碳纤维增强聚合物(CFRP)外壳多物理场冲击分析

H. Khawaja, M. Moatamedi, Z. Andleeb, C. Strand, P. Chen, B. Guo
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The experimental studies were performed and compared against finite element simulations using ANSYS®. The studies also included layering of the CFRP samples to find the limiting thickness of pellets penetration. It was concluded that the thickness of 0.79mm and below of CFRP, cannot resist the impact of pellets. The visual inspection of failure revealed that the CFRP has gone through a brittle failure. However, temperature was found to have no significant impact on the results as similar behavior of CFRP was observed in both room conditions (22°C) and cold temperatures (-28°C). Introduction In the last decades, a growing interest has been dedicated in the use of composite materials for structural applications. CFRP composites are gaining a special attention to replace traditional materials in several fields although it is well known that these systems are highly susceptible to internal damage caused by transverse loads even under low-velocity ones [1,2]. In general, CFRP composites can be damaged on the surface and also beneath the surface by relatively light impacts causing invisible impact damage [3]. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Operative conditions affect the material properties as reported in [4-6]. Experimental Setup a. Test Samples Test samples used in this study were from the DragonPlate®, manufactured by Allred and Associates Inc., Elbridge, New York [7]. The CFRP samples used were EconomyPlateTM Solid Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 116 Carbon Fiber Sheet ~ 1/32\" x 12\" x 12\" (0.79375mm x 304.8mm x 304.8mm) [8]. EconomyPlateTM sheets comprised of orthotropic (non-quasi-isotropic) at 0°/90° orientation laminates [9] (Figure 1.) utilizing a twill weave [10] (Figure 2.), while maintaining a symmetrical and balanced laminate. EconomyPlateTM composed entirely of a tough and rigid carbon reinforced epoxy matrix, with textured finish on both sides. Samples were cut into smaller pieces for test purposes (Figure 3.). Figure 1-0°/90° orientation laminate Figure 2-Carbon fiber twill weave Figure 3-CFRP test samples b. Impact Tests To perform the impact tests, a shooting box was built, as shown in Figure 4a. The shooting box was designed such that it collects the pallets once they pass through the samples. The box consists of an opening-closing system with locking screws and wingnuts, so test pieces could be fastened for testing (Figure 4b), and removed and replaced with new test pieces effectively. Diabolo and storm pellets (Figures 5 and 6.) were shot on to the CFRP test samples. The material of both pellets was lead and they were of 4.5mm caliber, weighing about 0.5g each. The test was performed in room temperature, on tempered test pieces at about 22°C and in the cold room on test pieces exposed to about -28 ̊C for 7 days. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 117 (a) Shooting box (b) Fastened test piece Figure 4 – The opening-closing system of the shooting box Figure 5-Diabolo pellets Figure 6-Storm pellets A speed tests were carried out using a high-speed camera (Figure 7.). The test showed the pellets speed of about 160m/s. Figure 7-Speed test of Diabolo pellet (pellet speed ~ 160m/s) Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 118 Experimental Results Impact tests revealed that diabolo and storm pellets at 160m/s pass through the single layer (~0.79 mm) of CFRP (Figure 8). Visual inspection showed that the CFRP test samples were ruptured (brittle failure) and the failure was in the close vicinity of the impact. Ruptured holes were more visible when Storm pellets were used, nonetheless, the failure areas were the same. (a) Diabolo pellets (b) Storm pellets Figure 8-Visual inspection of the impact Tests were repeated by tightly joining the layers of CFRP tests samples (0.79mm, 1.59mm, and 2.38mm). Pellets passed through 0.79mm and 1.59mm thick CFRP test samples, however, deflected for 2.38mm layer. Same results were observed when tests were conducted at room temperature conditions (22°C) and cold conditions (-28°C). Simulations Setup The simulations were performed in ANSYS® Explicit Dynamic [11]. Mesh sensitivity analysis was performed to ensure the accuracy of results. The model parameters are given in Table 1. Table 1: Simulation model parameters (ANSYS® Explicit Dynamic) Physics preference Explicit Relevance 70 Relevance Center Fine Span Angle Center Fine Nodes (optimized) 9193 Elements (optimized) 13786 Simulations Results ANSYS® Explicit Dynamic simulations revealed similar behavior as seen in experiments. For example, 0.79mm CFRP went through rupture failure as shown in Figure 9. Tsai-Wu failure model was used in the simulations [12]. