Home Technology Comparison of crash performance of auxetic structures for CF15, PA6/GF30, and GF30PP materials
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Comparison of crash performance of auxetic structures for CF15, PA6/GF30, and GF30PP materials

  • Ali Riza Yildiz

    Dr. Ali Riza Yildiz is a Professor in the Department of Mechanical Engineering at Bursa Uludağ University, Bursa, Turkey. He is head of the mechanical engineering department and a Full Member of the Turkish Academy of Sciences(TUBA). His research interests are the finite element analysis of structural components, auxetic structures, additive manufacturing, lightweight design, vehicle design, vehicle crashworthiness, shape and topology optimization of vehicle components, and meta-heuristic optimization techniques.

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Published/Copyright: April 29, 2025
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Abstract

Plate auxetic structures, distinguished by their negative Poisson’s ratio, demonstrate unconventional mechanical responses, expanding laterally under tension and contracting under compression. These systems, particularly plate-based designs, are increasingly studied for their exceptional energy absorption, impact resilience, and structural versatility. This research investigates the mechanical behavior of nine auxetic geometries, including reentrant, chiral, antichiral, meta-chiral, arrowhead, star, and a new hybrid auxetic design for three different materials, which are 30 % short glass fiber reinforced polypropylene (GF30PP), polyamide 6 reinforced with 30 % of short glass fiber (PA6/GF30), and high-temperature resistant polyamide with 15 % carbon fiber (CF15) are materials of the auxetic structures used in this paper. Energy absorption performance, maximum forces, and specific energy absorption amount are analyzed to evaluate their suitability for the nine auxetic designs. Findings reveal that Design 9, which is developed in this paper, shows the best energy absorption capacity for PA6/GF30 and CF15 materials.

1 Introduction

Auxetic materials form an exceptional class of substances defined by their unique mechanical behavior: when stretched, they expand laterally rather than thinning, and when compressed, they contract instead of thickening [1], [2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35], [36], [37], [38], [39], [40], [41]. This phenomenon, characterized by a negative Poisson’s ratio, starkly contrasts with most conventional materials, which exhibit a positive Poisson’s ratio, thinning under tension and thickening under compression. The counterintuitive response of auxetics arises from their sophisticated internal architectures, meticulously engineered to convert applied forces into lateral motion. These designs include angled cellular patterns (reentrant shapes), spiral-like chiral geometries, or interconnected rotating components that mechanically amplify expansion or contraction.

The engineered microstructures of auxetic materials grant them extraordinary properties, such as enhanced resistance to impacts, superior energy absorption, and the ability to conform to irregular surfaces. These capabilities have enabled their integration into a variety of applications across disciplines, from biomedical implants and protective equipment to aerospace components and shape-adaptive textiles. Advances in manufacturing techniques, mainly additive manufacturing (3D printing) and computational modeling, have revolutionized their development, allowing for intricate, tailored designs that optimize performance for specific use cases. Current research is expanding the horizons of auxetic materials by experimenting with hybrid composites, multifunctional geometries, and scalable production methods. By blending innovative structural design with material science, auxetics address critical engineering challenges, such as creating ultra-lightweight yet durable components, managing sudden or variable loads, and enabling responsive, shape-shifting systems. As this field progresses, auxetic structures are poised to transform industries, turning once-theoretical concepts into practical solutions that meet evolving demands for efficiency, adaptability, and resilience.

This research investigates the mechanical behavior of nine auxetic geometries, including reentrant, chiral, antichiral, meta-chiral, arrowhead, star, and a new hybrid auxetic design for 30 % short glass fiber reinforced polypropylene (GF30PP), polyamide 6 reinforced with 30 % of short glass fiber (PA6/GF30), and high-temperature resistant polyamide with 15 % carbon fiber (CF15) materials.

2 Literature review

In recent years, reducing vehicle weight has gained considerable significance. In this regard, research has been conducted on integrating advanced materials and composite structures into vehicle bodies. Studies have demonstrated that designs incorporating next-generation materials achieve the necessary strength characteristics. Consequently, the vehicle body becomes both more robust and substantially lighter. In addition, composite and auxetic structures show superior performance in reducing deformations of the vehicle body after crashes [27], [28], [29], [30], [31], [32].

