1980
DOI: 10.2208/jscej1969.1980.304_17
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Mechanics in Geometrically Nonlinear Problem of Discrete System and Application to Plane Frame-Works

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Cited by 14 publications
(8 citation statements)
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“…(5)- (7)= 291.9cm<leff (8)-(1O)=568.4cm. This result is contrary to the followings: since member (8) to (10) have a bending rigidity four times larger than other column members, as well as clamped at their lower ends, they shall have larger buckling strengths than member (5) to (7). In Example (3), a numerical result has been given for a vertical P applied at node 2 only.…”
Section: Discussionmentioning
confidence: 86%
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“…(5)- (7)= 291.9cm<leff (8)-(1O)=568.4cm. This result is contrary to the followings: since member (8) to (10) have a bending rigidity four times larger than other column members, as well as clamped at their lower ends, they shall have larger buckling strengths than member (5) to (7). In Example (3), a numerical result has been given for a vertical P applied at node 2 only.…”
Section: Discussionmentioning
confidence: 86%
“…[8] . In that study, after an exact separation of nodal displacements of a beam element into its displacement as a rigid body and its deformation, the stiffness relations are developed by the perturbation method up to the third order of deformation parameters.…”
Section: Numerical Analysismentioning
confidence: 99%
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“…In the Cartesian {x, y}, let us consider a threenode triangular element (e). The spatial coordinates of its three nodes are employed as the element position {x} (e)={(x, y) i, (x, y), (x, y) k} (1) where i < j < k. As the element coordinate system, we take {x', y'} in relation to the current configuration such that x' is directed from node i toward j with y' being perpendicular to x'. As well, in the initial (or stress-free) state, the {x', y'} of material points are employed as Lagrangian coordinates {S ri}:S=xo, ij=yo, where an initial quantity is denoted by subscript ()o.…”
Section: Description Of Geometry and Strainmentioning
confidence: 99%
“…In this paper, another formulation is presented for the 2-D triangular element, with a full physical explanation, which is developed explicitly in a complete accordance with an exisiting general procedure stated in Ref. 1,2) to separate the total freedom of an element into the parameters of position as a rigid and those of deformation. By the assumption of an elastic strain energy existing even for finite strains, the realistic material problems are disregarded, but the expansion classified into the total-Lagrangian is theoretical and rigorous as a geometrically nonlinear discretization.…”
Section: Introductionmentioning
confidence: 99%