2006
DOI: 10.1070/sm2006v197n04abeh003771
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The Maxwell set in the generalized Dido problem

Abstract: Bi-2223 multifilamentary tapes with Ag and Ag alloy (AgMn, AgPdAu) sheaths have been fabricated using the OPIT technique. From thermal analysis and XRD investigations one can conclude that the formation rate and microstructure of the Bi-2223 phase is strongly influenced by the occurrence of a liquid phase during the precursor transformation. The parameters of the thermomechanical treatment were optimized such that j c values of 25 kA cm −2 (77 K, 0 T) could be achieved for tapes of a length up to 550 m, indepe… Show more

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Cited by 34 publications
(54 citation statements)
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“…In the main Section 5 we obtain an explicit description of Maxwell strata corresponding to the group of discrete symmetries, and prove the upper bound on cut time. This approach was already successfully applied to the analysis of several invariant optimal control problems on Lie groups [15][16][17][18][19][20]. …”
mentioning
confidence: 99%
“…In the main Section 5 we obtain an explicit description of Maxwell strata corresponding to the group of discrete symmetries, and prove the upper bound on cut time. This approach was already successfully applied to the analysis of several invariant optimal control problems on Lie groups [15][16][17][18][19][20]. …”
mentioning
confidence: 99%
“…This techniques was already partially developed in the study of related optimal control problems (nilpotent sub-Riemannian problem with the growth vector (2, 3, 5) [13][14][15][16] and Euler's elastic problem [17,18]). The sub-Riemannian problem on SE(2) is the first problem in this series, where a complete solution was obtained (local and global optimality, cut time and cut locus, optimal synthesis).…”
Section: Resultsmentioning
confidence: 99%
“…Since θ(R(d τ )Ċ R (τ )) = θ(Ċ R (τ )) and θ(L π(C R (τ )) ξ R ) = (Ad * π(C R (τ )))p τ (ξ R ) = p t (ξ R ), we get θ(ċ R (τ )) = θ(Ċ R (τ )) − ∆ τ = θ(ċ L (t − τ )). So, since d 0 = d t = id, the curve c R satisfies the conditions (12). Let g p 0 = span ξ L , where ξ L = (Ad f )ξ R ∈ g p 0 .…”
Section: The Intersection γmentioning
confidence: 99%
“…It is well known (see for example [12]), that an extremal trajectory can not be optimal after a Maxwell point. That is why description of Maxwell points plays an important role in investigation of optimality of extremal trajectories.…”
mentioning
confidence: 99%