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arxiv: 2603.27227 · v2 · submitted 2026-03-28 · ⚛️ physics.flu-dyn

Recognition: 2 theorem links

· Lean Theorem

Reconfigurable kirigami mesostructure enables modulation of lift and drag

Authors on Pith no claims yet

Pith reviewed 2026-05-14 22:06 UTC · model grok-4.3

classification ⚛️ physics.flu-dyn
keywords kirigamireconfigurable structuresaerodynamicsfluid forcesdrag modulationlift generationmesostructurebuckling
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0 comments X

The pith

Kirigami sheets buckle into 3D lattices that generate controllable lift and drag in crossflow.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

Kirigami sheets patterned with parallel slits transform in flow into three-dimensional porous structures made of inclined plates. This reconfiguration allows a single sheet to produce varying amounts of drag and lift forces, and sometimes to adjust them somewhat independently, all while the flow conditions stay the same. The forces depend on the stiffness set by the cut pattern, and measurements collapse onto a single curve when plotted against the Cauchy number. A simple elastic model explains how the mesostructure controls the aerodynamic response. This approach offers a way to make surfaces that adapt their fluid forces passively through their geometry alone.

Core claim

Parallel-cut kirigami sheets, when placed perpendicular to oncoming flow, buckle out of plane to form a lattice of inclined plate-like elements. This mesostructure produces both drag and a substantial transverse lift force. Because the buckling pattern can switch between distinct states, the same sheet can achieve large changes in lift and drag coefficients under fixed flow conditions, and in some cases partially decouple the two forces. Force data for different patterns collapse when normalized by the Cauchy number, with the continuum elastic model capturing the dependence on stiffness.

What carries the argument

The reconfigurable kirigami mesostructure formed by out-of-plane buckling of parallel-slit sheets into an array of inclined plates.

If this is right

  • The mesostructure alters the scaling of aerodynamic forces with flow speed.
  • Stiffness from the cutting pattern is the dominant control parameter for the forces.
  • The architecture can be reversibly reconfigured in flow to switch between different force states.
  • Force measurements can be collapsed using the Cauchy number across different patterns.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If the buckling is reliable across scales, this could enable passive flow control on larger structures like wind turbines or vehicles.
  • The partial decoupling of lift and drag suggests possible applications in directional force management without active control.
  • Extending the pattern to other cut geometries might allow even finer tuning of the force ratios.
  • Testing in unsteady flows could reveal how the reconfiguration responds to changing conditions.

Load-bearing premise

The buckling into the lattice of inclined plates happens reliably and reversibly for the tested patterns without needing extra parameters beyond the continuum model.

What would settle it

Observing whether a kirigami sheet with a given cut pattern fails to buckle consistently or produces force data that does not collapse onto the Cauchy-number curve when flow speed or stiffness is varied.

Figures

Figures reproduced from arXiv: 2603.27227 by Agathe Schmider, Sophie Ramananarivo, Tom Marzin.

Figure 1
Figure 1. Figure 1: Kirigami surface for tunable lift and drag generation. a [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Pattern-induced stiffness as a control parameter for aerodynamic performance. a [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Pattern independence at matched stiffness. a [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Blade rotation as a mechanism for drag modulation. a [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Tuning of lift and drag via the mesostructural reconfiguration. a [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
read the original abstract

