Shear flexible curved spline beam element for static analysis

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Abstract

In this paper, an efficient curved cubic B-spline beam element is developed based on field consistency principle, for the static analysis. The formulation is general in the sense that it includes anisotropy, transverse shear deformation, in-plane and rotary inertia effects. The element is based on laminated beam theory, which satisfies the interface stress and displacement continuity, and has a vanishing shear stress on the top and bottom surfaces of the beam. The lack of consistency in the shear and membrane strain-field interpolations in their constrained physical limits causes poor convergence and unacceptable results due to locking. Hence, numerical experimentation is conducted to check these deficiencies with a series of assumed shear/membrane strain functions, redistributed in a field consistent manner. The performance of the element is assessed by studying the static behavior of a variety of problems ranging from straight beam to circular ring.

Introduction

The application of spline functions in the analysis of problems concerning structural mechanics has emerged to be an exciting area of research in the recent past. Due to their piecewise form, smoothness, capacity to handle local phenomena and higher-order continuity, spline functions offer distinct advantages such as computational efficiency, flexibility to model different boundary conditions, good accuracy and convergence characteristics, and versatility, etc. Among the spline functions, the functions based on B-spline basis, which can have different order of polynomial, is more in usage for the structural analysis.

The study of static and dynamic behavior of various structural elements, using different methods considering B-spline functions, have recently been carried out by many researchers. Some of the important contributions are cited here. Cheung et al. [1] and Cheung and Fan [2], have studied the static problems by employing spline finite strip method whereas finite element technique adopting spline functions has been used in the work of Shik [3] and Gupta et al. [4]. The dynamic characteristics of beams/plates and shells have been analyzed using spline finite point method by Zhou and Li [5]. Furthermore, finite element procedure using spline functions has been attempted for vibration study by Leung and Au [6], and Fan and Luah [7]. It may be observed from the existing literature that most of the available works applying various methods incorporating spline functions for structural analysis are based on the classical theory. It is further apparent from the available research works that the development of spline function based curved beam element has not been attempted, although several works are reported about straight beam, plate, and shell elements having functions based on spline bases.

It is a well-known fact that the classical theory is not suitable for analyzing either thick isotropic structures or even thin composite laminate cases, and therefore, it is more appropriate to analyze such structures by including the effect of shear deformation. However, the application of spline function in conjunction with shear deformation theory has been sparsely treated in the literature [8], [9], [10], [11], [12]. Spline collocation procedure has been adopted in Refs. [8], [9] to solve static problems whereas the vibration characteristics of straight beams and plates have been studied using spline functions in conjunction with Rayleigh–Ritz approach in Refs. [10], [11], [12]. It has been brought out from these studies that these methods yield results of good accuracy for moderately thick beam, plates and shells, but that accuracy of the results deteriorates significantly for thin structures due to shear locking phenomenon. The occurrence of shear locking phenomenon with respect to problems dealing with shear deformation theory in conjunction with B-spline functions has been eliminated by choosing different order of spline functions for the constrained field variables [10], by constructing B-spline displacement field based on the inspection of the Timoshenko beam mode functions [12], and by introducing modified shear modulii [8], [9]. The shear locking behavior in the finite element analysis of beams, plates and shells has been studied by many authors [13], [14], [15], [16], [17] in the context of elements based on conventional polynomial functions for the field variables. The more versatile approach, among the available techniques for alleviating locking such as reduced/selective integration scheme and assumed strain fields, etc., is the field-consistent formulation [16], [17]. It involves systematically eliminating spurious constraints causing shear/membrane locking in shear flexible finite elements. With such an approach, the order of integration required is freed and therefore, exact numerical integration schemes can be employed to evaluate all the strain energy terms. The performance of the elements based on such technique has been proved to be excellent for both thick and thin situations. An attempt is made here to develop a field-consistent shear-flexible curved beam element, adopting spline basis functions for the static analysis.

In this paper, we examine the cubic B-spline element from the point of view of field consistency to find the optimal assumed membrane/shear strain functions that will eliminate locking phenomena. The performance of the element is tested for static analysis of beams considering a number of problems. The results are compared, wherever possible, with the available analytical solutions.

Section snippets

Formulation based on laminated beam theory

A laminated composite beam, having radius of curvature R, is considered with the coordinates x along the axis of the beam and z along the thickness direction, respectively. The displacements in kth layer, uk and w at point (x,z) from the median surface are expressed as functions of mid-plane displacement u0 and w and independent rotation θ of the normal in xz plane, asuk(x,z)=u0(x)(1+z/R)−zw,x(x)+[f(z)+gk(z)](w,x(x)+θ(x)),w(x,z)=w(x).The functions f(z) and gk(z) are defined asf(z)=t/πsin(π

Curved cubic B-spline beam element

A beam element is assumed to be having q equal sections. The spline function adopted to represent the three field variables u0, w and θ is the cubic B-spline of equal section length (h), and is given as (Fig. 1)u0=i=−1q+1αiϕ0i,w=i=−1q+1βiϕ0i,θ=i=−1q+1γiϕ0i,in which each local cubic B-spline ϕ0i has non-zero values over four consecutive sections with the section-knot x=xi as the centre, and is defined asϕ0i=16h30,x<xi−2,(x−xi−2)3,xi−2⩽x⩽xi−1,h3+3h2(x−xi−1)+3h(x−xi−1)2−3(x−xi−1)3,xi−1⩽x⩽xi,h3

Numerical experiments

Numerical computation is carried out for the rank of the element and it has three proper zero values, and thus, does not produce any spurious mode. Further, for the critical evaluation of the present formulation, a series of test examples is considered to check the convergence properties and locking behavior. The element variations chosen for the study are the different functions for the redistributed strain fields through the field consistent strategy.

Conclusions

The shear-membrane locking phenomena in the shear flexible curved element based on cubic B-spline functions for the displacement fields have been analyzed using the field-consistency approach. The field-consistent redistribution of membrane and shear strain fields at the lowest level yields the accurate results for both fairly thick and extremely thin beams by using the full integration scheme for the evaluation of all the strain energy terms. The capabilities and effectiveness of the element

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