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 119 Side view Sample front view Sample back view Figure 9ANSYS® Explicit Dynamic simulations Comparison of Experiments and Simulations Table 2 summarizes the results from experiments and simulations. As shown, Experiments Simulations CFRP thickness = 0.79mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.59mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.63mm @ 25°C to -28°C (not tested) Safe CFRP thickness = 2.38mm @ 25°C to -28°C Safe Safe Conclusions and Limitations Following conclusion can be drawn from the study: 1. It can be concluded that pellet and storm pellets at 160 m/s can damage/pass through the 1.59mm and below thickness of CFRP. 2. Good agreement was found between the experiments and simulations. It confirms that Multiphysics methodology such as Explicit Dynamic simulations may be used for the design of CFRP structures undergoing impact loading. 3. It was found that CFRP material properties did not change noticeably in cold temperatures. Following limitations apply to the given study: 1. Commercially available CFRP samples (DragonPlate®) were used in this study. 2. Commercially available Multiphysics software ANSYS® was used for the simulations. 3. Samples were visually inspected and not for micro-fractures/micro-delamination. Acknowledgement Thanks to Prof. Young Kwon from Naval Postgraduate School, Monterey, California, USA for providing the test samples. References [1] Khawaja, Hassan Abbas; Moatamedi, Mojtaba. Multiphysics Investigation of Composite Shell Structures Subjected to Water Shock Wave Impact in Petroleum Industry. Materials Science Forum 2013. doi: https://doi.org/10.4028/www.scientific.net/MSF.767.60. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 120 [2] Khawaja, Hassan Abbas; Messahel, Ramzi; Souli, Mhmed; Al-Bahkali, Essam; Moatamedi, Mojtaba. Fluid solid interaction simulation of CFRP shell structure. Mathematics in Engineering, Science and Aerospace (MESA) 2017, 8(3), p. 311-324. Link: http://nonlinearstudies.com/index.php/mesa/article/view/1532 [3] Khawaja, Hassan Abbas; Bertelsen, Tommy; Andreassen, Roar; Moatamedi, Mojtaba. Study of CRFP Shell Structures under Dynamic Loading in Shock Tube Setup. Journal of Structures 2014, doi: http://dx.doi.org/10.1155/2014/487809. [4] Stange, Even; Andleeb, Zahra; Khawaja, Hassan; Moatamedi, Mojtaba. Multiphysics Study of Tensile Testing using Infrared thermography. The International Journal of Multiphysics 2019; 13(2), p. 191-202. doi: http://dx.doi.org/10.21152/1750-9548.13.2.191 [5] Myrli, Odd Einar; Khawaja, Hassan. Fluid-Structure Interaction (FSI) Modelling of Aquaculture Net Cage. The International Journal of Multiphysics 2019; 13(1). p. 97-111. doi: http://dx.doi.org/10.21152/1750-9548.13.1.97 [6] Ahmad, Tanveer; Khawaja, Hassan. Review of Low-Temperature Crack (LTC) Developments in Asphalt Pavements. The International Journal of Multiphysics 2018; 12(2). p. 169-187. doi: http://dx.doi.org/10.21152/1750-9548.12.2.169 [7] Allred and Associates Inc Company. [cited 03.03.2019]; Available from: http://dragonplate.com/sections/company.asp. [8] Allred and Associates Inc Product. [cited 03.03.2019]; Available from: https://dragonplate.com/economyplate-solid-carbon-fiber-sheet-1_32-x-12-x-12. [9] Allred and Associates Inc – Non-quasi-isotropic. [cited 03.03.2019]; Available from: https://dragonplate.com/quasi-isotropic-carbon-fiber-sheets. [10] Allred and Associates Inc -Twill weave. [cited 03.03.2019]; Available from: https://dragonplate.com/what-is-carbon-fiber. [11] ANSYS® Explicit Dynamic [cited 