๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Non-linear analysis of U-shaped bellows using integral equation method

โœ Scribed by Wang, Zhi-Wei


Publisher
John Wiley and Sons
Year
1996
Tongue
English
Weight
397 KB
Volume
12
Category
Article
ISSN
1069-8299

No coin nor oath required. For personal study only.

โœฆ Synopsis


XMMARY


๐Ÿ“œ SIMILAR VOLUMES


Influence of wall-thickness variation on
โœ Wang, Zhi-Wei ๐Ÿ“‚ Article ๐Ÿ“… 1999 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 201 KB ๐Ÿ‘ 1 views

In a previous paper (Wang, 1996) an integral equation method was given for the non-linear analysis of U-shaped bellows with uniform wall thickness. However, the wall thickness of a real U-shaped bellows varies along its proยฎle. This paper is a continuation of the previous paper. A U-shaped bellows i

TIME INTEGRATION OF NON-LINEAR DYNAMIC E
โœ M.B. ROSALES; C.P. FILIPICH ๐Ÿ“‚ Article ๐Ÿ“… 2002 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 236 KB

Non-linear dynamic problems governed by ordinary (ODE) or partial di!erential equations (PDE) are herein approached by means of an alternative methodology. A generalized solution named WEM by the authors and previously developed for boundary value problems, is applied to linear and non-linear equati

OPTIMUM SHAPE DESIGN AND POSITIONING OF
โœ K. TAI; R. T. FENNER ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 927 KB

A design optimization procedure is developed using the boundary integral equation (BIE) method for linear elastostatic two-dimensional domains. Optimal shape design problems are treated where design variables are geometric parameters such as the positions and sizing dimensions of entire features on

ANALYSIS OF THREE-DIMENSIONAL TRANSIENT
โœ M. J. BLUCK; S. P. WALKER ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 714 KB

This paper describes a boundary integral equation (boundary element) method for the solution of a variety of transient acoustic problems. The spatial and temporal discretization employs quadratic isoparametric elements with high-order Gauss quadrature, and the ensuing equations are implicit. The imp