Flexible surfaces can modulate fluid forces through deformation, enabling passive adaptation to flow conditions. Here we show that kirigami sheets, planar surfaces patterned with arrays of parallel slits, provide a simple route to tunable aerodynamics by transforming into three-dimensional porous meso-architectures that can be reversibly reconfigured in flow. When exposed to crossflow, parallel-cut kirigami buckle out of plane to form a lattice of inclined plate-like elements. Experiments reveal that this architecture generates not only drag but also a substantial transverse lift force, even when the sheet is held perpendicular to the incoming flow. Because the mesostructure can switch between distinct states, a single sheet produces large and selective variations in drag and lift under identical flow conditions, in some cases partially decoupling these forces. The evolving mesostructure also alters the scaling of forces with flow speed, influencing both instantaneous loads and their velocity dependence. Force measurements collapse when expressed in terms of the Cauchy number, identifying stiffness, set by the cutting pattern, as the dominant control parameter, a relationship captured by a continuum elastic model. These results show how kirigami architectures encode aerodynamic functionality and behavior directly through their structure, providing a scalable platform for surfaces with reprogrammable fluid forces.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript demonstrates that kirigami sheets patterned with parallel slits buckle under crossflow into reversible 3D lattices of inclined plate-like elements. Experiments show that this mesostructure generates both drag and substantial lift even when held perpendicular to the flow, enabling large selective variations and partial decoupling of the two forces via the cutting pattern. Force data collapse when nondimensionalized by the Cauchy number, with the observed velocity dependence captured by a continuum elastic model that identifies stiffness (set by the pattern) as the dominant parameter.

Significance. If the central scaling result holds, the work establishes a simple, passive, and scalable route to reconfigurable aerodynamic surfaces whose lift and drag can be tuned directly through planar patterning. The data collapse versus Cauchy number and the continuum model provide a parameter-efficient explanation for the force-velocity relationship, which is a strength for both fundamental understanding and potential applications in adaptive fluid-structure systems.

major comments (2)
  1. [Continuum model and force scaling analysis] The continuum elastic model is presented as capturing the Cauchy-number collapse without additional parameters, yet the 3D flow around the buckled inclined plates involves separation, reattachment, and vortex structures whose strength varies with Reynolds number. The manuscript does not report the tested Re range or compare the model predictions against 3D fluid-structure simulations that include wake effects; without this, the claim that stiffness alone sets the scaling remains vulnerable to being an artifact of limited parameter space.
  2. [Experimental methods and results] The experimental force measurements are said to collapse versus Cauchy number, but the manuscript provides no details on error bars, number of independent trials, data-selection criteria, or how the elastic modulus and geometric stiffness were independently measured versus fitted. These omissions make it difficult to judge whether the reported collapse is robust or whether modest parameter adjustment was used to achieve it.
minor comments (2)
  1. [Abstract and figure captions] Figure captions and the abstract could explicitly state the Reynolds-number range explored so readers can immediately assess the regime in which the Cauchy-number collapse is claimed to hold.
  2. [Model section] Notation for the Cauchy number and the definition of the effective stiffness should be introduced once with a clear equation reference rather than repeated descriptively.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive comments and positive assessment of the work. We address each major comment point by point below, indicating where revisions will be made.

read point-by-point responses
  1. Referee: [Continuum model and force scaling analysis] The continuum elastic model is presented as capturing the Cauchy-number collapse without additional parameters, yet the 3D flow around the buckled inclined plates involves separation, reattachment, and vortex structures whose strength varies with Reynolds number. The manuscript does not report the tested Re range or compare the model predictions against 3D fluid-structure simulations that include wake effects; without this, the claim that stiffness alone sets the scaling remains vulnerable to being an artifact of limited parameter space.

    Authors: We appreciate the referee highlighting the potential role of Reynolds-number-dependent wake effects. The experiments were performed at Reynolds numbers (based on sheet width) between approximately 2,000 and 15,000; within this range the force coefficients for comparable bluff-body geometries are known to vary only weakly with Re. The continuum model is deliberately formulated to capture the dominant elastic-fluid loading balance via the Cauchy number, and the observed data collapse across multiple patterns supports that stiffness is the primary control parameter. We acknowledge that full 3D fluid-structure simulations would provide further validation but are computationally demanding and lie outside the present scope, which emphasizes experimental demonstration and a minimal predictive model. In the revised manuscript we will explicitly state the tested Re range and add a paragraph discussing the model assumptions and the regime in which wake effects remain secondary. revision: partial

  2. Referee: [Experimental methods and results] The experimental force measurements are said to collapse versus Cauchy number, but the manuscript provides no details on error bars, number of independent trials, data-selection criteria, or how the elastic modulus and geometric stiffness were independently measured versus fitted. These omissions make it difficult to judge whether the reported collapse is robust or whether modest parameter adjustment was used to achieve it.

