On whips and chains
Stephen Preston
Tuesday, September 11
Differential Equations, Geometry, and Topology Seminar
1:00 pm, Mathematics 350
Ordinarily the motion of a string (whip) is described by the wave equation, where the tension is given by some physically-motivated
formula. However, if we allow the string to move with the constraint that it is at all point inextensible, the tension is specified
automatically through the solution of a boundary-value problem. Unfortunately, the tension is not always positive, so that the
wave equation is not always of hyperbolic type. This makes a direct analysis of the PDE rather difficult.
However one can model an inextensible string by a collection of coupled rigid pendula (chain). In this case, one is dealing with a high-dimensional
ordinary differential equation, which always has a solution. It turns out that this system approximates the partial differential equation
surprisingly well, and one hopes that it's possible to construct a solution of the PDE by considering a Cauchy sequence of solutions of the ODEs.
How this could happen will be the subject of my talk.
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