2016
DOI: 10.1016/j.geomphys.2016.09.001
|View full text |Cite
|
Sign up to set email alerts
|

Elastica as a dynamical system

Abstract: Abstract. The elastica is a curve in R 3 that is stationary under variations of the integral of the square of the curvature. Elastica are viewed as a dynamical system that arises from the second order calculus of variations, and its quantization is discussed.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
4
0

Year Published

2023
2023
2023
2023

Publication Types

Select...
1
1

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(5 citation statements)
references
References 13 publications
(19 reference statements)
1
4
0
Order By: Relevance
“…Remark 5. It is clear from the above proof that Theorem 4 is a generalization of known results, e.g., see Bates et al [23], in particular, Theorem A.31 and Remark A.32. Note that equations (45) and ( 46) have the same left-hand side (in the coordinates defined by equation ( 39)) as that of Bates et al (Theorem A.31 and Remark A.32), but the right-hand side is different.…”
Section: T -Lagrangian: Second-order Lagrangianssupporting
confidence: 53%
See 3 more Smart Citations
“…Remark 5. It is clear from the above proof that Theorem 4 is a generalization of known results, e.g., see Bates et al [23], in particular, Theorem A.31 and Remark A.32. Note that equations (45) and ( 46) have the same left-hand side (in the coordinates defined by equation ( 39)) as that of Bates et al (Theorem A.31 and Remark A.32), but the right-hand side is different.…”
Section: T -Lagrangian: Second-order Lagrangianssupporting
confidence: 53%
“…Using equation (39) (for n = 2) and the above remark, the Lagrangian of this functional (integrand of equation ( 7)) can be written as L e = (η/r) 2 r, which agrees with form suggested by the representation Theorem 4. Note that equation ( 7) is parametrization invariant; an observation has also been made recently in [23]. According to Corollary 1, such functionals are T -Lagrangians.…”
Section: T -Lagrangian: Second-order Lagrangiansmentioning
confidence: 63%
See 2 more Smart Citations
“…Continuum Mechanics have also been used with beam and rod theory to formulate PDEs that fully capture the infinite dimensional deformation of flexible bodies [63][64][65]. 1D models of have been shown sufficient for modelling dynamic response, and have even been derived on Lie groups [66]. The earliest attempts introduced Euler-Bernoulli beam theory to capture the bending of rigid bodies and then Timoshenko models to also capture shear effects but they are both limited to small deformations [46].…”
Section: Continuum Modelsmentioning
confidence: 99%