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High-symmetry architecture reveals both macroscopic and local patterns. In the actual short-fiber composite depicted in (a), there are three straight-fiber (SF) segments (AB, DE, and GH) and two curved-fiber (CF) segments (BD and EG). Meanwhile, (b) showcases the continuous representation of the short-fiber composite alongside its homogenized counterpart, consisting of a series of parallel blocks on different isotropy planes. The homogenized counterpart has the same effective modulus compared to the short-fiber composite, and its modulus can be theoretically calculated using the energy conservation principle and Hooke’s law.
(a–b) Multisegment curvilinear fiber reinforced (CFR) composites exhibit varying choices of 𝛼 and 𝛽, where 𝛼 denotes the change in curvature at the transition regime, and 𝛽 represents the orientation of the top and bottom of the domain. (c–d) Depicting the 𝜎𝑦𝑦 stress field for different values of 𝛼 and 𝛽 at a given loading state, with stress ranging from 0 GPa (blue) to 1 GPa (red). (e) Explores the impact of 𝛼 on modulus at a constant 𝛽, (f) examines the effect of 𝛽 on modulus at constant 𝛼, and (g) analyzes the combined effects of 𝛼 and 𝛽 on the effective modulus.
(Top) Fiber configurations and (Bottom) 𝜎𝑦𝑦 stress field for six orientations at a given load for sinusoidal carbon fiber reinforcement composites.
(Top) Fiber configurations and (Bottom) 𝜎𝑦𝑦 stress field for six orientations at a given load for hyperbolic tangent carbon fiber reinforcement composites.