2020
DOI: 10.1134/s1995080220100078
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Weak Solutions within the Gradient-Incomplete Strain-Gradient Elasticity

Abstract: In this paper we consider existence and uniqueness of the three-dimensional static boundary-value problems in the framework of so-called gradient-incomplete strain-gradient elasticity. We call the straingradient elasticity model gradient-incomplete such model where the considered strain energy density depends on displacements and only on some specific partial derivatives of displacements of first-and second-order. Such models appear as a result of homogenization of pantographic beam lattices and in some physic… Show more

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Cited by 11 publications
(8 citation statements)
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“…In this paper we will fully investigate the new boundary condition (14) for the classical Mindlin-Eringen micromorphic model. We will show existence and uniqueness under this weaker requirement, we will derive the missing normal Neumann-type condition on the Dirichlet boundary Γ for the third order moment stress tensor m DP and we will compare analytical solutions for (12) versus (14). This allows us to better understand the different Dirichlet conditions on P (which both lead to existence and uniqueness).…”
Section: The Classical Mindlin-eringen Micromorphic Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…In this paper we will fully investigate the new boundary condition (14) for the classical Mindlin-Eringen micromorphic model. We will show existence and uniqueness under this weaker requirement, we will derive the missing normal Neumann-type condition on the Dirichlet boundary Γ for the third order moment stress tensor m DP and we will compare analytical solutions for (12) versus (14). This allows us to better understand the different Dirichlet conditions on P (which both lead to existence and uniqueness).…”
Section: The Classical Mindlin-eringen Micromorphic Modelmentioning
confidence: 99%
“…The variations δP in the bulk and at the boundary are independent, therefore δF The second gradient linearized elasticity model (without mixed terms) reads (see for example [12,13,14,15,16,17,26,39,49,64])…”
Section: Boundary Conditions In the Relaxed Micromorphic Modelmentioning
confidence: 99%
“…Pantographic structures have been intensively studied in recent years [1][2][3][4][5][6] because of their peculiar behavior, consisting of two main features within the family of lightweight structures: (1) the capability to exploit large deformations in the elastic regime; (2) hierarchical behavior in the damage mechanisms. The research lines can be roughly classified into those devoted to the analysis of theoretical aspects [7][8][9][10][11][12], to the formulation of computational methods in discrete [13][14][15][16] and continuum framework [17][18][19][20], as well as to the investigations of experimental evidence [21][22][23][24][25][26][27]. The genesis in conceiving the pantographic sheet can be traced back in the grounding idea of non-local materials, and in particular of second or higher gradient theories [28][29][30][31][32][33][34][35][36][37], in which the constitutive law is a function also of the second or higher gradient of the displacement field.…”
Section: Introductionmentioning
confidence: 99%
“…Through a homogenization procedure [60], the behavior of the structure is estimated by the reduced‐order model [61, 62]. The existence and uniqueness of weak solutions for linear pantographic structures is presented in [63, 64]. The wave dispersion in nonlinear pantographic beams has been studied [65].…”
Section: Introductionmentioning
confidence: 99%