Auxetic materials are specially designed artificial materials with a Negative Poisson’s Ratio (NPR), meaning they have an unusual mechanical response, expanding sideways when stretched and contracting laterally when compressed [5], [6]. These materials are classified based on the structural mechanisms responsible for their auxetic properties. Major categories include reentrant designs [7], [8], [9], [10], arrow-head [11], chiral configurations [12], [13], [14], star shapes [15], antitrichiral [16], meta-chiral (antichiral–reentrant) [17], trichiral [18], meta-chiral [19], and crumpled geometries [20], [22]. Recently, auxetic metamaterials have been used in various fields, such as biomedical applications [23], [24], [25], energy harvesting systems [26], [27], [28], [29], and impact energy absorption [30], [31], [32].

Novel auxetic structures’ innovative design and efficiency were investigated [33]. The performance of a honeycomb, auxetic strut structures, and a hybrid structure is compared. The influence of auxetic structures on crash performance was examined [34]. Utilizing a systematic design approach, they developed three distinct auxetic structures with the dimensions illustrated in the figure. These structures were manufactured via additive manufacturing using SUS316L metal powder. Various structures were designed incorporating negative Poisson’s ratio helical forms, lattice configurations, and high-strength composite materials [35]. Their findings indicated that composites reinforced with auxetic lattice structures exhibited superior mechanical properties. It developed auxetic structures using an innovative design approach and negative Poisson’s ratio properties to create auxiliary structures with unique attributes [36]. The design parameters for these three distinct structures are presented in the accompanying table. A new auxetic structure is proposed [37]. This evaluation was conducted by physically testing 3D-printed samples produced via the selective laser melting (SLM) method and computer simulations. These auxetic structures, manufactured using additive techniques, were designed with predefined dimensions. Conducted research by designing a reentrant model and a hexagonal structure using two types of auxetic materials [38]. They created the models utilizing nylon, carbon-reinforced nylon, and glass-reinforced nylon. The samples required for testing were fabricated through additive manufacturing. Four different auxetic structures were investigated to enhance their energy absorption capabilities [39]. The specific unit cells used in their study are illustrated in Figure 26. They introduced x and y parameters to optimize the energy absorption capacity. It was studied foam-filled structures [40]. They proposed a structure incorporating a double arrow auxetic design, as depicted in the figure, and investigated its energy absorption characteristics. A gradient configuration was established to enhance energy absorption performance, and its effects on energy dissipation were examined. It was designed as an auxetic structure [41].

3 Quasi-static compression analysis of the auxetic structures

This research investigated the crash performance of nine different auxetic structures: reentrant, chiral, antichiral, arrowhead, star, meta-chiral, and a new hybrid auxetic design. As shown in Figure 1, dimensions of the plates are 200 × 160 × 15 mm. Table 1 shows a list of the auxetic structures used in this paper.

Figure 1: 
Boundary conditions for the finite element method analysis.
Figure 1:

Boundary conditions for the finite element method analysis.

Table 1:

List of auxetic structures used in this paper.

Types of auxetics Cellular geometries Auxetic structures
Re-entrant [7]
Arrow-head [11]
Chiral [12]
Star [15]
Anti-trichiral [16]
Meta-chiral (Antichiral-reentrant) [17]
Trichiral [18]
Trichiral [19]
Hybrid

In this research, nine different auxetic plates are designed, as shown in Figures 2, 6, 10, 14, 18, 22, 26, 30, 34. In the same figures, the deformation behaviours of the auxetic structures are also shown. All design crash analyses are completed in Hypermesh RADIOSS under the boundary conditions in Figure 1. The results presented in Table 2, Table 3, and Table 4 for GF30PP, PA6/GF30, and CF15 materials are obtained. The force–displacement curves found from the FEA for the auxetic plates for three different materials, which are GF30pp, Pa 6 GF30, and CF15, are shown in Figures 3, 5, 7, 9, 11, 13, 15,17, and 19, respectively. The mass of the auxetic designs changes from 105.8 to 232.6 g. The specific energy absorption of Design 9 is 2.0922 kJ kg−1, which is better than the rest of the designs for GF30PP material. Design 8 has the best specific energy absorption with 2.2915 kJ kg−1. Design 9 has the best value of specific energy absorption and amount of energy absorption, but the maximum force is the worst of Design 9 for GF30PP material. Design 9 absorbs maximum energy for PA6/GF30 and CF15 materials. However, the peak force of Design 9 for PA6/GF30 and CF15 materials is the biggest.

Figure 2: 
Deformation behavior of design 1 (re-entrant) for GF30PP.
Figure 2:

Deformation behavior of design 1 (re-entrant) for GF30PP.

Figure 3: 
Force-displacement curve for design 1 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 3:

Force-displacement curve for design 1 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 4: 
Force-displacement curve for design 1 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 4:

Force-displacement curve for design 1 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 5: 
Force-displacement curve for design 1 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 5:

Force-displacement curve for design 1 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 6: 
Deformation behavior of design 2(arrow-head) for 30 % short glass fiber reinforced polypropylene for GF30PP.
Figure 6:

Deformation behavior of design 2(arrow-head) for 30 % short glass fiber reinforced polypropylene for GF30PP.

