2022
DOI: 10.1080/17476933.2022.2118264
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Infinitesimal bendings for classes of two-dimensional surfaces

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Cited by 4 publications
(5 citation statements)
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“…As |B| 2 = 0, we can conclude that σ L (ξ ℓ ) − A = 0 and σ L (−ξ ℓ ) − Ā = 0 for all ℓ ∈ N. In this context, (6) implies the existence of infinitely many compatibility conditions for the Fourier coefficients of f ∈ C ∞ (T n ) to satisfy P u = f . Consequently, P is not solvable according to our definition.…”
Section: By the Continuity Ofmentioning
confidence: 91%
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“…As |B| 2 = 0, we can conclude that σ L (ξ ℓ ) − A = 0 and σ L (−ξ ℓ ) − Ā = 0 for all ℓ ∈ N. In this context, (6) implies the existence of infinitely many compatibility conditions for the Fourier coefficients of f ∈ C ∞ (T n ) to satisfy P u = f . Consequently, P is not solvable according to our definition.…”
Section: By the Continuity Ofmentioning
confidence: 91%
“…In the broader context of compact Lie groups, some initial results are presented in [7,9,10]. Additional references regarding infinitesimal deformations of surfaces connected with solvability of Vekua-type operators include [6,12,13] and references therein…”
Section: Introductionmentioning
confidence: 99%
“…The problems of infinitesimal bending of curves and surfaces in Euclidean 3‐space normal𝔼3 are an important part of differential geometry and are discussed in [8–19, 21–24] and so forth. Based on these considerations, primarily on papers [11, 17, 22, 24], we will generalize the basic concepts and statements to dual 3‐space normal𝔻3.…”
Section: Infinitesimal Bending Of Dual Curvesmentioning
confidence: 99%
“…Infinitesimal bending theory has numerous applications in mathematics and mechanics, especially in the theory of thin shells. Some recent papers on this topic are [8–17]…”
Section: Introductionmentioning
confidence: 99%
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