Fabric Phononic Crystals for Passive Vibration Control
Pith reviewed 2026-07-02 01:32 UTC · model grok-4.3
The pith
Double-woven fabrics with periodic copper inclusions form phononic crystals that suppress out-of-plane vibrations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using double weaving to integrate periodic stiff copper inclusions within a soft cotton weave creates a fabric phononic crystal lattice whose dispersion supports a pronounced bandgap for out-of-plane vibrations. A multiscale model that homogenizes weave blocks into effective macroscale properties guides the design. Experiments on finite crystals confirm the bandgap through transmission measurements, while equivalent uniform cotton fabrics show no suppression. The platform further yields a fully woven higher-order topological insulator exhibiting in-gap edge states and localized corner states.
What carries the argument
Double-woven periodic lattice of soft cotton with stiff copper inclusions, whose wave behavior is predicted by multiscale homogenization of weave blocks into effective macroscale properties.
If this is right
- Phononic bandgaps and topological states can be encoded directly in fabrics through chosen weaving patterns and material contrast.
- Passive vibration filtering becomes possible in lightweight, flexible layers suitable for integration into clothing or surfaces.
- Edge and corner states in the woven topological insulator enable localized waveguiding without additional fabrication steps.
- The multiscale modeling framework supports computationally efficient design of new fabric-based wave devices.
Where Pith is reading between the lines
- Existing textile looms could produce these crystals at large scale without new machinery.
- Vibration-based sensing layers in wearables or soft robotics might emerge by combining the bandgap filtering with embedded detectors.
- Similar weaving contrasts could be explored for other wave types, such as acoustic or electromagnetic, by substituting different fiber materials.
Load-bearing premise
The hierarchical weave structure allows accurate wave prediction by first homogenizing small blocks and then using those effective properties at the larger scale.
What would settle it
Transmission measurements on the woven copper-cotton crystal that show out-of-plane vibration amplitudes inside the predicted bandgap range comparable to those in a uniform cotton weave would falsify the bandgap claim.
Figures
read the original abstract
Weaving patterns in fabrics, traditionally used for aesthetic purposes, present a largely untapped opportunity to create metamaterials that serve as passive layers for sensing, filtering, and signal processing. However, the hierarchical architecture of fabrics makes structural design and wave prediction challenging. Here, we establish fully woven fabrics as phononic crystals that passively filter and route elastic vibrations. Using double weaving, we integrate a soft cotton weave with stiff woven copper inclusions to form periodic fabric lattices with engineered dispersion. A multiscale modeling framework that combines homogenization of weave blocks with an effective-property macroscale model enables computationally efficient design of phononic crystals. Simulations and experiments confirm a pronounced phononic bandgap for out-of-plane vibrations in a finite fabric crystal, while an equivalent pure cotton weave shows no band suppression in the corresponding frequency range. Building on the same platform, we realize a fully woven higher-order topological insulator. Modal analysis and transmission measurements reveal in-gap edge states and localized corner states. These results show that phononic bandgaps and topological states can be directly encoded through weaving patterns and material contrast, enabling passive vibration management layers and multifunctional waveguiding fabrics for sensing, haptic interfaces, robotics, and noise mitigation.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that double-woven fabrics integrating soft cotton with stiff copper inclusions can be engineered as phononic crystals and higher-order topological insulators. A multiscale framework (homogenization of weave blocks plus effective-property macroscale model) is used to design periodic lattices that open a bandgap for out-of-plane vibrations; simulations and experiments on finite samples are said to confirm the gap (absent in pure cotton controls) together with in-gap edge states and localized corner states.
Significance. If the central claims hold, the work would demonstrate a scalable, textile-based route to passive elastic wave control and topological waveguiding without microfabrication. Experimental realization of both a bandgap and higher-order topological states in a fully woven platform would be a notable bridge between metamaterials and fabric engineering, with direct relevance to wearable sensing and vibration mitigation.
major comments (2)
- [Modeling framework / abstract] Modeling framework (described in the abstract and presumably §3–4): the central claim that the homogenized effective stiffness/density tensors correctly predict the out-of-plane bandgap and topological states rests on the validity of scale separation and the absence of local yarn-bending or contact effects. No quantitative benchmark is supplied comparing the homogenized dispersion or transmission spectra against a fully resolved unit-cell finite-element calculation at the relevant frequencies; without this check the experimental confirmation cannot be unambiguously attributed to the designed bandgap rather than to unmodeled hierarchical mechanics.
