2015
DOI: 10.1007/s00466-015-1188-4
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8-Node solid-shell elements selective mass scaling for explicit dynamic analysis of layered thin-walled structures

Abstract: To overcome the issue of spurious maximum eigenfrequencies leading to small steps in explicit time integration, a recently proposed selective mass scaling technique, specifically conceived for 8-node hexahedral solid-shell elements, is reconsidered for application to layered shells, where several solid-shell elements are used through the thickness of thin-walled structures.In this case, the resulting scaled mass matrix is not perfectly diagonal. However, the introduced coupling is shown to be limited to the no… Show more

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Cited by 6 publications
(4 citation statements)
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“…A solid-shell finite element discretization is adopted, by using the element proposed in [15] and successive modifications (in particular we use the selective mass scaling described in [3] and [4]). In the paper we assume the following numbering for the reference element: since the thickness is small, it is always possible to identify nodes 1-4 for the lower surface, and nodes 5-8 for the upper surface.…”
Section: Formulationmentioning
confidence: 99%
“…A solid-shell finite element discretization is adopted, by using the element proposed in [15] and successive modifications (in particular we use the selective mass scaling described in [3] and [4]). In the paper we assume the following numbering for the reference element: since the thickness is small, it is always possible to identify nodes 1-4 for the lower surface, and nodes 5-8 for the upper surface.…”
Section: Formulationmentioning
confidence: 99%
“…The static, free vibration and crack propagation for detecting the failure behaviours are investigated (Nguyen-Thanh et al, 2018;Li et al, 2020;Huang et al, 2022). Currently, the conventional thin shell theory (Fluegge, 1973;Love, 2013;Tzou and Howard, 1994), which is based on the Kirchhoff-Love hypothesis ignoring transverse shear deformation, is often used to study shell problems (Confalonieri et al, 2015;Kiendl et al, 2009;Zukas, 1974;Zareh and Qian, 2018;Creaghan and Palazotto, 1994), and for shell structures with small shear stiffness (i.e. prone to significant transverse shear deformation), certain errors will be introduced (Hansbo and Larson, 2011;Repin and Sauter, 2010;Weise, 2018;Rychter, 1988).…”
Section: Introductionmentioning
confidence: 99%
“…, 2022). Currently, the conventional thin shell theory (Fluegge, 1973; Love, 2013; Tzou and Howard, 1994), which is based on the Kirchhoff–Love hypothesis ignoring transverse shear deformation, is often used to study shell problems (Confalonieri et al. , 2015; Kiendl et al.…”
Section: Introductionmentioning
confidence: 99%
“…Shells are categorised according to their radius-to-thickness ratio, as defined in Table 1. To date, research into shell vibration has focused predominantly on thin shells, based on the classical theory of thin shells (Donnell, 1933; Sanders and Lyell, 1959; Fluegge, 1973; Love, 2013) while ignoring transverse shear deformations (Love, 2013; Confalonieri et al , 2015). However, practical engineering situations often involve thicker plate and shell structures that lie beyond the application scope of this theory.…”
Section: Introductionmentioning
confidence: 99%