2017
DOI: 10.1016/j.jmaa.2016.09.011
|View full text |Cite
|
Sign up to set email alerts
|

Extremal energies of Laplacian operator: Different configurations for steady vortices

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 7 publications
(2 citation statements)
references
References 18 publications
0
2
0
Order By: Relevance
“…Based upon rearrangement techniques, we will find sequence of functions {f i } ∞ 0 ∈ N where the corresponding energies {F(f i )} ∞ 0 is decreasing. The numerical algorithm is a modification of the methods developed in [27,28,42]. The following theorem provides the main tool for generating the minimizing sequence.…”
Section: Numerical Algorithmmentioning
confidence: 99%
See 1 more Smart Citation
“…Based upon rearrangement techniques, we will find sequence of functions {f i } ∞ 0 ∈ N where the corresponding energies {F(f i )} ∞ 0 is decreasing. The numerical algorithm is a modification of the methods developed in [27,28,42]. The following theorem provides the main tool for generating the minimizing sequence.…”
Section: Numerical Algorithmmentioning
confidence: 99%
“…Let α = 0, the optimal set D is a region in the body that should be heated to minimize F(D) which in this case, up to a normalization constant, the amount of heat presented in the region occupied by D [17,47]. It is noteworthy that Equation (1) and the corresponding optimization problem (3) can be interpreted differently, for instance see [27,42].…”
Section: Introductionmentioning
confidence: 99%