03.03.201","PeriodicalId":415881,"journal":{"name":"Explosion Shock Waves and High Strain Rate Phenomena","volume":"48 1-4","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Multiphysics Impact Analysis of Carbon Fiber Reinforced Polymer (CFRP) Shell\",\"authors\":\"H. Khawaja, M. Moatamedi, Z. Andleeb, C. Strand, P. Chen, B. Guo\",\"doi\":\"10.21741/9781644900338-20\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"With increasing popularity of Carbon Fiber Reinforced Polymer (CFRP) over time, the need for research in the field has increased dramatically. Many industries, i.e. aeronautical, automotive, and marine are opting to install carbon fiber in their structures to account for harsh environments like cold temperatures applications, but the research on the temperature exposure behavior of the materials are limited. This study aims to investigate the impact resistance of CFRP samples using the air gun tests. Two different shaped pellets (Diabolo and Storm pellets) were used in this work. The pellets speeds were calculated using a high-speed camera. The tests were performed in the room temperature (22°C) as well as in the cold room where the test pieces were exposed to about -28°C for seven days. The experimental studies were performed and compared against finite element simulations using ANSYS®. The studies also included layering of the CFRP samples to find the limiting thickness of pellets penetration. It was concluded that the thickness of 0.79mm and below of CFRP, cannot resist the impact of pellets. The visual inspection of failure revealed that the CFRP has gone through a brittle failure. However, temperature was found to have no significant impact on the results as similar behavior of CFRP was observed in both room conditions (22°C) and cold temperatures (-28°C). Introduction In the last decades, a growing interest has been dedicated in the use of composite materials for structural applications. CFRP composites are gaining a special attention to replace traditional materials in several fields although it is well known that these systems are highly susceptible to internal damage caused by transverse loads even under low-velocity ones [1,2]. In general, CFRP composites can be damaged on the surface and also beneath the surface by relatively light impacts causing invisible impact damage [3]. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Operative conditions affect the material properties as reported in [4-6]. Experimental Setup a. Test Samples Test samples used in this study were from the DragonPlate®, manufactured by Allred and Associates Inc., Elbridge, New York [7]. The CFRP samples used were EconomyPlateTM Solid Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 116 Carbon Fiber Sheet ~ 1/32\\\" x 12\\\" x 12\\\" (0.79375mm x 304.8mm x 304.8mm) [8]. EconomyPlateTM sheets comprised of orthotropic (non-quasi-isotropic) at 0°/90° orientation laminates [9] (Figure 1.) utilizing a twill weave [10] (Figure 2.), while maintaining a symmetrical and balanced laminate. EconomyPlateTM composed entirely of a tough and rigid carbon reinforced epoxy matrix, with textured finish on both sides. Samples were cut into smaller pieces for test purposes (Figure 3.). Figure 1-0°/90° orientation laminate Figure 2-Carbon fiber twill weave Figure 3-CFRP test samples b. Impact Tests To perform the impact tests, a shooting box was built, as shown in Figure 4a. The shooting box was designed such that it collects the pallets once they pass through the samples. The box consists of an opening-closing system with locking screws and wingnuts, so test pieces could be fastened for testing (Figure 4b), and removed and replaced with new test pieces effectively. Diabolo and storm pellets (Figures 5 and 6.) were shot on to the CFRP test samples. The material of both pellets was lead and they were of 4.5mm caliber, weighing about 0.5g each. The test was performed in room temperature, on tempered test pieces at about 22°C and in the cold room on test pieces exposed to about -28 ̊C for 7 days. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 117 (a) Shooting box (b) Fastened test piece Figure 4 – The opening-closing system of the shooting box Figure 5-Diabolo pellets Figure 6-Storm pellets A speed tests were carried out using a high-speed camera (Figure 7.). The test showed the pellets speed of about 160m/s. Figure 7-Speed test of Diabolo pellet (pellet speed ~ 160m/s) Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 118 Experimental Results Impact tests revealed that diabolo and storm pellets at 160m/s pass through the single layer (~0.79 mm) of CFRP (Figure 8). Visual inspection showed that the CFRP test samples were ruptured (brittle failure) and the failure was in the close vicinity of the impact. Ruptured holes were more visible when Storm pellets were used, nonetheless, the failure areas were the same. (a) Diabolo pellets (b) Storm pellets Figure 8-Visual inspection of the impact Tests were repeated by tightly joining the layers of CFRP tests samples (0.79mm, 1.59mm, and 2.38mm). Pellets passed through 0.79mm and 1.59mm thick CFRP test samples, however, deflected for 2.38mm layer. Same results were observed when tests were conducted at room temperature conditions (22°C) and cold conditions (-28°C). Simulations Setup The simulations were performed in ANSYS® Explicit Dynamic [11]. Mesh sensitivity analysis was performed to ensure the accuracy of results. The model parameters are given in Table 1. Table 1: Simulation model parameters (ANSYS® Explicit Dynamic) Physics preference Explicit Relevance 70 Relevance Center Fine Span Angle Center Fine Nodes (optimized) 9193 Elements (optimized) 13786 Simulations Results ANSYS® Explicit Dynamic simulations revealed similar behavior as seen in experiments. For example, 0.79mm CFRP went through rupture failure as shown in Figure 9. Tsai-Wu failure model was used in the simulations [12]. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 119 Side view Sample front view Sample back view Figure 9ANSYS® Explicit Dynamic simulations Comparison of Experiments and Simulations Table 2 summarizes the results from experiments and simulations. As shown, Experiments Simulations CFRP thickness = 0.79mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.59mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.63mm @ 25°C to -28°C (not tested) Safe CFRP thickness = 2.38mm @ 25°C to -28°C Safe Safe Conclusions and Limitations Following conclusion can be drawn from the study: 1. It can be concluded that pellet and storm pellets at 160 m/s can damage/pass through the 1.59mm and below thickness of CFRP. 2. Good agreement was found between the experiments and simulations. It confirms that Multiphysics methodology such as Explicit Dynamic simulations may be used for the design of CFRP structures undergoing impact loading. 3. It was found that CFRP material properties did not change noticeably in cold temperatures. Following limitations apply to the given study: 1. Commercially available CFRP samples (DragonPlate®) were used in this study. 2. Commercially available Multiphysics software ANSYS® was used for the simulations. 3. Samples were visually inspected and not for micro-fractures/micro-delamination. Acknowledgement Thanks to Prof. Young Kwon from Naval Postgraduate School, Monterey, California, USA for providing the test samples. References [1] Khawaja, Hassan Abbas; Moatamedi, Mojtaba. Multiphysics Investigation of Composite Shell Structures Subjected to Water Shock Wave Impact in Petroleum Industry. Materials Science Forum 2013. doi: https://doi.org/10.4028/www.scientific.net/MSF.767.60. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 120 [2] Khawaja, Hassan Abbas; Messahel, Ramzi; Souli, Mhmed; Al-Bahkali, Essam; Moatamedi, Mojtaba. Fluid solid interaction simulation of CFRP shell structure. Mathematics in Engineering, Science and Aerospace (MESA) 2017, 8(3), p. 311-324. Link: http://nonlinearstudies.com/index.php/mesa/article/view/1532 [3] Khawaja, Hassan Abbas; Bertelsen, Tommy; Andreassen, Roar; Moatamedi, Mojtaba. Study of CRFP Shell Structures under Dynamic Loading in Shock Tube Setup. Journal of Structures 2014, doi: http://dx.doi.org/10.1155/2014/487809. [4] Stange, Even; Andleeb, Zahra; Khawaja, Hassan; Moatamedi, Mojtaba. Multiphysics Study of Tensile Testing using Infrared thermography. The International Journal of Multiphysics 2019; 13(2), p. 191-202. doi: http://dx.doi.org/10.21152/1750-9548.13.2.191 [5] Myrli, Odd