带有刚性边距框架的双层玻璃单元冷弯性能研究

T. V. van Driel, C. Noteboom, M. Overend
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摘要

带有弯曲玻璃的自由形式的面板正变得越来越流行。由于弯曲玻璃提供了更好的抗面外载荷,它可以导致更薄的玻璃。一项很有前途的新技术是将具有刚性结构边缘的薄玻璃板冷弯成双曲抛物面(hypar),并随后锁定角落,以创建一个自包含的自应力系统。在这项研究中,研究了特殊制造的双层玻璃单元(“面板”)的弯曲过程,重点研究了局部不稳定现象。假设这种不稳定性受到板的边缘刚度的影响,通过使用30x30mm GFRP型材作为沿玻璃周长的间隔来测试。这些是用陶氏993有机硅粘合剂粘合到玻璃上的。总共生产了4块1.5 × 1.5米的面板,其中3块采用4mm全钢化(FT)玻璃,另一块采用1.1 mm化学钢化(CT)玻璃。这些板在一系列的实验室实验中被冷弯。建立了一个数值模型,以进一步了解力学响应并预测实验结果。由于所使用的面板的尺寸,不可能形成hypar。由于玻璃的厚度小,当冷弯时,对角线总是会变直。底板在转角位移约150mm,总荷载为2.6 kN时发生断裂,4mm FT板失效。1.1 mm连续油管底板也首先发生断裂,转角位移为120mm,总载荷为1.4 kN。当转角位移约为50毫米时,FT 4毫米面板的顶部和底部板在板的中心接触,而CT 1.1毫米面板的转角位移约为30毫米。数值模型预测了这种接触和面板的整体行为,直到角位移为60毫米。最后得出的结论是,这种玻璃太薄,无法产生这种面板尺寸的超焦。与数值模型一起产生的实验数据对今后的研究和发展是有用的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Investigations on the Cold Bending Behaviour of a Double Glazing Unit with a Rigid Edge-Spacer Frame
Free-form façades with bent glass are becoming increasingly popular. As bending glass provides it with a better resistance to out-of-plane loads, it can result in thinner glass. A promising new technique is to cold bend thin glass plates with a stiff structural edge into a hyperbolic paraboloid (hypar), and to subsequently lock the corners to create a self-contained, self-stressed system. In this study, the bending process of specially-fabricated double glazing units (‘panels’) is investigated with a focus on a local instability phenomenon. The hypothesis that this instability is affected by edge stiffness of the plate, is tested by using 30x30 mm GFRP profiles as spacers along the perimeter of the glass. These were bonded to the glass using Dow 993 silicone adhesive. Four 1.5x1.5 m panels were produced in total, three with 4mm fully toughened (FT) glass, and one with 1.1 mm chemically toughened (CT) glass. The panels were cold bent in a series of laboratory experiments. A numerical model was developed to provide further insight on the mechanical response and to predict the outcome of the experiments. With the sizes of panels used it was not possible to form a hypar. Due to the small thickness of the glass, one the diagonals would always straighten when cold-bent. The 4 mm FT panels failed when the bottom plate fractured at a corner displacement of around 150 mm and a total load of 2.6 kN. The bottom plate of the CT 1.1 mm was also the first to fracture, at a corner displacement of 120 mm and a total load of 1.4 kN. The top and bottom plates came into contact in the centre of the plate when the  corner displacement was around 50 mm for the FT 4 mm panels, and around 30 mm for the CT 1.1 mm panel. The numerical model predicted this contact and the overall behaviour of the panel up to a corner displacement of 60 mm. It was concluded that the glass was too thin to create a hypar with this panel size. The experimental data generated along with the numerical model are useful for future research and developments.  
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