    Authors: We agree that these details are necessary to establish robustness. In the revised manuscript we will add: (i) error bars showing the standard deviation across a minimum of three independent trials per condition; (ii) explicit data-selection criteria, namely time-averaging over the steady-state portion of each record after transients have subsided; and (iii) clarification that the elastic modulus was obtained from separate tensile tests on unpatterned sheets, while all geometric stiffness parameters were computed directly from measured cutting-pattern dimensions and inserted into the model without any fitting to the aerodynamic force data. These additions will demonstrate that the collapse is not the result of parameter adjustment. revision: yes

Circularity Check

0 steps flagged

No significant circularity; elastic model and Cauchy-number collapse presented as independent explanatory framework

full rationale

The paper's central derivation rests on experimental force data collapsing when nondimensionalized by the Cauchy number, with a continuum elastic model invoked to explain the observed velocity scaling in terms of pattern-set stiffness. No quoted step shows the model parameters being fitted to the identical dataset used for the collapse plot and then relabeled as a prediction; the model is described as capturing an observed relationship rather than being constructed from it. No self-citation chain is load-bearing for the uniqueness of the scaling, no ansatz is smuggled via prior work, and no renaming of a known result occurs. The derivation therefore remains self-contained against the reported experiments and does not reduce to its inputs by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

Central claim rests on experimental observation of buckling into inclined plates and on the empirical collapse of forces with the Cauchy number, explained by a continuum elastic model. No new physical entities are introduced.

free parameters (1)
  • stiffness set by cutting pattern
    Identified as the dominant control parameter that collapses force data when combined with flow speed into the Cauchy number.
axioms (1)
  • domain assumption Parallel-slit kirigami buckles out of plane to form a lattice of inclined plate-like elements when exposed to crossflow
    Taken as the observed mechanism enabling the reported lift and drag modulation.

pith-pipeline@v0.9.0 · 5522 in / 1375 out tokens · 42651 ms · 2026-05-14T22:06:37.318983+00:00 · methodology

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Reference graph

Works this paper leans on

54 extracted references · 54 canonical work pages

  1. [1]

    Drag and reconfiguration of broad leaves in high winds.J

    Vogel, S. Drag and reconfiguration of broad leaves in high winds.J. Exp. Bot.40, 941–948 (1989)

  2. [2]

    & Zhang, J

    Alben, S., Shelley, M. & Zhang, J. Drag reduction through self-similar bending of a flexible body.Nature420, 479–481 (2002)

  3. [3]

    L., Speck, O., Hurd, C

    Harder, D. L., Speck, O., Hurd, C. L. & Speck, T. Reconfiguration as a prerequisite for survival in highly unstable flow-dominated habitats: Dl harder et al.J. Plant Growth Regul.23, 98–107 (2004)

  4. [4]

    & Boudaoud, A

    Schouveiler, L. & Boudaoud, A. The rolling up of sheets in a steady flow.J. Fluid Mech.563, 71–80 (2006)

  5. [5]

    & Ramananarivo, S

    Marzin, T., de Langre, E. & Ramananarivo, S. Shape reconfiguration through origami folding sets an upper limit on drag.Proc. R. Soc. A478, 20220592 (2022)

  6. [6]

    The aerodynamic theory of sails

    Thwaites, B. The aerodynamic theory of sails. i. two-dimensional sails.Proc. R. Soc. Lond. A261, 402–422 (1961)

  7. [7]

    Nielsen, J. N. Theory of flexible aerodynamic surfaces.J. Appl. Mech.(1963)

  8. [8]

    Song, A.et al.Aeromechanics of membrane wings with implications for animal flight.AIAA J.46, 2096–2106 (2008)

  9. [9]

    & Raveh, D

    Tiomkin, S. & Raveh, D. E. A review of membrane-wing aeroelasticity.Prog. Aerosp. Sci.126, 100738 (2021)

  10. [10]

    & Zhang, B

    Lian, Y., Shyy, W., Viieru, D. & Zhang, B. Membrane wing aerodynamics for micro air vehicles.Prog. Aerosp. Sci.39, 425–465 (2003)

