2009
DOI: 10.1016/j.ijsolstr.2009.03.019
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Does generalized elastica lead to bimodal optimal solutions?

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Cited by 4 publications
(5 citation statements)
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“…First we note that when j ¼ 0 and k 1 ¼ 0, we recover the optimality condition for the Pflüger beam posed in the sense of the classical Bernoulli-Euler elastica theory (see Atanackovic and Simic, 1999). Secondly, the influence of nonlocal theory as well as the generalization of the classical elastica theory shown in Spasic and Glavardanov (2009), lead to a complicated two point boundary value problem since the optimality conditions are given in complex form. Namely, in both cases the posed boundary value problems require the solution of a cubic or quadratic equation.…”
Section: Optimization Problem and Its Solutionmentioning
confidence: 65%
See 1 more Smart Citation
“…First we note that when j ¼ 0 and k 1 ¼ 0, we recover the optimality condition for the Pflüger beam posed in the sense of the classical Bernoulli-Euler elastica theory (see Atanackovic and Simic, 1999). Secondly, the influence of nonlocal theory as well as the generalization of the classical elastica theory shown in Spasic and Glavardanov (2009), lead to a complicated two point boundary value problem since the optimality conditions are given in complex form. Namely, in both cases the posed boundary value problems require the solution of a cubic or quadratic equation.…”
Section: Optimization Problem and Its Solutionmentioning
confidence: 65%
“…Note that generalizations of the classical elastica theory, like the one at hand, lead to more complicated two point boundary value problems since optimality conditions are given in the form of polynomials. For example, see Spasic and Glavardanov (2009) where the posed boundary value problem requires a solution of the cubic equation and where its explicit solution, that determines optimal shape, was shown in terms of the Chebishev radicals. Thus, in obtaining a numerical solution that determines the optimal shape of a micro/nano beam for given arc length, in each iteration one solve the depressed quartic equation explicitly by the use of Ferrari's method.…”
Section: Introductionmentioning
confidence: 99%
“…From ( 30), (31) and [16], p.4, we conclude that 𝑓 is contact equivalent to 𝑓 given below, that is, the terms of the order 𝑂(𝑎 3 Δ𝜆, 𝑎Δ𝜆 2 , 𝑎 5 ) may be neglected in the analysis of number of solution of (29). Therefore, we analyze only…”
Section: 𝔽(𝜆 𝜑) = 𝔹(𝜆)𝜑 + ℕ(𝜆 𝜑)mentioning
confidence: 92%
“…This theory represents one of two approaches to the mathematical rod theory and it identifies the rod with the axis of the rod. For details of derivation see [4] p. 45, or [5]. Assume that the rod axis in the undeformed state coincides with the x axis of the rectangular coordinate system xy$x-y$.…”
Section: Introductionmentioning
confidence: 99%
“…In order to solve more complex problems of plane elastica i.e. problems with different constitutive axioms and different load, engineering communities are still interested in efficient methods for solving both linear and nonlinear differential equations, see [2][3][4][5][6][7][8]. Recently, due to an enormous and wide-spread availability of computational power one more efficient method was added to the list, see [9] where the Laplace transform and the method of successive approximations (LT&MSA for short), was used in finding the analytical approximative solutions describing Toda oscillators …”
Section: Introductionmentioning
confidence: 99%