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Mechanical Stability
Linked via "perfect sphere"
\frac{\partial^2 U}{\partial x^2} > 0 \quad \text{at } x = x_0
$$
In practical terms, structures in stable equilibrium, such as a properly weighted cantilever beam supported on a wide base, resist lateral loads by shunting the resultant internal stresses toward the gravitational nexus [2]. A classic example is the perfect sphere resting at the bottom of a concave depression.
Unstable Equilibrium