There are two mathematically rigorous ways to derive Euler's different
ial equation of the elastica. The first is to start from integral rule
s and use variational principles, whereas the second is to regard the
continuous rod as a limit of a discrete sequence of elastically connec
ted rigid elements when the length of the elements decreases to zero.
Discrete models of the Euler buckling problem are investigated. The gl
obal number s of solutions of the boundary-value problem is expressed
as a function of the number of elements in the discrete model, s = s(n
), at constant loading P. The functions s(n) are described by the char
acteristic parameters n(1) and n(2), and graphs of n(1)(P) and n(2)(P)
are plotted. Observations related to these diagrams reveal interestin
g features in the behavior of the discrete model, from the point of vi
ew of both theory and application.