- [Results / experiments] Experimental validation (abstract and results section): while a pronounced bandgap is reported for the copper-cotton fabric versus no suppression in pure cotton, the manuscript supplies no error bars, repeatability statistics, or direct comparison of measured transmission spectra against the homogenized-model prediction. This leaves open whether the observed suppression quantitatively matches the multiscale prediction or arises from other damping or boundary effects.
minor comments (1)
- [Modeling] Notation for the effective tensors and weave-block homogenization should be defined explicitly with reference to the underlying constitutive assumptions.
Simulated Author's Rebuttal
We thank the referee for the constructive comments and positive assessment of the work's significance. Below we respond point by point to the major comments and indicate the revisions we will make.
read point-by-point responses
-
Referee: [Modeling framework / abstract] Modeling framework (described in the abstract and presumably §3–4): the central claim that the homogenized effective stiffness/density tensors correctly predict the out-of-plane bandgap and topological states rests on the validity of scale separation and the absence of local yarn-bending or contact effects. No quantitative benchmark is supplied comparing the homogenized dispersion or transmission spectra against a fully resolved unit-cell finite-element calculation at the relevant frequencies; without this check the experimental confirmation cannot be unambiguously attributed to the designed bandgap rather than to unmodeled hierarchical mechanics.
Authors: We agree that an explicit quantitative benchmark between the homogenized model and a fully resolved unit-cell finite-element calculation would strengthen the justification of the scale-separation assumption. In the revised manuscript we will add this comparison, presenting dispersion relations obtained from both the homogenized effective-medium model and a detailed yarn-resolved finite-element discretization of the weave unit cell over the frequency range of interest. This will demonstrate that local yarn-bending and contact nonlinearities remain negligible at the relevant wavelengths and that the bandgap and topological features are indeed captured by the multiscale framework. revision: yes
-
Referee: [Results / experiments] Experimental validation (abstract and results section): while a pronounced bandgap is reported for the copper-cotton fabric versus no suppression in pure cotton, the manuscript supplies no error bars, repeatability statistics, or direct comparison of measured transmission spectra against the homogenized-model prediction. This leaves open whether the observed suppression quantitatively matches the multiscale prediction or arises from other damping or boundary effects.
Authors: We acknowledge that the experimental section would benefit from more complete statistical reporting and direct model-experiment comparison. In the revision we will include error bars derived from repeated measurements on multiple independently fabricated samples, report the number of repeats and standard deviations, and overlay the measured transmission spectra with the predictions of the homogenized model to allow quantitative assessment of agreement within the bandgap and at the edge/corner-state frequencies. revision: yes
Circularity Check
No circularity: multiscale homogenization and experimental validation are independent of fitted inputs.
