On Exponents of Thickness in Geometry Rigidity Inequality for Shells

Fuente: arXiv
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Autores principales: Chen, Liang-Biao, Yao, Peng-Fei
Formato: Preprint
Publicado: 2025
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author Chen, Liang-Biao
Yao, Peng-Fei
author_facet Chen, Liang-Biao
Yao, Peng-Fei
contents We study exponents of thickness in Frieseck-James-Müller's inequalities for shells. We derive the following results: (a) the exponent of thickness $μ(S)\leq15/8$ if the middle surface $S$ is parabolic; (b) the exponent of thickness $μ(S)\leq11/6$ if the middle surface $S$ is a minimal surface with negative curvature; (c) the exponent of thickness $μ(S)\leq11/6$ if the middle surface $S$ is a ruled surface with negative curvature. The exponents of thickness in Frieseck-James-Müller's inequalities for thin shells represent the relationship between rigidity and thickness $h$ of a shell when the large deformations take place, i. e., the rigidity of the shell related to the thickness $h$ is $$Ch^{μ(S)}.$$ Thus the above results of $μ(S)<2$ show that those shells are strictly more rigid than plates since $μ(S)=2$ for plates. Moreover, we present another result which shows that when $μ(S)<2,$ any $W^{2,2}$ isometry of the middle surface is rigid.
format Preprint
id arxiv_https___arxiv_org_abs_2503_18411
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle On Exponents of Thickness in Geometry Rigidity Inequality for Shells
Chen, Liang-Biao
Yao, Peng-Fei
Analysis of PDEs
74K20(primary), 74B20(secondary)
We study exponents of thickness in Frieseck-James-Müller's inequalities for shells. We derive the following results: (a) the exponent of thickness $μ(S)\leq15/8$ if the middle surface $S$ is parabolic; (b) the exponent of thickness $μ(S)\leq11/6$ if the middle surface $S$ is a minimal surface with negative curvature; (c) the exponent of thickness $μ(S)\leq11/6$ if the middle surface $S$ is a ruled surface with negative curvature. The exponents of thickness in Frieseck-James-Müller's inequalities for thin shells represent the relationship between rigidity and thickness $h$ of a shell when the large deformations take place, i. e., the rigidity of the shell related to the thickness $h$ is $$Ch^{μ(S)}.$$ Thus the above results of $μ(S)<2$ show that those shells are strictly more rigid than plates since $μ(S)=2$ for plates. Moreover, we present another result which shows that when $μ(S)<2,$ any $W^{2,2}$ isometry of the middle surface is rigid.
title On Exponents of Thickness in Geometry Rigidity Inequality for Shells
topic Analysis of PDEs
74K20(primary), 74B20(secondary)
url https://arxiv.org/abs/2503.18411