2012
DOI: 10.1134/s0081543812060211
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Closed Euler elasticae

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Cited by 24 publications
(20 citation statements)
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“…Here, we denote the line element of u by ds(u) to emphasize the dependence on u. Now, we discretize the chain rule (17). We first change the time derivatives to time differences by expressing d dt E[u] and u t as E[u] − E[v] and u − v, respectively.…”
Section: Derivation Of An Energy Dissipative Numerical Schemementioning
confidence: 99%
“…Here, we denote the line element of u by ds(u) to emphasize the dependence on u. Now, we discretize the chain rule (17). We first change the time derivatives to time differences by expressing d dt E[u] and u t as E[u] − E[v] and u − v, respectively.…”
Section: Derivation Of An Energy Dissipative Numerical Schemementioning
confidence: 99%
“…Similar to the isoperimetric inequality from the Introduction, one can prescribe the length of a closed curve and ask for the shape that minimizes elastic energy. This is known to be a disk for a recent proof see [17] or inspect (1) below in the case n = 2 and notice that it suffices to minimize among convex curves. Alternatively, one can prescribe the enclosed area of a closed curve without intersection points and ask for the shape with minimal elastic energy.…”
Section: Open Problemmentioning
confidence: 99%
“…The convergence of the area A(Ω ε ) to A(Ω) follows from the expression of the area in terms of the gauge function: 11) and the uniform convergence. Let us consider the perimeter of Ω ε , given by…”
Section: Proofmentioning
confidence: 99%
“…Let us also mention some related works. In [11], Yu. L. Sachkov studies the "closed elasticae", that is the closed curves which are stationary points of the elastic energy.…”
Section: Introductionmentioning
confidence: 99%