用Rayleigh-Ritz, Abaqus和实验对厚双稳态碳纤维层压板的功能描述

Christopher H. Knippenberg, O. Myers, Christopher Nelon
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引用次数: 0

摘要

以[0i, 90i], i > 0的不对称铺层方向构建的复合材料层压板具有两个稳定的平衡位置,并且可以被驱动从初级固化形状转变为反向相关的次级稳定形状。本研究旨在通过先前建立的分析方法和实验验证,帮助开发厚双稳层压板的全面描述,其增加的厚度有失去双稳性的风险。将最小势能原理应用于两种材料,采用瑞利-里兹最小化技术对AS4/8552和TR50S-12k碳纤维复合材料层合板的固化形状进行了分析。这些材料被建模为边长可达0.914m的方形厚双稳态层合复合材料。面外位移的可视化显示与瑞利-里兹分析的描述。此外,利用Abaqus CAE 6.14软件建立有限元模型,并利用DA409/G35和TR50S-12K/NP301预浸料进行实验,进一步从双稳损失、驱动载荷和原理形状等方面对厚双稳层压板进行了基本描述和发展。该解析模型是Hyer(2002)和Mattioni(2009)对厚双稳态层压板的扩展,其中主要假设分别是主稳定位置和次稳定位置的x轴曲率等于负y轴曲率。这一假设导致了已经得到证实的结论,即双稳态层叠板一旦固化,就会呈现出两种相反的抛物面形状之一。有限元模拟与此相矛盾,显示了上述形状的平均11%的曲率大小差异。此外,四阶多项式被用来描述沿轴的曲率,不同于以前使用的门格尔曲率(三点近似)。利用峰值挠度和平均曲率绘制的分岔图清楚地表明,双稳性存在于约50层;然而,能量景观样地表明,从36层开始,双稳定性显著下降。实验在一个试验台上进行,在施加中心面外载荷的情况下,模拟了有限元分析中使用的相同边界条件。实验观察表明,稳定固化形状的峰值位移减小。观察还表明,与负y轴曲率相比,x轴曲率的幅度有显著差异。然而,双稳性的存在与FEA能量景观图一致,在28-36层的厚度处有明显的“断裂”。此外,驱动力与有限元模拟结果有很好的相关性。临界点的差异可归因于DA409和TR50S-12K的材料性能差异,未能捕获聚合物弛豫,实验设置的局限性以及手工铺层制造错误。最后,本文增加了在宏观尺度应用中使用较厚层压板的可行性,在这些应用中,形状变形或形状保持属性是必要的约束,尽管只有在预期低载荷的情况下。
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Functional Description for Thick Bistable Carbon Fiber Laminates With Rayleigh-Ritz, Abaqus, and Experiments
Composite laminates constructed in an asymmetric layup orientation of [0i, 90i], i > 0, exhibit two stable equilibrium positions and may be actuated to snap from a primary cure shape to an inversely related secondary stable shape. This study aims to aid in developing a comprehensive description of thick bistable laminates, whose increased thickness risks the loss of bistability, through previously established analytical approaches and verification via experimentation. The principle of minimum potential energy is applied to two materials and analyzed using the Rayleigh-Ritz minimization technique to determine the cure shapes of carbon fiber reinforced polymer laminates composed of AS4/8552 and TR50S-12k carbon fibers. These materials were modeled to act as square thick bistable laminated composites with sidelengths up to 0.914m. Visualizations of the out-of-plane displacements are shown with a description of the Rayleigh-Ritz analysis. Additionally, a finite element model (FEM) created in Abaqus CAE 6.14 and experiments using DA409/G35 and TR50S-12K/NP301 prepreg were used to further describe and develop the fundamental description for thick bistable laminates in terms of loss of bistability, actuation load, and principle shape. The analytical model is an extension of Hyer’s (2002) and Mattioni’s (2009) work applied to thick bistable laminates where the primary assumption was the x-axis curvature equaled the negative y-axis curvature for the primary and secondary stable positions, respectively. This assumption leads to the already cemented conclusion that bistable laminates, once cured, take on one of two inversely related paraboloid shapes. FEA simulations contradicted this by showing an average 11% difference in curvature magnitude for the aforementioned shapes. Furthermore, fourth order polynomials were used to describe the curvature along the axes, differing from the previously used Menger curvatures, (three-point approximation). Bifurcation plots using peak deflections and average curvature generated from FEA simulations clearly showed bistability existed to approximately 50 plies; however, the energy landscape plots indicated a significant degradation of bistability starting at 36 plies. Experimentation was performed on a test stand mimicking the same boundary conditions used in FEA while applying a central out-of-plane load. Experimental observations showed decreased peak displacements of stable cure shapes. Observations also indicated that the x-axis curvature had a significant difference in magnitude compared to the negative y-axis curvature. However, the existence of bistability agreed with FEA energy landscape plots, with clear “snaps” ending at thicknesses of 28–36 plies. Moreover, actuation force was found to correlate well with FEA simulations. Differences in the critical point can be attributed to the combination of material property differences for DA409 and TR50S-12K, failure to capture polymer relaxation, limitations of the experimental setup, and hand layup fabrication errors. Lastly, this paper adds viability of thicker laminates for use in macroscale applications where shape morphing or shape-retention attributes are a necessary constraint, although only where low loads are expected.
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