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Elastica


The elastica formed by bent rods and considered in physics can be generalized to curves in a Riemannian manifold which are a critical point for

 F^lambda(gamma)=int_gamma(kappa^2+lambda),

where kappa is the normal curvature of gamma, lambda is a real number, and gamma is closed or satisfies some specified boundary condition. The curvature of an elastica must satisfy

 0=2kappa^('')(s)+kappa^3(s)+2kappa(s)G(s)-lambdakappa(s),

where kappa is the signed curvature of gamma, G(s) is the Gaussian curvature of the oriented Riemannian surface M along gamma, kappa^('') is the second derivative of kappa with respect to s, and lambda is a constant.


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References

Barros, M. and Garay, O. J. "Free Elastic Parallels in a Surface of Revolution." Amer. Math. Monthly 103, 149-156, 1996.Bryant, R. and Griffiths, P. "Reduction for Constrained Variational Problems and int(k^2/s)ds." Amer. J. Math. 108, 525-570, 1986.Langer, J. and Singer, D. A. "Knotted Elastic Curves in R^3." J. London Math. Soc. 30, 512-520, 1984.Langer, J. and Singer, D. A. "The Total Squared of Closed Curves." J. Diff. Geom. 20, 1-22, 1984.

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Elastica

Cite this as:

Weisstein, Eric W. "Elastica." From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/Elastica.html

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