Einar; Khawaja, Hassan. Fluid-Structure Interaction (FSI) Modelling of Aquaculture Net Cage. The International Journal of Multiphysics 2019; 13(1). p. 97-111. doi: http://dx.doi.org/10.21152/1750-9548.13.1.97 [6] Ahmad, Tanveer; Khawaja, Hassan. Review of Low-Temperature Crack (LTC) Developments in Asphalt Pavements. The International Journal of Multiphysics 2018; 12(2). p. 169-187. doi: http://dx.doi.org/10.21152/1750-9548.12.2.169 [7] Allred and Associates Inc Company. [cited 03.03.2019]; Available from: http://dragonplate.com/sections/company.asp. [8] Allred and Associates Inc Product. [cited 03.03.2019]; Available from: https://dragonplate.com/economyplate-solid-carbon-fiber-sheet-1_32-x-12-x-12. [9] Allred and Associates Inc – Non-quasi-isotropic. [cited 03.03.2019]; Available from: https://dragonplate.com/quasi-isotropic-carbon-fiber-sheets. [10] Allred and Associates Inc -Twill weave. [cited 03.03.2019]; Available from: https://dragonplate.com/what-is-carbon-fiber. 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引用次数: 6

摘要

当使用Storm弹丸时,破裂的孔洞更加明显,尽管如此,失效区域是相同的。(a)空竹球(b)风暴球图8-冲击目视检查通过紧密连接CFRP测试样品(0.79mm, 1.59mm和2.38mm)的层来重复测试。颗粒通过0.79mm和1.59mm厚的CFRP测试样品,但在2.38mm层上发生偏转。在室温条件(22°C)和低温条件(-28°C)下进行测试时,观察到相同的结果。在ANSYS®Explicit Dynamic中进行仿真[11]。为保证结果的准确性,进行网格敏感性分析。模型参数如表1所示。表1:仿真模型参数(ANSYS®Explicit Dynamic)物理偏好显式相关性70关联中心细跨度角中心细节点(优化)9193元素(优化)13786仿真结果ANSYS®Explicit Dynamic仿真显示了与实验相似的行为。如图9所示,0.79mm CFRP发生破裂破坏。模拟采用Tsai-Wu失效模型[12]。爆炸激波与高应变率现象Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 119侧视图样品前视图样品后视图图9ANSYS®显式动态仿真实验与仿真对比表2总结了实验与仿真结果。如图所示,实验模拟CFRP厚度= 0.79mm @ 25°C至-28°C失效失效CFRP厚度= 1.59mm @ 25°C至-28°C失效失效CFRP厚度= 1.63mm @ 25°C至-28°C(未测试)安全CFRP厚度= 2.38mm @ 25°C至-28°C安全结论和限制可以得出,160 m/s的颗粒和暴风颗粒可以破坏/穿透厚度在1.59mm及以下的CFRP。2. 实验结果与模拟结果吻合较好。它证实了多物理场方法,如显式动态模拟,可用于设计碳纤维布结构承受冲击载荷。3.研究发现,低温条件下CFRP材料的性能变化不明显。以下限制适用于给定的研究:本研究使用市售CFRP样品(DragonPlate®)。2. 使用市售的多物理场软件ANSYS®进行仿真。3.目视检查样品,而不是微断裂/微分层。感谢美国加利福尼亚州蒙特利海军研究生院Young Kwon教授提供测试样本。[1] Khawaja, Hassan Abbas;Moatamedi Mojtaba。石油工业水激波冲击下复合壳结构的多物理场研究。2013材料科学论坛。doi: https://doi.org/10.4028/www.scientific.net/MSF.767.60。爆炸冲击波与高应变率现象材料研究论坛有限责任公司材料研究进展13 (2019)115-120 https://doi.org/10.21741/9781644900338-20 120 [2]Messahel Ramzi;Souli,嗯;Al-Bahkali小镇;Moatamedi Mojtaba。CFRP壳体结构流固相互作用模拟。数学学报(自然科学版),2017,33 (3),p. 311-324。链接:http://nonlinearstudies.com/index.php/mesa/article/view/1532 [3] Khawaja, Hassan Abbas;汤米Bertelsen;Andreassen咆哮;Moatamedi Mojtaba。激波管设置动载下CRFP壳结构的研究。结构学报,2014,doi: http://dx.doi.org/10.1155/2014/487809。[4][参考译文]Andleeb Zahra;主席哈桑;Moatamedi Mojtaba。红外热成像拉伸测试的多物理场研究。国际多物理场杂志2019;13(2),第191-202页。[5]米莉,奥德·埃纳尔;主席,哈桑。水产养殖网箱流固耦合(FSI)模型。国际多物理场杂志2019;13(1)。p . 97 - 111。[6] Ahmad, Tanveer;主席,哈桑。沥青路面低温裂缝研究进展国际多物理场杂志2018;12(2)。p . 169 - 187。doi: http://dx.doi.org/10.21152/1750-9548.12.2.169 [7] Allred and Associates Inc Company。(引用03.03.2019);可从:http://dragonplate.com/sections/company.asp。[8]杨志强。(引用03.03.2019);可从:https://dragonplate.com/economyplate-solid-carbon-fiber-sheet-1_32-x-12-x-12。[9]李志强,李志强。非准各向同性。(引用03.03.2019);可从:https://dragonplate.com/quasi-isotropic-carbon-fiber-sheets。[10]中国纺织工业股份有限公司。(引用03.03.2019);可从:https://dragonplate.com/what-is-carbon-fiber。[11] ANSYS®Explicit Dynamic [j]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Multiphysics Impact Analysis of Carbon Fiber Reinforced Polymer (CFRP) Shell
With increasing popularity of Carbon Fiber Reinforced Polymer (CFRP) over time, the need for research in the field has increased dramatically. Many industries, i.e. aeronautical, automotive, and marine are opting to install carbon fiber in their structures to account for harsh environments like cold temperatures applications, but the research on the temperature exposure behavior of the materials are limited. This study aims to investigate the impact resistance of CFRP samples using the air gun tests. Two different shaped pellets (Diabolo and Storm pellets) were used in this work. The pellets speeds were calculated using a high-speed camera. The tests were performed in the room temperature (22°C) as well as in the cold room where the test pieces were exposed to about -28°C for seven days. The experimental studies were performed and compared against finite element simulations using ANSYS®. The