热致动纤维增强形状记忆聚合物复合材料的弯曲分析

IF 1.9 Q3 MATERIALS SCIENCE, MULTIDISCIPLINARY
N. Tiwari, A. Shaikh
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引用次数: 3

摘要

形状记忆聚合物复合材料(SMPC)在过去几十年中因其在宽应变和温度范围内的灵活形状记忆行为而广受欢迎。本文对SMPC梁在均布横向荷载作用下的非线性弯曲进行了分析。采用基于高阶剪切变形理论的简化C0连续有限元法对SMPC进行了弯曲分析。采用迭代Newton-Raphson方法得到了数值解。用体积平均理论计算了以形状记忆聚合物(SMP)为基体、碳纤维为增强材料的SMPC的材料性能。已经针对许多参数评估了温度对SMPC的影响,例如层数、纵横比、边界条件、碳纤维的体积分数和层压板堆叠方向。此外,还提出了单位长度上的挠度分布和厚度上的应力行为,以详细说明玻璃化转变温度(Tg)的影响。本研究详细解释了在273-373K的宽温度范围内,不同参数对SMPC梁弯曲的影响,该温度范围包括SMPC的玻璃化转变区。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flexural analysis of thermally actuated fiber reinforced shape memory polymer composite
Shape Memory Polymer Composites (SMPC) have gained popularity over the last few decades due to its flexible shape memory behaviour over wide range of strains and temperatures. In this paper, non-linear bending analysis has been carried out for SMPC beam under the application of uniformly distributed transverse load (UDL). Simplified C0 continuity Finite Element Method (FEM) based on Higher Order Shear Deformation Theory (HSDT) has been adopted for flexural analysis of SMPC. The numerical solutions are obtained by iterative Newton Raphson method. Material properties of SMPC with Shape Memory Polymer (SMP) as matrix and carbon fibre as reinforcements, have been calculated by theory of volume averaging. Effect of temperature on SMPC has been evaluated for numerous parameters for instance number of layers, aspect ratio, boundary conditions, volume fraction of carbon fiber and laminate stacking orientation. Moreover, deflection profile over unit length and behavior of stresses across thickness are also presented to elaborate the effect of glass transition temperature (Tg). Present study provides detailed explanation on effect of different parameters on the bending of SMPC beam for large strain over a broad span of temperature from 273-373K, which encompasses glass transition region of SMPC.
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来源期刊
Advances in Materials Research-An International Journal
Advances in Materials Research-An International Journal MATERIALS SCIENCE, MULTIDISCIPLINARY-
CiteScore
3.50
自引率
27.30%
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0
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