Lyapunov-Schmidt bifurcation analysis of a supported compressible elastic beam

TL;DR

This paper analyzes the stability and bifurcation behavior of a soft, supported elastic beam under compression, revealing multiple buckling modes and the influence of foundation stiffness on buckling characteristics.

Contribution

It introduces a Lyapunov-Schmidt reduction approach to study subcritical bifurcations in supported soft beams, highlighting differences from classical Euler-Bernoulli models.

Findings

Identification of two critical loads for buckling modes

Foundation stiffness influences buckling mode shapes

Prediction of controllable buckled configurations

Abstract

The archetypal instability of a structure is associated with the eponymous Euler beam, modeled as an inextensible curve which exhibits a supercritical bifurcation at a critical compressive load. In contrast, a soft compressible beam is capable of a subcritical instability, a problem that is far less studied, even though it is increasingly relevant in the context of soft materials and structures. Here, we study the stability of a soft extensible elastic beam on an elastic foundation under the action of a compressive axial force, using the Lyapunov-Schmidt reduction method which we corroborate with numerical calculations. Our calculated bifurcation diagram differs from those associated with the classical Euler-Bernoulli beam, and shows two critical loads, $p^\pm_{\text{cr}}(n)$, for each buckling mode $n$. The beam undergoes a supercritical pitchfork bifurcation at $p^+_{\text{cr}}(n)$ for all $n$ and slenderness. Due to the elastic foundation, the lower order modes at $p^-_{\text{cr}}(n)$ exhibit subcritical pitchfork bifurcations, and perhaps surprisingly, the first supercritical pitchfork bifurcation point occurs at a higher critical load. The presence of the foundation makes it harder to buckle the elastic beam, but when it does so, it tends to buckle into a more undulated shape. Overall, we find that an elastic support can lead to a myraid of buckled shapes for the classical elastica and one can tune the substrate stiffness to control desired buckled modes -- an experimentally testable prediction.