Matches in SemOpenAlex for { <https://semopenalex.org/work/W2074983168> ?p ?o ?g. }
- W2074983168 endingPage "885" @default.
- W2074983168 startingPage "873" @default.
- W2074983168 abstract "The aim of this paper is to develop the governing equations for a fully constrained finitely deforming hyperelastic Cosserat continuum where the directors are constrained to rotate with the body rotation. This is the generalization of small deformation couple stress theories and would be useful for developing mathematical models for an elastic material with embedded stiff short fibers or inclusions (e.g., materials with carbon nanotubes or nematic elastomers, cellular materials with oriented hard phases, open cell foams, and other similar materials), that account for certain longer range interactions. The theory is developed as a limiting case of a regular Cosserat elastic material where the directors are allowed to rotate freely by considering the case of a high “rotational mismatch energy”. The theory is developed using the formalism of Lagrangian mechanics, with the static case being based on Castigliano's first theorem. By considering the stretch U and the rotation R as additional independent variables and using the polar decomposition theorem as an additional constraint equation, we obtain the governing and as well as the boundary conditions for finite deformations. The resulting equations are further specialized for plane strain and axisymmetric finite deformations, deformations of beams and plates with small strain and moderate rotation, and for small deformation theories. We also show that the boundary conditions for this theory involve “surface tension” like terms due to the higher gradients in the strain energy function. For beams and plates, the rotational gradient dependent strain energy does not require additional variables (unlike Cosserat theories) and additional differential equations; nor do they raise the order of the differential equations, thus allowing us to include a material length scale dependent response at no extra “computational cost” even for finite deformation beam/plate theories" @default.
- W2074983168 created "2016-06-24" @default.
- W2074983168 creator A5083314175 @default.
- W2074983168 creator A5088110497 @default.
- W2074983168 date "2013-03-01" @default.
- W2074983168 modified "2023-09-29" @default.
- W2074983168 title "A model for a constrained, finitely deforming, elastic solid with rotation gradient dependent strain energy, and its specialization to von Kármán plates and beams" @default.
- W2074983168 cites W1970603318 @default.
- W2074983168 cites W1971013052 @default.
- W2074983168 cites W1978145689 @default.
- W2074983168 cites W1979480695 @default.
- W2074983168 cites W1982728423 @default.
- W2074983168 cites W1997063453 @default.
- W2074983168 cites W1998494366 @default.
- W2074983168 cites W2008855763 @default.
- W2074983168 cites W2014112194 @default.
- W2074983168 cites W2015082159 @default.
- W2074983168 cites W2023338094 @default.
- W2074983168 cites W2023579973 @default.
- W2074983168 cites W2027880021 @default.
- W2074983168 cites W2029325129 @default.
- W2074983168 cites W2030972504 @default.
- W2074983168 cites W2041593217 @default.
- W2074983168 cites W2042682843 @default.
- W2074983168 cites W2047558462 @default.
- W2074983168 cites W2052710166 @default.
- W2074983168 cites W2059668248 @default.
- W2074983168 cites W2063591045 @default.
- W2074983168 cites W2063882799 @default.
- W2074983168 cites W2065667277 @default.
- W2074983168 cites W2073811122 @default.
- W2074983168 cites W2091418685 @default.
- W2074983168 cites W2091727318 @default.
- W2074983168 cites W2116462892 @default.
- W2074983168 cites W2122323682 @default.
- W2074983168 cites W2138857297 @default.
- W2074983168 cites W2162818592 @default.
- W2074983168 cites W2169504835 @default.
- W2074983168 doi "https://doi.org/10.1016/j.jmps.2012.10.008" @default.
- W2074983168 hasPublicationYear "2013" @default.
- W2074983168 type Work @default.
- W2074983168 sameAs 2074983168 @default.
- W2074983168 citedByCount "65" @default.
- W2074983168 countsByYear W20749831682013 @default.
- W2074983168 countsByYear W20749831682014 @default.
- W2074983168 countsByYear W20749831682015 @default.
- W2074983168 countsByYear W20749831682016 @default.
- W2074983168 countsByYear W20749831682017 @default.
- W2074983168 countsByYear W20749831682018 @default.
- W2074983168 countsByYear W20749831682019 @default.
- W2074983168 countsByYear W20749831682020 @default.
- W2074983168 countsByYear W20749831682021 @default.
- W2074983168 countsByYear W20749831682022 @default.
- W2074983168 crossrefType "journal-article" @default.
- W2074983168 hasAuthorship W2074983168A5083314175 @default.
- W2074983168 hasAuthorship W2074983168A5088110497 @default.
- W2074983168 hasConcept C121332964 @default.
- W2074983168 hasConcept C121854251 @default.
- W2074983168 hasConcept C134306372 @default.
- W2074983168 hasConcept C135628077 @default.
- W2074983168 hasConcept C14041564 @default.
- W2074983168 hasConcept C147370603 @default.
- W2074983168 hasConcept C159985019 @default.
- W2074983168 hasConcept C163892269 @default.
- W2074983168 hasConcept C182310444 @default.
- W2074983168 hasConcept C192562407 @default.
- W2074983168 hasConcept C199201527 @default.
- W2074983168 hasConcept C20192703 @default.
- W2074983168 hasConcept C2524010 @default.
- W2074983168 hasConcept C29320194 @default.
- W2074983168 hasConcept C33026886 @default.
- W2074983168 hasConcept C33923547 @default.
- W2074983168 hasConcept C57879066 @default.
- W2074983168 hasConcept C62520636 @default.
- W2074983168 hasConcept C64904818 @default.
- W2074983168 hasConcept C74650414 @default.
- W2074983168 hasConcept C84035572 @default.
- W2074983168 hasConcept C97355855 @default.
- W2074983168 hasConceptScore W2074983168C121332964 @default.
- W2074983168 hasConceptScore W2074983168C121854251 @default.
- W2074983168 hasConceptScore W2074983168C134306372 @default.
- W2074983168 hasConceptScore W2074983168C135628077 @default.
- W2074983168 hasConceptScore W2074983168C14041564 @default.
- W2074983168 hasConceptScore W2074983168C147370603 @default.
- W2074983168 hasConceptScore W2074983168C159985019 @default.
- W2074983168 hasConceptScore W2074983168C163892269 @default.
- W2074983168 hasConceptScore W2074983168C182310444 @default.
- W2074983168 hasConceptScore W2074983168C192562407 @default.
- W2074983168 hasConceptScore W2074983168C199201527 @default.
- W2074983168 hasConceptScore W2074983168C20192703 @default.
- W2074983168 hasConceptScore W2074983168C2524010 @default.
- W2074983168 hasConceptScore W2074983168C29320194 @default.
- W2074983168 hasConceptScore W2074983168C33026886 @default.
- W2074983168 hasConceptScore W2074983168C33923547 @default.
- W2074983168 hasConceptScore W2074983168C57879066 @default.
- W2074983168 hasConceptScore W2074983168C62520636 @default.
- W2074983168 hasConceptScore W2074983168C64904818 @default.
- W2074983168 hasConceptScore W2074983168C74650414 @default.