full rationale
The paper's central claims rest on a standard multiscale framework (homogenization of weave blocks followed by macroscale effective properties) whose validity is checked by direct simulation-experiment comparison on finite samples. No equations or steps reduce predictions to quantities defined by the same data; the bandgap and topological states are presented as outcomes of material contrast and weaving patterns, not as self-consistent fits. No self-citations are invoked as load-bearing uniqueness theorems, and no ansatz is smuggled in. The derivation chain is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The weave structure can be accurately represented by homogenized effective properties at the macroscale
Reference graph
Works this paper leans on
-
[1]
Kornreich,Introduction to fibres and fabrics, Textile Book Service,1966
E. Kornreich,Introduction to fibres and fabrics, Textile Book Service,1966
1966
-
[2]
J. Fan, L. Hunter,Engineering apparel fabrics and garments, Elsevier,2009
2009
-
[3]
Sockalingam, S
S. Sockalingam, S. C. Chowdhury, J. W. Gillespie Jr, M. Keefe,Textile Research Journal2017,87, 8 984
-
[4]
L. M. Castano, A. B. Flatau,Smart Materials and structures2014,23, 5 053001
-
[5]
G. Loke, W. Yan, T. Khudiyev, G. Noel, Y. Fink,Advanced Materials2020,32, 1 1904911
-
[6]
G. Loke, T. Khudiyev, B. Wang, S. Fu, S. Payra, Y. Shaoul, J. Fung, I. Chatziveroglou, P.-W. Chou, I. Chinn, et al.,Nature communications2021,12, 1 3317
-
[7]
Takamatsu, T
S. Takamatsu, T. Kobayashi, N. Shibayama, K. Miyake, T. Itoh,Sensors and Actuators A: Physical 2012,18457
2012
-
[8]
L. Shu, T. Hua, Y. Wang, Q. Li, D. D. Feng, X. Tao,IEEE Transactions on information technology in biomedicine2010,14, 3 767
-
[9]
S. Lee, J. Kim, I. Yun, G. Y. Bae, D. Kim, S. Park, I.-M. Yi, W. Moon, Y. Chung, K. Cho,Nature communications2019,10, 1 2468
-
[10]
Kim, K.-S
K. Kim, K.-S. Yun,International Journal of Precision Engineering and Manufacturing-Green Tech- nology2019,6, 4 699
-
[11]
Catrysse, R
M. Catrysse, R. Puers, C. Hertleer, L. Van Langenhove, H. Van Egmond, D. Matthys,Sensors and Actuators A: Physical2004,114, 2-3 302
-
[12]
A. F. Abouraddy, O. Shapira, M. Bayindir, J. Arnold, F. Sorin, D. S. Hinczewski, J. D. Joannopoulos, Y. Fink,Nature materials2006,5, 7 532
-
[13]
Lumelsky, M
V. Lumelsky, M. S. Shur, S. Wagner, M. Ding,Sensitive skin, volume 18, World Scientific,2000
2000
-
[14]
Someya, Y
T. Someya, Y. Kato, T. Sekitani, S. Iba, Y. Noguchi, Y. Murase, H. Kawaguchi, T. Sakurai,Proceed- ings of the National Academy of Sciences2005,102, 35 12321
-
[15]
Hasegawa, M
Y. Hasegawa, M. Shikida, D. Ogura, K. Sato, In2007 IEEE 20th International Conference on Micro Electro Mechanical Systems (MEMS). IEEE,2007603–606
-
[16]
Meyer, B
J. Meyer, B. Arnrich, J. Schumm, G. Troster,IEEE Sensors Journal2010,10, 8 1391
-
[17]
Takamatsu, T
S. Takamatsu, T. Kobayashi, N. Shibayama, K. Miyake, T. Itoh, In2011 Symposium on Design, Test, Integration & Packaging of MEMS/MOEMS (DTIP). IEEE,2011142–147
-
[18]
Grant, K
E. Grant, K. Luthy, J. Muth, L. Mattos, J. Braly, A. Seyam, T. Ghosh, A. Dhawan, K. Natarajan, International Journal of Clothing Science and Technology2004,16, 1-2 73
-
[19]
