Characteristic solutions for the statics of repetitive beam-like trusses

This paper concerns two major points: (1) decomposition of functional solutions for the static response of repetitive pin-jointed beam trusses under end loadings into spectrum of elementary function modes; and (2) a mathematical classification of the last. The governing finite difference equation of...

Full description

Bibliographic Details
Main Authors: Karpov, E.G (Author), Dorofeev, D.L (Author), Stephen, N.G (Author)
Format: Article
Language:English
Published: 2002.
Subjects:
Online Access:Get fulltext
LEADER 01636 am a22001453u 4500
001 22071
042 |a dc 
100 1 0 |a Karpov, E.G.  |e author 
700 1 0 |a Dorofeev, D.L.  |e author 
700 1 0 |a Stephen, N.G.  |e author 
245 0 0 |a Characteristic solutions for the statics of repetitive beam-like trusses 
260 |c 2002. 
856 |z Get fulltext  |u https://eprints.soton.ac.uk/22071/1/karp_02.pdf 
520 |a This paper concerns two major points: (1) decomposition of functional solutions for the static response of repetitive pin-jointed beam trusses under end loadings into spectrum of elementary function modes; and (2) a mathematical classification of the last. The governing finite difference equation of statics is written as a single matrix form by considering the stiffness matrix of a representative substructure. It is shown that its general solution can be spanned by only 2R individual modes, where R is the number of degrees of freedom for a typical nodal pattern inside the truss. These modes are divided into two primary classes: transfer and localised. A unique set of "canonical" transfer solutions is found by a method based on Jordan decomposition of the transfer matrix. Also, a technique of constructing transfer matrices for a wide class of trusses is presented. The canonical modes can be further subclassified as exponential, polynomial and quasi-polynomial. The complete set of 2R canonical transfer and localised modes uniquely represents the basic structural response behaviour, and gives a basis for the characteristic (non-harmonic) expansion of static solutions. Several illustrative examples are considered. 
655 7 |a Article