Figure 7: 
Force-displacement curve for design 2 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 7:

Force-displacement curve for design 2 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 8: 
Force-displacement curve for design 2 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 8:

Force-displacement curve for design 2 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 9: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 9:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 10: 
Deformation behavior of design 3(chiral) for GF30.
Figure 10:

Deformation behavior of design 3(chiral) for GF30.

Figure 11: 
Force-displacement curve for design 3 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 11:

Force-displacement curve for design 3 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 12: 
Force-displacement curve for design 3 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 12:

Force-displacement curve for design 3 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 13: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 13:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 14: 
Deformation behavior of design 4(star) for GF30PP.
Figure 14:

Deformation behavior of design 4(star) for GF30PP.

Figure 15: 
Force-displacement curve for design 4 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 15:

Force-displacement curve for design 4 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 16: 
Force-displacement curve for design 4 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 16:

Force-displacement curve for design 4 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 17: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 17:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 18: 
Deformation behavior of design 5 (anti-chiral) for GF30PP.
Figure 18:

Deformation behavior of design 5 (anti-chiral) for GF30PP.

Figure 19: 
Force-displacement curve of design 5 for 30 % short glass fiber reinforced polypropylene for GF30PP.
Figure 19:

Force-displacement curve of design 5 for 30 % short glass fiber reinforced polypropylene for GF30PP.

Figure 20: 
Force-displacement curve of design 5 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 20:

Force-displacement curve of design 5 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 21: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 21:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 22: 
Deformation behavior of design 6 for GF30 PP.
Figure 22:

Deformation behavior of design 6 for GF30 PP.

Figure 23: 
Force-displacement curve of design 6 for 30 % short glass fiber reinforced polypropylene.
Figure 23:

Force-displacement curve of design 6 for 30 % short glass fiber reinforced polypropylene.

Figure 24: 
Force-displacement curve of design 6 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 24:

Force-displacement curve of design 6 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 25: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 25:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 26: 
Deformation behavior of design 7(meta-chiral) for GF30PP.
Figure 26:

Deformation behavior of design 7(meta-chiral) for GF30PP.

Figure 27: 
Force-displacement curve of design 7 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 27:

Force-displacement curve of design 7 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 28: 
Force-displacement curve of design 7 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 28:

Force-displacement curve of design 7 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 29: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 29:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 30: 
Deformation behavior of design 8 for GF30PP.
Figure 30:

Deformation behavior of design 8 for GF30PP.

Figure 31: 
Force-displacement curve of design 8 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 31:

Force-displacement curve of design 8 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 32: 
Force-displacement curve of design 8 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 32:

Force-displacement curve of design 8 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 33: 
Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.
Figure 33:

Force-displacement curve for design 2 for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Figure 34: 
Deformation behavior of design 9 for GF30PP.
Figure 34:

Deformation behavior of design 9 for GF30PP.

Figure 35: 
Force-displacement curve of design 9 for 30 % short glass fiber reinforced polypropylene-GF30PP.
Figure 35:

Force-displacement curve of design 9 for 30 % short glass fiber reinforced polypropylene-GF30PP.

Figure 36: 
Force-displacement curve of design 9 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.
Figure 36:

Force-displacement curve of design 9 for polyamide 6 reinforced with 30 % of short glass fiber-PA6 GF30.

Figure 37: 
Force-displacement curve for design 2 for polyamide 6 reinforced with 30 % of short glass fiber-CF15.
Figure 37:

Force-displacement curve for design 2 for polyamide 6 reinforced with 30 % of short glass fiber-CF15.

Table 2:

Comparison of crash performances of the auxetic designs for 30 % short glass fiber reinforced polypropylene-GF30PP.

Design 1 (re-entrant) Design 2 (arrow-head) Design 3 (missing rib) Design 4 (star) Design 5 (anti-chiral) Design 6 (anti-chiral-2) Design 7 (meta chiral) Design 8 (meta chiral) Design 9 (hybrid)
Mass(gram) 122.4 154.0 134.2 147.9 112.1 127.0 105.8 117.7 232.6
Maximum force (kN) 3.199 4.866 4.141 3.791 3.821 1.848 3.398 3.94 7.73
Energy absorption (Joule) 66.8 236.1 50.4 115.9 65.1 65 57.8 97.6 48.67
Specific energy absorption (kJ/kg) 0.546 1.532 0.375 0.783 0.581 0.512 0.546 0.829 2.092
Table 3:

Comparison of crash performances of the auxetic designs for polyamide 6 reinforced with 30 % of short glass fiber-Pa6 GF30.

