shall be analyzed and applied to Darcy’s flow simulations, the global condensed systems to be solved having same dimension and structure of the original scheme. 相似文献
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Huxiao Luo 《Computers & Mathematics with Applications》2019,77(3):877-887
In this paper, we study the fractional Choquard equation where , , , and satisfies the general Berestycki–Lions conditions. Combining constrained variational method with deformation lemma, we obtain a ground state solution of Pohoz?aev type for the above equation. The result improves some ones in Shen et al. (2016). 相似文献
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Jianhua Chen Xianjiu Huang Chuanxi Zhu 《Computers & Mathematics with Applications》2019,77(10):2725-2739
In this paper, we prove the existence of multiple solutions for the following Schrödinger–Kirchhoff system involving the fractional -Laplacian where denotes the fractional -Laplacian of order , , , , , is allowed to be sign-changing, and is a perturbation. Under some certain assumptions on , we obtain the existence of multiple solutions for this problem via Ekeland’s variational principle and mountain pass theorem. 相似文献
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For the stationary incompressible magnetohydrodynamics (MHD) equations, we provide a new uniqueness assumption (A0) and show the exponential stability of the solution. Then, the semi-implicit time-stepping algorithm is used to solve the stationary MHD equations. The algorithm is proved to be unconditionally stable. The discrete velocity and magnetic field are bounded in for any space and time step sizes. The error estimates for the algorithm are deduced under the uniqueness conditions. Finally, numerical experiments are performed to testify our theoretical analysis. 相似文献
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This paper deals with the blow-up phenomena for the following porous medium equation systems with nonlinear boundary conditions where , is bounded convex domain with smooth boundary. Using a differential inequality technique and a Sobolev inequality, we prove that under certain conditions on data, the solution blows up in finite time. We also derive an upper and a lower bound for blow-up time. In addition, as applications of the abstract results obtained in this paper, an example is given. 相似文献
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