Salvado, A
J. Salvado, A. Esp´ ırito-Santo, M. Calado,Sensors2012,12, 6 7614
-
[20]
C. Ma, R. G. Parker, B. B. Yellen,Journal of Sound and Vibration2013,332, 20 4876
-
[21]
H. Ge, M. Yang, C. Ma, M.-H. Lu, Y.-F. Chen, N. Fang, P. Sheng,National Science Review2018,5, 2 159. 18
-
[22]
Mart´ ınez-Sala, J
R. Mart´ ınez-Sala, J. Sancho, J. V. S´ anchez, V. G´ omez, J. Llinares, F. Meseguer, et al.,nature1995, 378, 6554 241
-
[23]
J. V. S´ anchez-P´ erez, D. Caballero, R. M´ artinez-Sala, C. Rubio, J. S´ anchez-Dehesa, F. Meseguer, J. Llinares, F. G´ alvez,Physical Review Letters1998,80, 24 5325
-
[24]
Zhang, Z
X. Zhang, Z. Liu,Applied Physics Letters2004,85, 2 341
-
[25]
Feng, X.-P
L. Feng, X.-P. Liu, Y.-B. Chen, Z.-P. Huang, Y.-W. Mao, Y.-F. Chen, J. Zi, Y.-Y. Zhu,Physical Review B—Condensed Matter and Materials Physics2005,72, 3 033108
-
[26]
Feng, X.-P
L. Feng, X.-P. Liu, M.-H. Lu, Y.-B. Chen, Y.-F. Chen, Y.-W. Mao, J. Zi, Y.-Y. Zhu, S.-N. Zhu, N.-B. Ming,Physical review letters2006,96, 1 014301
-
[27]
S. Yang, J. H. Page, Z. Liu, M. L. Cowan, C. T. Chan, P. Sheng,Physical review letters2004,93, 2 024301
-
[28]
M. Ke, Z. Liu, C. Qiu, W. Wang, J. Shi, W. Wen, P. Sheng,Physical Review B—Condensed Matter and Materials Physics2005,72, 6 064306
-
[29]
C. Qiu, X. Zhang, Z. Liu,Physical Review B—Condensed Matter and Materials Physics2005,71, 5 054302
-
[30]
Sukhovich, B
A. Sukhovich, B. Merheb, K. Muralidharan, J. O. Vasseur, Y. Pennec, P. A. Deymier, J. Page,Physical review letters2009,102, 15 154301
-
[31]
C. He, X. Ni, H. Ge, X.-C. Sun, Y.-B. Chen, M.-H. Lu, X.-P. Liu, Y.-F. Chen,Nature physics2016, 12, 12 1124
-
[32]
Zhang, B.-Y
X. Zhang, B.-Y. Xie, H.-F. Wang, X. Xu, Y. Tian, J.-H. Jiang, M.-H. Lu, Y.-F. Chen,Nature communications2019,10, 1 5331
-
[33]
Zhang, H.-X
X. Zhang, H.-X. Wang, Z.-K. Lin, Y. Tian, B. Xie, M.-H. Lu, Y.-F. Chen, J.-H. Jiang,Nature Physics 2019,15, 6 582
2019
-
[34]
Zhang, Q
Z. Zhang, Q. Wei, Y. Cheng, T. Zhang, D. Wu, X. Liu,Physical review letters2017,118, 8 084303
-
[35]
H. Dai, B. Xia, D. Yu,Journal of Applied Physics2019,125, 23
-
[36]
M. Y. Wang, M. Thevamaran, M. S. Mattei, B. G. Hacha, G. A. Mazzei Capote, Z. Yu, T. Osswald, R. H. Goldsmith, D. J. Thoma, C. Ma,Applied Physics Letters2022,120, 14
-
[37]
Zheng, J
Z. Zheng, J. Yin, J. Wen, D. Yu, X. Chen,International Journal of Mechanical Sciences2023,243 108035
-
[38]
R. Gong, B. Ozgen, M. Soleimani,Textile Research Journal2009,79, 11 1014
-
[39]
R. B. Turan, A. Okur,Textile Research Journal2012,82, 7 719
-
[40]
Carvelli, C
V. Carvelli, C. Poggi,Composites Part A: Applied Science and Manufacturing2001,32, 10 1425
-
[41]
Thierry, S
V. Thierry, S. Cantero-Chinchilla, W. Wu, A. Lhemery, D. Chronopoulos,Structural Control and Health Monitoring2021,28, 6 e2728
-
[42]
Thierry, L
V. Thierry, L. Brown, D. Chronopoulos,Composites Part B: Engineering2018,150144
-
[43]
Thierry, O
V. Thierry, O. Mesnil, D. Chronopoulos,Ultrasonics2020,103106068
-
[44]
Chaunsali, C.-W
R. Chaunsali, C.-W. Chen, J. Yang,New Journal of Physics2018,20, 11 113036
-
[45]
Kittel, P
C. Kittel, P. McEuen,Introduction to solid state physics, John Wiley & Sons,2018. 19
2018
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.