Design 1 (re-entrant) Design 2 (arrow-head) Design 3 (missing rib) Design 4 (star) Design 5 (anti-chiral) Design 6 (anti-chiral-2) Design 7 (meta chiral) Design 8 (meta chiral) Design 9 (hybrid)
Mass(gram) 132.2 166.3 144.9 159.7 121.1 137.2 114.3 127.1 251.2
Maximum force (kN) 7.8459 14.2432 10.1745 8.3159 9.3755 4.4418 9.7457 9.6229 16.8558
Energy absorption (Joule) 126.2 323.2 95.1 230.4 127.6 127.8 165.6 196.8 349.2
Specific energy absorption (kJ/kg) 0.9545 1.9434 0.6566 1.4426 1.0536 0.9316 1.4489 1.5482 1.390
Table 4:

Comparison of crash performances of the auxetic designs for high-temperature resistant polyamide with 15 % carbon fiber-CF15.

Design 1 (re-entrant) Design 2 (arrow-head) Design 3 (missing rib) Design 4 (star) Design 5 (anti-chiral) Design 6 (anti-chiral-2) Design 7 (meta chiral) Design 8 (meta chiral) Design 9 (hybrid)
Mass(gram) 122.4 154.0 144.9 159.7 121.1 137.2 114.3 127.1 251.2
Maximum force (kN) 12.8852 19.7427 16.7297 13.7054 15.3605 7.1967 15.8593 15.5479 26.5606
Energy absorption (Joule) 183.8 329.8 135.5 332.6 183.4 183.9 241.4 291.3 435.5
Specific energy absorption (kJ/kg-1) 1.3903 1.9831 0.9348 2.0827 1.5145 1.3405 2.1122 2.2915 1.7338

4 Conclusions

This study presents a detailed comparative evaluation of in-plane plate-type auxetic structures, analyzing their mechanical performance. The study highlights how structural configuration influences energy absorption characteristics by investigating various geometrical designs, including reentrant, chiral, antichiral, meta-chiral, arrowhead, star, and a new hybrid auxetic design, Design 9. The materials of the auxetic structures are 30 % short glass fiber reinforced polypropylene (GF30PP), polyamide 6 reinforced with 30 % of short glass fiber (PA6/GF30), and high-temperature resistant polyamide with 15 % carbon fiber (CF15). Findings indicate that Design 9, which is developed in this paper, exhibits the best energy absorption capacity for PA6/GF30 and CF15 materials. Design 8 has the best specific energy absorption with 2.2915 kJ kg−1 for CF15. With advancements in computational simulations, additive manufacturing, and material innovation, auxetic structures can be further optimized for enhanced functionality in lightweight, high-strength, and energy-efficient designs. This research lays the groundwork for future studies exploring hybrid auxetic materials, dynamic loading effects, and large-scale experimental validation, helping bridge the gap between theoretical modeling and real-world engineering applications.


Corresponding author: Ali Riza Yildiz, Department of Mechanical Engineering, 37523 Bursa Uludag University , Bursa, Türkiye, E-mail:

Funding source: Bursa Uludağ University Scientific Research Projects (BAP)

Award Identifier / Grant number: FGA-2023-1316

About the author

Ali Riza Yildiz

Dr. Ali Riza Yildiz is a Professor in the Department of Mechanical Engineering at Bursa Uludağ University, Bursa, Turkey. He is head of the mechanical engineering department and a Full Member of the Turkish Academy of Sciences(TUBA). His research interests are the finite element analysis of structural components, auxetic structures, additive manufacturing, lightweight design, vehicle design, vehicle crashworthiness, shape and topology optimization of vehicle components, and meta-heuristic optimization techniques.

Acknowledgment

This research is supported by the Bursa Uludağ University Scientific Research Projects (BAP) unit under the Research Universities Support Program (ADEP) (Project number: FGA-2023-1316).

  1. Research ethics: Not applicable.

  2. Informed consent: Not applicable.

  3. Author contributions: The author has accepted responsibility for the entire content of this manuscript and approved its submission.

  4. Use of Large Language Models, AI and Machine Learning Tools: None declared.

  5. Conflict of interest: The author states no conflict of interest.

  6. Research funding: None declared.

  7. Data availability: Not applicable.

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Published Online: 2025-04-29
Published in Print: 2025-06-26

© 2025 the author(s), published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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