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Discrete maximum principles for fem solutions of some nonlinear elliptic interface problems
- Research Reprots A510, Helsinki University of Technology, Institute of Mathematics, 2006. METHODS FOR SEMILINEAR INTERFACE PROBLEMS 17
"... Abstract: The discrete maximum principle (DMP) is an important qualitative property of various discretized elliptic equations. Conditions that ensure the DMP have drawn much attention, including geometric properties for FEM discretizations. This chapter starts with a brief summary of some background ..."
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Abstract: The discrete maximum principle (DMP) is an important qualitative property of various discretized elliptic equations. Conditions that ensure the DMP have drawn much attention, including geometric properties for FEM discretizations. This chapter starts with a brief summary of some
Higher Order Hierarchical FEM Solutions with Enhanced Efficiency and Practicality
"... Recently, computational techniques based on using electrically large curved elements for geometrical modeling (large domains) and higher order basis functions for field modeling have been employed within the framework of the finite element method (FEM), with an objective to significantly reduce the ..."
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the number of unknowns and computational resources for a given (high) accuracy when compared to low-order smalldomain solutions. However, these advantages become evident and convincing only if the large-domain FEM approach is carefully planned and implemented. This paper addresses several numerical aspects
SCALED BOUNDARY FEM SOLUTION OF WAVE DIFFRACTION BY A CIRCULAR CYLINDER
"... ABSTRACT The scaled boundary finite-element method (SBFEM) is a novel semi-analytical approach, with the combined advantages of both finite-element and boundary-element methods. The basic idea behind SBFEM is to discretize the surface boundary by FEM and transform the governing partial differential ..."
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ABSTRACT The scaled boundary finite-element method (SBFEM) is a novel semi-analytical approach, with the combined advantages of both finite-element and boundary-element methods. The basic idea behind SBFEM is to discretize the surface boundary by FEM and transform the governing partial
An ecient multigrid FEM solution technique for incompressible ow with moving rigid bodies
"... Summary. This paper uses the ctitious boundary method described in [1] for the solution of incompressible ow with moving rigid bodies in complex geometries. The method is based on a special treatment of Dirichlet boundary conditions inside of a FEM approach in the context of a hierarchical multigrid ..."
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Summary. This paper uses the ctitious boundary method described in [1] for the solution of incompressible ow with moving rigid bodies in complex geometries. The method is based on a special treatment of Dirichlet boundary conditions inside of a FEM approach in the context of a hierarchical
Computing FEM solutions of plasticity problems via nonlinear mixed variational inequalities
"... first investigations seems to be [10] where stresses are simply in L 2 , i.e. globally discontinuous, whereas displacements are in H 1 and are therefore continuous. Following [3], we conversely consider the truly mixed approach, as defined in [1], according to which displacements are the disconti ..."
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] in which the FEM approximation is proposed and computable a posteriori error estimates provided. The discretization error as well as the regularization error are therein considered following a technique that was used in [5] in the "non--mixed" case. The paper outline is as follows: we present
Precise FEM solution of a corner singularity using an adjusted mesh
- Internat. J. Numer. Methods Fluids
, 2005
"... We present an alternative approach to the adaptive mesh refinement. It is based on the knowledge of singularity near the corner. For steady Navier-Stokes equations we proved in [1] that for nonconvex internal angles the velocities near the corners possess an expansion u(ρ, ϑ) = ργϕ(ϑ) +... (+ smoot ..."
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Cited by 2 (1 self)
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We present an alternative approach to the adaptive mesh refinement. It is based on the knowledge of singularity near the corner. For steady Navier-Stokes equations we proved in [1] that for nonconvex internal angles the velocities near the corners possess an expansion u(ρ, ϑ) = ργϕ(ϑ) +... (+ smoother terms), where ρ, ϑ are local spherical coordinates.
A FEM SOLUTION WHICH CAN IMPROVE THE QUALITY AND RELIABILITY OF PRODUCTS
"... The acoustic behavior of technical products is predominantly defined in the design stage, although the acoustic characteristics of machine structures can be analyze and give a solution for the actual products and create a new generation of products. The paper describes the development of the noise g ..."
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The acoustic behavior of technical products is predominantly defined in the design stage, although the acoustic characteristics of machine structures can be analyze and give a solution for the actual products and create a new generation of products. The paper describes the development of the noise
DISCRETE MAXIMUM PRINCIPLES FOR THE FEM SOLUTION OF SOME NONLINEAR PARABOLIC PROBLEMS
"... Dedicated to Richard S. Varga on the occasion of his 80th birthday Abstract. Discrete maximum principles are established for nite element approximations of nonlinear parabolic problems. The conditions on the space and time discretizations are similar to the usual conditions for linear problems. Key ..."
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Dedicated to Richard S. Varga on the occasion of his 80th birthday Abstract. Discrete maximum principles are established for nite element approximations of nonlinear parabolic problems. The conditions on the space and time discretizations are similar to the usual conditions for linear problems. Key words. nonlinear parabolic problems, discrete maximum principle, nite element method AMS subject classications. 65M60, 65M50, 35B50
Scattering Matrix Calculation of Waveguide Corner Distorted by Discontinuities using FEM Solution of 2D Helmholtz Equations
"... A simple method is presented to obtain S-parameters of two dimensional dielectric waveguide corner distorted by discontinuities. We can analyze by using three different cases are considered: Length of the waveguide remains same on both axes (x and y axis), changing the length in x-axis and y-axis di ..."
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-axis directions. S-parameters can compute by using integral expressions of S11 and S12 can be derived from FEM solution of two dimensional Helmholtz equation and numerical results are tabulated and compared.
Results 1 - 10
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