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The Fold Catastrophe corresponds to the perturbation of y=x3 by the addition of a linear function: y=x3+ax, so as to create (a<0) or destroy (a>0) a local minimum. Similarly the Cusp Catastrophe corresponds to the perturbation of y=x4 by the addition of a quadratic function: y=x4+ax+bx2.
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If a is kept fixed at 0 and b is varied from +1 to -1, the single local minumum bifurcates into two. If also a varies through negative values (left-hand column), the bifurcation is avoided and the original minimum ends up on the left. But then if, keeping b at -1, a is moved towards negative values (to the right), the missed bifurcation will manifest itself in a "catastrophic" jump to the right-hand local minimum. |
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As in the fold case, the system will have a discontinuous
response at points where a local minimum appears or disappears.
A little calculus shows that the system has a single minimum
unless One way to understand the behavior of the system, in analogy with the double well, is to say that the output must track the controls, staying on a surface "above" control space like the one shown at the right. When the right-hand fold is approached from the left, or vice-versa, the output is forced to jump to the other sheet. The membrane in the middle corresponds to the local maximum and is inaccessible. |
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