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	<title>self-recovering impact absorbing materials &#8211; Science</title>
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	<title>self-recovering impact absorbing materials &#8211; Science</title>
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		<title>Twisting Metamaterial Turns Compression Into Self-Recovering Impact Protection</title>
		<link>https://scienmag.com/twisting-metamaterial-turns-compression-into-self-recovering-impact-protection/</link>
		
		<dc:creator><![CDATA[Neil Sanderson]]></dc:creator>
		<pubDate>Fri, 16 Oct 2026 06:05:41 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[3D printing]]></category>
		<category><![CDATA[advanced protective materials with energy dissipation]]></category>
		<category><![CDATA[axial compression to relative rotation conversion]]></category>
		<category><![CDATA[blast resistance]]></category>
		<category><![CDATA[compression–torsion coupling]]></category>
		<category><![CDATA[crash-resistant structures]]></category>
		<category><![CDATA[design of adaptive mechanical metamaterials]]></category>
		<category><![CDATA[energy dissipation]]></category>
		<category><![CDATA[friction]]></category>
		<category><![CDATA[friction-based energy dissipation mechanisms]]></category>
		<category><![CDATA[geometric amplification in mechanical structures]]></category>
		<category><![CDATA[impact protection]]></category>
		<category><![CDATA[impact protection using twisting metamaterials]]></category>
		<category><![CDATA[innovative impact protection technologies]]></category>
		<category><![CDATA[Metamaterial energy dissipation]]></category>
		<category><![CDATA[Metamaterials]]></category>
		<category><![CDATA[neural network optimization]]></category>
		<category><![CDATA[NSGA-II]]></category>
		<category><![CDATA[seismic isolation]]></category>
		<category><![CDATA[self-recovering impact absorbing materials]]></category>
		<category><![CDATA[structural reorganization under load]]></category>
		<category><![CDATA[topological interlocking]]></category>
		<category><![CDATA[topological interlocking assemblies]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=282430</guid>

					<description><![CDATA[A new topological interlocking metamaterial converts axial compression into torsional sliding, dissipating energy through amplified friction while recovering its shape after deformation.]]></description>
										<content:encoded><![CDATA[<p>&#8230;</p>
<p>&#8230;</p>
<p>The central achievement of the new metamaterial lies in how it reorganizes the way mechanical energy leaves a structure. In classical topological interlocking assemblies, individual blocks are held in place purely by geometry rather than by fasteners or adhesives, and when the assembly is loaded, the blocks slide against one another along their mating surfaces. That sliding is what dissipates energy, but it is inherently passive: the amount of frictional work extracted depends on the load path, and once the blocks have slipped into a new configuration, they generally stay there. The compression–torsion coupling strategy changes this picture fundamentally. By arranging the interlocking elements so that axial compression is converted into relative rotation between layers, the designers ensure that the sliding distance at each interface is no longer dictated simply by the applied displacement. Instead, the twist amplifies the relative motion between struts, so a modest vertical compression produces a much larger frictional sweep across the contacting surfaces. This geometric amplification is the key to extracting more dissipated energy per unit of input displacement than a purely passive arrangement can deliver.</p>
<p>The self-recovery aspect deserves particular attention because it addresses one of the most persistent weaknesses of friction-based protective materials. Conventional crushable absorbers, whether metallic honeycombs, foams, or lattice structures, absorb energy through permanent plastic deformation. They perform well in a single event, but after the crash or the earthquake, the material is deformed and must be replaced. Frictional systems avoid this by dissipating energy through Coulomb sliding, which is reversible in principle: remove the load, and elastic restoring forces push the components back toward their original positions. The difficulty has always been that in a stand-alone interlocking assembly, nothing actively drives the blocks back. Gravity or residual elastic strain may partially reseat them, but the recovery is unreliable. By embedding the interlocking elements within a torsion-coupling framework, the elastic members that undergo twist during compression store strain energy and then release it during unloading, actively rotating the interlocking blocks back into their initial registry. The result is a repeatable energy dissipation cycle, which the authors demonstrate through experiments and simulations showing progressive stiffening and stable dissipation up to a nominal strain of 0.25.</p>