studies also included layering of the CFRP samples to find the limiting thickness of pellets penetration. It was concluded that the thickness of 0.79mm and below of CFRP, cannot resist the impact of pellets. The visual inspection of failure revealed that the CFRP has gone through a brittle failure. However, temperature was found to have no significant impact on the results as similar behavior of CFRP was observed in both room conditions (22°C) and cold temperatures (-28°C). Introduction In the last decades, a growing interest has been dedicated in the use of composite materials for structural applications. CFRP composites are gaining a special attention to replace traditional materials in several fields although it is well known that these systems are highly susceptible to internal damage caused by transverse loads even under low-velocity ones [1,2]. In general, CFRP composites can be damaged on the surface and also beneath the surface by relatively light impacts causing invisible impact damage [3]. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Therefore, this study has been carried out both to highlight effects of variables linked to geometrical parameters of composite sheets, impactor, and operative conditions. Operative conditions affect the material properties as reported in [4-6]. Experimental Setup a. Test Samples Test samples used in this study were from the DragonPlate®, manufactured by Allred and Associates Inc., Elbridge, New York [7]. The CFRP samples used were EconomyPlateTM Solid Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 116 Carbon Fiber Sheet ~ 1/32" x 12" x 12" (0.79375mm x 304.8mm x 304.8mm) [8]. EconomyPlateTM sheets comprised of orthotropic (non-quasi-isotropic) at 0°/90° orientation laminates [9] (Figure 1.) utilizing a twill weave [10] (Figure 2.), while maintaining a symmetrical and balanced laminate. EconomyPlateTM composed entirely of a tough and rigid carbon reinforced epoxy matrix, with textured finish on both sides. Samples were cut into smaller pieces for test purposes (Figure 3.). Figure 1-0°/90° orientation laminate Figure 2-Carbon fiber twill weave Figure 3-CFRP test samples b. Impact Tests To perform the impact tests, a shooting box was built, as shown in Figure 4a. The shooting box was designed such that it collects the pallets once they pass through the samples. The box consists of an opening-closing system with locking screws and wingnuts, so test pieces could be fastened for testing (Figure 4b), and removed and replaced with new test pieces effectively. Diabolo and storm pellets (Figures 5 and 6.) were shot on to the CFRP test samples. The material of both pellets was lead and they were of 4.5mm caliber, weighing about 0.5g each. The test was performed in room temperature, on tempered test pieces at about 22°C and in the cold room on test pieces exposed to about -28 ̊C for 7 days. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 117 (a) Shooting box (b) Fastened test piece Figure 4 – The opening-closing system of the shooting box Figure 5-Diabolo pellets Figure 6-Storm pellets A speed tests were carried out using a high-speed camera (Figure 7.). The test showed the pellets speed of about 160m/s. Figure 7-Speed test of Diabolo pellet (pellet speed ~ 160m/s) Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 118 Experimental Results Impact tests revealed that diabolo and storm pellets at 160m/s pass through the single layer (~0.79 mm) of CFRP (Figure 8). Visual inspection showed that the CFRP test samples were ruptured (brittle failure) and the failure was in the close vicinity of the impact. Ruptured holes were more visible when Storm pellets were used, nonetheless, the failure areas were the same. (a) Diabolo pellets (b) Storm pellets Figure 8-Visual inspection of the impact Tests were repeated by tightly joining the layers of CFRP tests samples (0.79mm, 1.59mm, and 2.38mm). Pellets passed through 0.79mm and 1.59mm thick CFRP test samples, however, deflected for 2.38mm layer. Same results were observed when tests were conducted at room temperature conditions (22°C) and cold conditions (-28°C). Simulations Setup The simulations were performed in ANSYS® Explicit Dynamic [11]. Mesh sensitivity analysis was performed to ensure the accuracy of results. The model parameters are given in Table 1. Table 1: Simulation model parameters (ANSYS® Explicit Dynamic) Physics preference Explicit Relevance 70 Relevance Center Fine Span Angle Center Fine Nodes (optimized) 9193 Elements (optimized) 13786 Simulations Results ANSYS® Explicit Dynamic simulations revealed similar behavior as seen in experiments. For example, 0.79mm CFRP went through rupture failure as shown in Figure 9. Tsai-Wu failure model was used in the simulations [12]. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 119 Side view Sample front view Sample back view Figure 9ANSYS® Explicit Dynamic simulations Comparison of Experiments and Simulations Table 2 summarizes the results from experiments and simulations. As shown, Experiments Simulations CFRP thickness = 0.79mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.59mm @ 25°C to -28°C Failed Failed CFRP thickness = 1.63mm @ 25°C to -28°C (not tested) Safe CFRP thickness = 2.38mm @ 25°C to -28°C Safe Safe Conclusions and Limitations Following conclusion can be drawn from the study: 1. It can be concluded that pellet and storm pellets at 160 m/s can damage/pass through the 1.59mm and below thickness of CFRP. 2. Good agreement was found between the experiments and simulations. It confirms that Multiphysics methodology such as Explicit Dynamic simulations may be used for the design of CFRP structures undergoing impact loading. 3. It was found that CFRP material properties did not change noticeably in cold temperatures. Following limitations apply to the given study: 1. Commercially available CFRP samples (DragonPlate®) were used in this study. 2. Commercially available Multiphysics software ANSYS® was used for the simulations. 3. Samples were visually inspected and not for micro-fractures/micro-delamination. Acknowledgement Thanks to Prof. Young Kwon from Naval Postgraduate School, Monterey, California, USA for providing the test samples. References [1] Khawaja, Hassan Abbas; Moatamedi, Mojtaba. Multiphysics Investigation of Composite Shell Structures Subjected to Water Shock Wave Impact in Petroleum Industry. Materials Science Forum 2013. doi: https://doi.org/10.4028/www.scientific.net/MSF.767.60. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 115-120 https://doi.org/10.21741/9781644900338-20 120 [2] Khawaja, Hassan Abbas; Messahel, Ramzi; Souli, Mhmed; Al-Bahkali, Essam; Moatamedi, Mojtaba. Fluid solid interaction simulation of CFRP shell structure. Mathematics in Engineering, Science and Aerospace (MESA) 2017, 8(3), p. 311-324. Link: http://nonlinearstudies.com/index.php/mesa/article/view/1532 [3] Khawaja, Hassan Abbas; Bertelsen, Tommy; Andreassen, Roar; Moatamedi, Mojtaba. Study of CRFP Shell Structures under Dynamic Loading in Shock Tube Setup. Journal of Structures 2014, doi: http://dx.doi.org/10.1155/2014/487809. [4] Stange, Even; Andleeb, Zahra; Khawaja, Hassan; Moatamedi, Mojtaba. Multiphysics Study of Tensile Testing using Infrared thermography. The International Journal of Multiphysics 2019; 13(2), p. 191-202. doi: http://dx.doi.org/10.21152/1750-9548.13.2.191 [5] Myrli, Odd Einar; Khawaja, Hassan. Fluid-Structure Interaction (FSI) Modelling of Aquaculture Net Cage. The International Journal of Multiphysics 2019; 13(1). p. 97-111. doi: http://dx.doi.org/10.21152/1750-9548.13.1.97 [6] Ahmad, Tanveer; Khawaja, Hassan. Review of Low-Temperature Crack (LTC) Developments in Asphalt Pavements. The International Journal of Multiphysics 2018; 12(2). p. 169-187. doi: http://dx.doi.org/10.21152/1750-9548.12.2.169 [7] Allred and Associates Inc Company. [cited 03.03.2019]; Available from: http://dragonplate.com/sections/company.asp. [8] Allred and Associates Inc Product. [cited 03.03.2019]; Available from: https://dragonplate.com/economyplate-solid-carbon-fiber-sheet-1_32-x-12-x-12. [9] Allred and Associates Inc – Non-quasi-isotropic. [cited 03.03.2019]; Available from: https://dragonplate.com/quasi-isotropic-carbon-fiber-sheets. [10] Allred and Associates Inc -Twill weave. [cited 03.03.2019]; Available from: https://dragonplate.com/what-is-carbon-fiber. [11] ANSYS® Explicit Dynamic [cited 03.03.201
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