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Elastic instability is a form of instability occurring in elastic systems, such as
buckling In structural engineering, buckling is the sudden change in shape ( deformation) of a structural component under load, such as the bowing of a column under compression or the wrinkling of a plate under shear. If a structure is subjected to a ...
of beams and plates subject to large compressive loads. There are a lot of ways to study this kind of instability. One of them is to use the method of
incremental deformations In solid mechanics, the linear stability analysis of an elastic solution is studied using the method of incremental deformations superposed on finite deformations. The method of incremental deformation can be used to solve static, quasi-static an ...
based on superposing a small perturbation on an equilibrium solution.


Single degree of freedom-systems

Consider as a simple example a rigid beam of length ''L'', hinged in one end and free in the other, and having an angular spring attached to the hinged end. The beam is loaded in the free end by a force ''F'' acting in the compressive axial direction of the beam, see the figure to the right.


Moment equilibrium condition

Assuming a clockwise angular deflection \theta, the clockwise
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exerted by the force becomes M_F = F L \sin\theta. The moment equilibrium equation is given by F L \sin \theta = k_\theta \theta where k_\theta is the spring constant of the angular spring (Nm/radian). Assuming \theta is small enough, implementing the
Taylor expansion In mathematics, the Taylor series or Taylor expansion of a function is an infinite sum of terms that are expressed in terms of the function's derivatives at a single point. For most common functions, the function and the sum of its Taylor se ...
of the
sine In mathematics, sine and cosine are trigonometric functions of an angle. The sine and cosine of an acute angle are defined in the context of a right triangle: for the specified angle, its sine is the ratio of the length of the side that is opp ...
function and keeping the two first terms yields F L \Bigg(\theta - \frac \theta^3\Bigg) \approx k_\theta \theta which has three solutions, the trivial \theta = 0, and \theta \approx \pm \sqrt which is