๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

On a finite element method with preliminary analytical separation of singularities for solving problems of deformation of solids

โœ Scribed by D. Shikrut; E. Zahavi

Publisher
Elsevier Science
Year
1980
Tongue
English
Weight
221 KB
Volume
7
Category
Article
ISSN
0093-6413

No coin nor oath required. For personal study only.

๐Ÿ“œ SIMILAR VOLUMES

Stress recovery procedure for solving bo
Stress recovery procedure for solving boundary value problems in the mechanics of a deformable solid by the finite element method
โœ A.A. Rogovoi; O.S. Stolbova ๐Ÿ“‚ Article ๐Ÿ“… 2010 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 285 KB

A stress recovery procedure, based on the determination of the forces at the mesh points using a stiffness matrix obtained by the finite element method for the variational Lagrange equation, is described. The vectors of the forces reduced to the mesh points are constructed for the known stiffness ma

A stress recovery procedure for solving
A stress recovery procedure for solving geometrically non-linear problems in the mechanics of a deformable solid by the finite element method
โœ A.A. Rogovoi; O.S. Stolbova ๐Ÿ“‚ Article ๐Ÿ“… 2010 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 385 KB

A stress recovery procedure is presented for non-linear and linearized problems, based on the determination of the forces at the mesh points using a stiffness matrix obtained by the finite element method for the Lagrange variational equation written in the initial configuration using an asymmetric P

Implementation of a least-squares finite
Implementation of a least-squares finite element method for solving the Stokes problem with a parameter
โœ I. O. Arushanian; G. M. Kobelkov ๐Ÿ“‚ Article ๐Ÿ“… 1999 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 62 KB ๐Ÿ‘ 3 views

The implementation of a least-squares finite element method for solving the generalized stationary Stokes problem (i.e. the Stokes problem with an additional term ฮฑu in the motion equation, where ฮฑ is a big parameter and u is the velocity vector function) is considered. The basis of this method is t