<p>Progressive stiffening itself is a noteworthy mechanical signature. Many protective materials exhibit the opposite behavior: they soften as they collapse, producing a long plateau followed by densification. A stiffening response means that the resistance grows as the deformation accumulates, which is valuable in impact scenarios because it limits the total stroke consumed before the structure becomes rigid again. For a crash absorber, this translates into a predictable, self-limiting compression stroke. For a seismic isolation bearing, it means that as ground displacement grows, the restoring and dissipative forces grow with it, preventing the bearing from bottoming out. The combination of stiffening, stable dissipation, and self-recovery in a single architecture is what distinguishes this design from earlier frictional metamaterials, which typically achieved one or two of these attributes at the expense of the others.</p>
<p>The optimization methodology employed in the study reflects a broader shift in how architected materials are designed. The geometric parameters governing the compression–torsion coupling and the interlocking geometry form a high-dimensional design space that cannot be explored exhaustively through physical prototyping or even through brute-force finite element simulation. The researchers therefore trained a neural network surrogate model on simulated responses and coupled it with the NSGA-II multi-objective genetic algorithm. This combination allows the simultaneous pursuit of competing objectives, such as maximizing energy dissipation while controlling peak transmitted force and preserving self-recovery capability. Multi-objective optimization of this kind yields a Pareto front rather than a single optimum, giving engineers a family of candidate designs from which to select according to the priorities of a specific application. The approach mirrors strategies now common across the metamaterials community, where machine learning surrogates have dramatically reduced the computational cost of exploring nonlinear, history-dependent behaviors such as frictional sliding, which are notoriously difficult to capture with traditional analytical homogenization methods.</p>
<p>The blast simulation results provide perhaps the most striking quantitative evidence of the design&#8217;s protective capability. When a blast wave strikes a structure, the protective layer&#8217;s job is to attenuate the stress pulse before it reaches the protected component, in this case the base supporting the core. A conventional pyramidal lattice, a well-studied architected topology valued for its stiffness-to-weight ratio, transmits a sharp stress spike to its base shortly after the wave arrives. The TI-CTC core reduced this peak base stress by 78.5 percent relative to the pyramidal benchmark and delayed the arrival of the peak by a factor of 13.6. Both effects matter enormously in practice. Peak stress reduction determines whether the protected component yields or fractures, while the delay in peak arrival extends the time over which the impulse is delivered, effectively stretching the loading event and giving any connected damping or control systems more time to respond. The mechanism behind this attenuation is the distributed frictional sliding activated throughout the interlocking assembly, which converts the concentrated wave energy into heat at many interfaces simultaneously rather than allowing it to propagate coherently through the core.</p>
<p>The choice of polyamide as the printing material, referenced in the broader literature on selective laser sintering, is consistent with the demands of a frictional design. Frictional dissipation depends on the coefficient of friction at the interlocking interfaces and on the wear behavior of the contacting surfaces, both of which are material properties that must remain stable over repeated loading cycles. Polymers such as PA12 offer a favorable combination of printability, surface finish, and tribological behavior, and their viscoelasticity can contribute additional damping. At the same time, the reliance on friction raises questions that any deployment program would need to address: how the coefficient of friction evolves with wear, temperature, and contamination, and how the interlocking tolerances affect performance when parts are manufactured at scale. The experimental validation reported in the study, combining physical compression tests with numerical simulation, provides a foundation for answering these questions, but long-term cyclic durability under realistic environmental conditions remains an area for continued investigation.</p>
<p>The prospective applications named by the authors, self-recoverable crash-resistant automotive bumpers and seismic isolation bearings for bridge piers, span two very different loading regimes, and the metamaterial&#8217;s suitability for each follows from different aspects of its behavior. In automotive crash protection, the requirement is to absorb a large, essentially single-directional impulse while keeping the transmitted force below injury thresholds and then returning the component to a serviceable state, which reduces repair costs in minor collisions. The self-recovery and progressive stiffening characteristics align well with this scenario. In seismic isolation, the requirement is to accommodate many cycles of alternating displacement during an earthquake while dissipating energy in each cycle and recentering the structure afterward, preventing residual drift that would complicate post-event inspection and repair. Friction dampers have long served this role in civil engineering, and the variable-friction devices studied in recent literature demonstrate how staged stiffness and dissipation can be engineered into such systems. The TI-CTC metamaterial extends this concept into a three-dimensional architected form whose properties can be tuned geometrically rather than through material selection alone, offering designers a route to isolation bearings whose force-displacement law is prescribed by architecture rather than by metallurgy.</p>
