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On the Application of Beam on Elastic Foundation Theory to the Analysis of Stiffened Plate Strips

机译:梁在弹性地基理论上在加筋板条分析中的应用

摘要

The main objective of this thesis is to show that plate strips subjected to transverse line loads can be analysed by using the beam on elastic foundation (BEF) approach. It is shown that the elastic behaviour of both the centre line section of a semi infinite plate supported along two edges, and the free edge of a cantilever plate strip can be accurately predicted by calculations based on the two parameter BEF theory. The transverse bending stiffness of the plate strip forms the foundation. The foundation modulus is shown, mathematically and physically, to be the zero order term of the fourth order differential equation governing the behaviour of BEF, whereas the torsion rigidity of the plate acts like pre tension in the second order term. Direct equivalence is obtained for harmonic line loading by comparing the differential equations of Levy's method (a simply supported plate) with the BEF method. By equating the second and zero order terms of the semi infinite BEF model for each harmonic component, two parameters are obtained for a simply supported plate of width B: the characteristic length, 1/ λ, and the normalized sum, n, being the effect of axial loading and stiffening resulting from the torsion stiffness, nlin. This procedure gives the following result for the first mode when a uniaxial stress field was assumed (ν = 0): 1/λ = √2B/π and nlin = 1. For constant line loading, which is the superimposition of harmonic components, slightly differing foundation parameters are obtained when the maximum deflection and bending moment values of the theoretical plate, with v = 0, and BEF analysis solutions are equated: 1 /λ= 1.47B/π and nlin. = 0.59 for a simply supported plate; and 1/λ = 0.99B/π and nlin = 0.25 for a fixed plate. The BEF parameters of the plate strip with a free edge are determined based solely on finite element analysis (FEA) results: 1/λ = 1.29B/π and nlin. = 0.65, where B is the double width of the cantilever plate strip. The stress biaxial, v > 0, is shown not to affect the values of the BEF parameters significantly the result of the geometric nonlinearity caused by in plane, axial and biaxial loading is studied theoretically by comparing the differential equations of Levy's method with the BEF approach. The BEF model is generalised to take into account the elastic rotation stiffness of the longitudinal edges. Finally, formulae are presented that take into account the effect of Poisson's ratio, and geometric non linearity, on bending behaviour resulting from axial and transverse inplane loading. It is also shown that the BEF parameters of the semi infinite model are valid for linear elastic analysis of a plate strip of finite length. The BEF model was verified by applying it to the analysis of bending stresses caused by misalignments in a laboratory test panel. In summary, it can be concluded that the advantages of the BEF theory are that it is a simple tool, and that it is accurate enough for specific stress analysis of semi infinite and finite plate bending problems.
机译:本文的主要目的是表明可以通过使用弹性地基上的梁(BEF)方法来分析承受横向线荷载的板条。结果表明,通过基于两个参数的BEF理论计算,可以精确地预测沿两个边缘支撑的半无限板的中心线部分和悬臂板带的自由边缘的弹性行为。板条的横向弯曲刚度构成基础。基础模量在数学上和物理上都显示为控制BEF行为的四阶微分方程的零阶项,而板的扭转刚度在第二阶项中的作用类似于预拉伸。通过将Levy方法(简单支撑板)的微分方程与BEF方法进行比较,可以得出谐波线负载的直接当量。通过将半无限BEF模型的第二阶和零阶项等同于每个谐波分量,可以得到宽度为B的简单支撑板的两个参数:特征长度1 /λ和归一化和n(即效应)扭转刚度nlin引起的轴向载荷和刚度的变化。在假定单轴应力场(ν= 0)的情况下,对于第一模式,此过程给出以下结果:1 /λ=√2B/π且nlin =1。对于恒定线负载,这是谐波分量的叠加,略当理论板的最大挠度和弯矩值(v = 0)和BEF分析解决方案等效为:1 /λ= 1.47B /π和nlin时,可获得不同的基础参数。对于简单支撑的板= 0.59;对于固定板,1 /λ= 0.99B /π,nlin = 0.25。具有自由边缘的板带的BEF参数仅基于有限元分析(FEA)结果确定:1 /λ= 1.29B /π和nlin。 = 0.65,其中B是悬臂板带的两倍宽度。研究表明,通过将Levy方法的微分方程与BEF方法进行比较,理论上研究了平面,轴向和双轴载荷引起的几何非线性的结果,表明双轴应力v> 0不会显着影响BEF参数的值。 。 BEF模型被普遍考虑到纵向边缘的弹性旋转刚度。最后,给出了考虑泊松比和几何非线性对轴向和横向平面内载荷产生的弯曲行为的影响的公式。还表明,半无限模型的BEF参数对于有限长度的板条的线性弹性分析有效。通过将BEF模型应用于实验室测试面板中因未对准而引起的弯曲应力的分析,验证了该模型。总之,可以得出的结论是,BEF理论的优点在于它是一种简单的工具,并且对于半无限和有限板弯曲问题的比应力分析而言,它足够准确。

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    Partanen Teuvo;

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  • 年度 1999
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