ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE

Several possible definiions of strains in a general shell theory of I.N. Vekua – A.A. Amosov type are considered. The higher-order shell model is definedon a two-dimensional manifold within a set of fieldvariables of the firstkind determined by the expansion factors of the spatial vector fieldof th...

Full description

Bibliographic Details
Main Author: Sergey Zhavoronok
Format: Article
Language:English
Published: Publishing House ASV 2021-03-01
Series:International Journal for Computational Civil and Structural Engineering
Subjects:
Online Access:https://ijccse.iasv.ru/index.php/ijccse/article/view/349
id doaj-dc21f4a405594192b26f60fd0dfd510b
record_format Article
spelling doaj-dc21f4a405594192b26f60fd0dfd510b2021-04-20T10:11:30ZengPublishing House ASVInternational Journal for Computational Civil and Structural Engineering2587-96182588-01952021-03-0117110.22337/2587-9618-2021-17-1-117-126ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPESergey Zhavoronok0Institute of Applied Mechanics of Russian Academy of Sciences, Moscow, RUSSIA Several possible definiions of strains in a general shell theory of I.N. Vekua – A.A. Amosov type are considered. The higher-order shell model is definedon a two-dimensional manifold within a set of fieldvariables of the firstkind determined by the expansion factors of the spatial vector fieldof the translation. Two base vector systems are introduced, the firs one so-called concomitant corresponds to the cotangent fibrtion of the modelling surface while the other is defind on a surface equidistant to the modelling one. The distortion appears as a two-point tensor referred to both base systems after covariant differentiationof the translation vector feld. Thus, two main definition of the strain tensor become possible, the firstone referred to the main basis whereas the second to the concomitant one. Some possible simplificationsof these tensors are considered, and the interrelation between the general theory of A.A. Amosov type and the classical ones is shown. https://ijccse.iasv.ru/index.php/ijccse/article/view/349hierarchical modeling of shells, dimensional reduction, analytical continuum dynamics, strain tensors, stress tensors
collection DOAJ
language English
format Article
sources DOAJ
author Sergey Zhavoronok
spellingShingle Sergey Zhavoronok
ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
International Journal for Computational Civil and Structural Engineering
hierarchical modeling of shells, dimensional reduction, analytical continuum dynamics, strain tensors, stress tensors
author_facet Sergey Zhavoronok
author_sort Sergey Zhavoronok
title ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
title_short ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
title_full ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
title_fullStr ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
title_full_unstemmed ON DIFFERENT DEFINITIONS OF STRAIN TENSORS IN GENERAL SHELL THEORIES OF VEKUA-AMOSOV TYPE
title_sort on different definitions of strain tensors in general shell theories of vekua-amosov type
publisher Publishing House ASV
series International Journal for Computational Civil and Structural Engineering
issn 2587-9618
2588-0195
publishDate 2021-03-01
description Several possible definiions of strains in a general shell theory of I.N. Vekua – A.A. Amosov type are considered. The higher-order shell model is definedon a two-dimensional manifold within a set of fieldvariables of the firstkind determined by the expansion factors of the spatial vector fieldof the translation. Two base vector systems are introduced, the firs one so-called concomitant corresponds to the cotangent fibrtion of the modelling surface while the other is defind on a surface equidistant to the modelling one. The distortion appears as a two-point tensor referred to both base systems after covariant differentiationof the translation vector feld. Thus, two main definition of the strain tensor become possible, the firstone referred to the main basis whereas the second to the concomitant one. Some possible simplificationsof these tensors are considered, and the interrelation between the general theory of A.A. Amosov type and the classical ones is shown.
topic hierarchical modeling of shells, dimensional reduction, analytical continuum dynamics, strain tensors, stress tensors
url https://ijccse.iasv.ru/index.php/ijccse/article/view/349
work_keys_str_mv AT sergeyzhavoronok ondifferentdefinitionsofstraintensorsingeneralshelltheoriesofvekuaamosovtype
_version_ 1721517995419762688