<p>Placed in the context of the wider metamaterials literature, the design occupies an interesting intersection of several research threads. Topological interlocking itself draws inspiration from biological protective systems such as fish scales, osteoderms, and chainmail fabrics, in which rigid elements are assembled into flexible yet protective coverings through geometric constraint rather than bonding. Compression–torsion coupling, meanwhile, has been explored extensively in chiral metamaterials, where helical or rotated unit cells convert axial load into twist, sometimes with counterintuitive consequences for Poisson&#8217;s ratio and stiffness. Prior work had developed compression–torsion metamaterials with repeatable energy dissipation, and frictional metamaterials exploiting Coulomb sliding had been demonstrated independently. The novelty of the present design lies in fusing these two mechanisms so that the torsional deformation actively drives and amplifies the frictional sliding, rather than treating twist as merely a kinematic curiosity. This fusion converts what would otherwise be a passive frictional assembly into an actively self-cycling dissipative system.</p>
<p>The broader significance of the work extends to questions of sustainability and lifecycle performance. Structures that recover their shape after loading can be reused across many events, reducing material consumption compared with single-use crush zones. Because the dissipation mechanism is frictional rather than plastic, the material itself is not progressively damaged in the way that metal honeycombs or crush foams are, provided the contact surfaces remain within their wear limits. This reusability aligns with growing interest in architected materials designed for circularity, and the authors&#8217; use of a generalizable interlocking framework suggests that the concept could be adapted to different element geometries and material systems as manufacturing methods mature. Additive manufacturing is the natural fabrication route for the intricate interlocking geometries involved, and continued advances in printing resolution and surface quality will directly benefit the consistency of the frictional interfaces on which the entire mechanism depends.</p>
<p>Several avenues for future development follow naturally from the reported results. Experimental validation under true high-rate impact loading, beyond quasi-static testing and numerical blast simulation, would establish how the frictional behavior scales with strain rate, a question of central importance for crash and blast applications where polymer friction is known to be rate-sensitive. Scaling studies would clarify whether the favorable performance persists across the size range from centimeter-scale prototypes to meter-scale bridge bearings. Coupled thermal-mechanical analysis would quantify how frictional heating affects the interface properties during repeated or prolonged events. And the neural network surrogate framework, once trained, could be extended to explore material heterogeneity, graded architectures, and hybrid designs that combine the TI-CTC mechanism with negative-stiffness or auxetic elements to further tailor the response. Each of these directions builds on the core insight demonstrated here: that architecture can be designed not merely to carry load or to deform predictably, but to orchestrate the conversion of mechanical work into heat through geometrically amplified, self-restoring frictional motion, opening a path toward protective materials that survive not one event but many.</p>
<p><strong>Subject of Research:</strong> A compression–torsion coupling metamaterial based on topological interlocking for self-recoverable quasi-static and impact energy dissipation</p>
<p><strong>Article Title:</strong> Topological interlocking metamaterials with compression–torsion coupling for quasi-static and impact energy dissipation</p>
<p><strong>Article References:</strong> Lv, W., &amp; Li, D. (2026). Topological interlocking metamaterials with compression–torsion coupling for quasi-static and impact energy dissipation. <em>Journal of Materials Science, 61</em>(42), 32877-32890. <a href="https://doi.org/10.1007/s10853-026-13773-x" rel="noopener noreferrer">https://doi.org/10.1007/s10853-026-13773-x</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10853-026-13773-x" rel="noopener noreferrer">10.1007/s10853-026-13773-x</a></p>
<p><strong>Keywords:</strong> metamaterials, topological interlocking, compression–torsion coupling, energy dissipation, friction, impact protection, blast resistance, neural network optimization, NSGA-II, crash-resistant structures, seismic isolation, 3D printing</p>
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