Abstract

High levels of strength- and stiffness-to-mass ratio can be achieved in slender structures by lengthwise tailoring of their cross-sectional areas. During use, a non-prismatic beam element can be subject to surface forces or loads acting on only a part of their cross-section. Practical examples involve tapered aircraft wings, wind turbine and helicopter rotor blades under fluid pressure and shear forces; arched beams in bridges subject to vehicular traction forces and tensile stresses in tendons of prestressed concrete. Presently, beam theories generalise the external loads to the entire cross-sectional area. However, this technique does not accurately describe surface-load boundary conditions and beams under partial cross-sectional loads. Hence, an efficient analytical plane-stress recovery methodology is introduced in the present study that generalises the external load to a specific sub-area of the cross-section of homogeneous non-prismatic beams with one plane of symmetry. As a result, the transverse stress components become piecewise distributions, i.e. non-smooth but continuous in the thickness direction. Additional novelties include the boundary equilibrium recovered considering applied surface loads and terms up to second-order derivatives of the internal forces to define the transverse stress field. Closed-form solutions for the specific case of non-prismatic beams with a rectangular cross-section loaded both on top and bottom surfaces are presented. For validation purposes, different numerical examples are modelled with results compared to solid-like finite element analyses as well with relevant analytical theories. The results show that the developed formulation predicts the stress field in non-prismatic beams under surface forces and non-uniform loads applied to a part of the cross-sectional area with goods levels of accuracy. The error associated with the proposed method escalates with the taper angle, such that a 10° taper angle could result in a 6% error at the surfaces and reduced values for interior zones, while the analytical state-of-the-art models were not able to predict the transverse stresses correctly.

Highlights

  • Non-prismatic beam structures, referred to tapered and variable cross-section beams, are employed in several engineering applications due to their excellent structural efficiency

  • It is important to mention that during an early design stage practitioners tend to model prestressed concrete beams as homogeneous materials and consider the external load to be uniformly distributed through the entire cross-sectional area, while the current formulation captures the influence of the in-plane tendon geometry on the stress field

  • A stress-recovery procedure to predict the stress field of homoge­ neous, untwisted non-prismatic beams that are symmetric about a plane formed by the longitudinal and transverse axes, has been derived

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Summary

Introduction

Non-prismatic beam structures, referred to tapered and variable cross-section beams, are employed in several engineering applications due to their excellent structural efficiency. To perform stress analysis in such slender structures using beam theories, practitioners tend to assume that the external load is uniformly distributed through the entire beam crosssection [4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25] This hypothesis, is unrealistic for beams with surface and body forces acting over only partial cross-sectional areas, which represents practical problems in applications, such as beams subject to pressure loads. Up-to-date studies concerning non-prismatic beams subject to surface forces are limited to specific taper shape or taper only in the width direction [42,45,46,47,48] These shortcomings encourage engineers to model such problems using solid-like finite element analysis to obtain desired levels of accuracy.

Equilibrium equations
Stress distribution
Shear stress
Transverse direct stress
Closed-form solutions
Numerical examples
Double-tapered beam
Linearly tapered beam
Arched beam
Trapezoidal cross-section beam
Findings
Conclusion
Full Text
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