Strengthening of an Edge-Cracked Plate Under Bending Using Piezoelectric Actuators

Sourav Pattanayak, Supriyo Roy, Prasanta Sahoo, Goutam Pohit
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Abstract

Monitoring structural stability and repairing damaged components has grown in importance to ensure the safety and longevity of various engineering structures. This paper presents an innovative method for improving the performance and delaying the failure of edge-cracked plate-like structures by incorporating piezoelectric actuators during bending. The proposed method uses two piezoelectric actuators strategically placed along the plate's surface to create a counter-moment that reduces the severity of the crack. The analytical model was based on well-known stress intensity factor (SIF) solutions for the cracked plate, while the SIF after actuation was calculated with the counter moment produced by the piezoelectric patch. The superposition principle was then used to determine the total SIF after repair. The proposed technique was validated against the ABAQUS-based finite element solutions. SIFs are calculated for various parameters like crack length, patch thickness, and repair voltage. The results demonstrate that the integration of piezoelectric actuators significantly enhances the beam's structural integrity by reducing the SIF. A 21.48% reduced SIF was obtained under 200 V repair voltage for a 5 mm crack length and 0.5 mm patch thickness. Overall, this novel approach offers a promising method for increasing the integrity of cracked structural components, particularly under bending, reducing maintenance costs, and enhancing overall safety.

Abstract Image

弯曲作用下边缘裂纹板的压电强化
监测结构的稳定性和修复受损构件对于保证各种工程结构的安全和寿命越来越重要。本文提出了一种利用压电致动器提高边缘裂纹类板结构弯曲性能并延缓其失效的创新方法。所提出的方法使用两个压电致动器策略性地放置在板的表面,以产生一个反矩,以减少裂纹的严重程度。分析模型基于裂纹板的应力强度因子(SIF)解,而驱动后的SIF是用压电片产生的反矩计算的。然后利用叠加原理确定修复后的总SIF。利用基于abaqus的有限元解对所提出的方法进行了验证。SIFs计算了各种参数,如裂纹长度,补丁厚度和修复电压。结果表明,压电致动器的集成通过减小SIF显著提高了梁的结构完整性。在200 V修复电压下,裂纹长度为5 mm,补片厚度为0.5 mm, SIF降低21.48%。总的来说,这种新方法提供了一种很有前途的方法,可以提高开裂结构部件的完整性,特别是在弯曲下,降低维护成本,提高整体安全性。
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CiteScore
0.70
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