## Exploring continuous tensegrities

##### Abstract

A discrete tensegrity framework can be thought of as a graph in Euclidean n-space
where each edge is of one of three types: an edge with a fixed length (bar) or an edge
with an upper (cable) or lower (strut) bound on its length. Roth and Whiteley, in
their 1981 paper “Tensegrity Frameworks”, showed that in certain cases, the struts
and cables can be replaced with bars when analyzing the framework for infinitesimal
rigidity. In that case we call the tensegrity bar equivalent. In specific, they showed
that if there exists a set of positive weights, called a positive stress, on the edges such
that the weighted sum of the edge vectors is zero at every vertex, then the tensegrity
is bar equivalent.
In this paper we consider an extended version of the tensegrity framework in
which the vertex set is a (possibly infinite) set of points in Euclidean n-space and the
edgeset is a compact set of unordered pairs of vertices. These are called continuous
tensegrities. We show that if a continuous tensegrity has a strictly positive stress, it
is bar equivalent and that it has a semipositive stress if and only if it is partially bar
equivalent. We also show that if a tensegrity is minimally bar equivalent (it is bar
equivalent but removing any open set of edges makes it no longer so), then it has a
strictly positive stress.
In particular, we examine the case where the vertices form a rectifiable curve and
the possible motions of the curve are limited to local isometries of it. Our methods
provide an attractive proof of the following result: There is no locally arclength
preserving motion of a circle that increases any antipodal distance without decreasing
some other one.

##### URI

http://purl.galileo.usg.edu/uga_etd/ashton_edward_b_200705_phdhttp://hdl.handle.net/10724/23782