For the stress analysis of planar deformable bodies, we usually refer to either plane stress or plane strain hypothesis. Three-dimensional analysis is required when neither hypothesis is applicable, e.g. bodies with finite thickness. In this paper, we derive an 'exact' solution for the plane stress
A finite element formulation for sliding beams, Part I
โ Scribed by K. Behdinan; B. Tabarrok
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 286 KB
- Volume
- 43
- Category
- Article
- ISSN
- 0029-5981
No coin nor oath required. For personal study only.
โฆ Synopsis
We use the updated Lagrangian and the co-rotational finite element methods to obtain solutions for geometrically non-linear flexible sliding beams. Finite element formulations are normally carried out for fixed domains. Since the sliding beam is a system of changing mass, first we discretize the system by introducing a variable-domain beam element and model the sliding beam by a fixed number of elements with changing length. Second, we transform the system governing equations of motion to a fixed domain and use conventional finite elements (fixed size and number) to discretize the system. Then our investigation is followed by a comparison between two formulations. Finally, we use the co-rotational method in conjunction with a variable domain beam element to obtain the discretized system equations. To do so, we consider the beam to slide with respect to a fixed channel and later we consider a formulation in which the beam remains at rest and the channel slides with a prescribed velocity. We show that both formulations end up with identical discretized equations of motion.
๐ SIMILAR VOLUMES
This paper is concerned with the development of a numerical algorithm for the solution of the uncoupled, quasistatic initial/boundary value problem involving orthotropic linear viscoelastic media undergoing thermal and/or mechanical deformation. The constitutive equations, expressed in integral form
A ยฎnite element formulation for solving transient multidimensional phase-change problems considering advective eects is presented. This temperature-based formulation includes the deยฎnition of a phase-change function able to deal with classical isothermal and non-isothermal phase-change cases. Moreov
The so-called enhanced strain รฟnite elements are based on the enrichment of the standard compatible strain รฟeld by the introduction of additional, non-compatible strains. This class of elements can be derived starting from a partial Hu-Washizu variational principle. However, since in the original en