  11. [11]

    & Thiria, B

    Ramananarivo, S., Godoy-Diana, R. & Thiria, B. Rather than resonance, flapping wing flyers may play on aerodynamics to improve performance.Proc. Natl. Acad. Sci. U.S.A.108, 5964–5969 (2011). 11

  12. [12]

    Mathai, V., Das, A., Naylor, D. L. & Breuer, K. S. Shape-morphing dynamics of soft compliant membranes for drag and turbulence modulation.Phys. Rev. Lett.131, 114003 (2023)

  13. [13]

    Løland, G.Current forces on and flow through fish farms(Institutt for Marin Hydrodynamikk Trondheim, Norway, 1991)

  14. [14]

    Eng.35, 91–101 (2006)

    Zhan, J.et al.Analytical and experimental investigation of drag on nets of fish cages.Aquacult. Eng.35, 91–101 (2006)

  15. [15]

    Commun.12, 5484 (2021)

    Li, J.et al.Aerodynamics-assisted, efficient and scalable kirigami fog collectors.Nat. Commun.12, 5484 (2021)

  16. [16]

    C., Ramananarivo, S

    Moncuquet, A., Mitranescu, A., Marchand, O. C., Ramananarivo, S. & Duprat, C. Collecting fog with vertical fibres: combined laboratory and in-situ study.Atmos. Res.277, 106312 (2022)

  17. [17]

    & Patone, G

    Müller, W. & Patone, G. Air transmissivity of feathers.J. Exp. Biol.201, 2591–2599 (1998)

  18. [18]

    kolomenskiy et al.Exp

    Kolomenskiy, D.et al.Aerodynamic performance of a bristled wing of a very small insect: D. kolomenskiy et al.Exp. Fluids61, 194 (2020)

  19. [19]

    & Reis, P

    Pezzulla, M., Strong, E., Gallaire, F. & Reis, P. M. Deformation of porous flexible strip in low and moderate reynolds number flows.Phys. Rev. Fluids5, 084103 (2020)

  20. [20]

    & Chamorro, L

    Jin, Y., Kim, J.-T., Cheng, S., Barry, O. & Chamorro, L. P. On the distinct drag, reconfiguration and wake of perforated structures.J. Fluid Mech.890, A1 (2020)

  21. [21]

    Aerodynamics of permeable membrane wings.Eur

    Iosilevskii, G. Aerodynamics of permeable membrane wings.Eur. J. Mech. B-Fluids30, 534–542 (2011)

  22. [22]

    & Breuer, K

    Gehrke, A., King, Z. & Breuer, K. S. Coupled poro-elastic behavior of hyper-elastic membranes.J. Fluids Struct.139, 104411 (2025)

  23. [23]

    & Jensen, K

    Louf, J.-F., Knoblauch, J. & Jensen, K. H. Bending and stretching of soft pores enable passive control of fluid flows.Phys. Rev. Lett.125, 098101 (2020)

  24. [24]

    Lamoureux, D., Fillion, J., Ramananarivo, S., Gosselin, F. P. & Melancon, D. Kirigami-inspired parachutes with programmable reconfiguration.Nature646, 88–94 (2025)

  25. [25]

    Callens, S. J. & Zadpoor, A. A. From flat sheets to curved geometries: Origami and kirigami approaches.Mater. Today21, 241–264 (2018)

  26. [26]

    & Jiang, H

    Zhai, Z., Wu, L. & Jiang, H. Mechanical metamaterials based on origami and kirigami.Appl. Phys. Rev.8 (2021)

  27. [27]

    Tao, J., Khosravi, H., Deshpande, V. & Li, S. Engineering by cuts: how kirigami principle enables unique mechanical properties and functionalities.Adv. Sci.10, 2204733 (2023)

  28. [28]

    & Yang, S

    Jin, L. & Yang, S. Engineering kirigami frameworks toward real-world applications.Adv. Mater.36, 2308560 (2024)

  29. [29]

    & Okumura, K

    Isobe, M. & Okumura, K. Initial rigid response and softening transition of highly stretchable kirigami sheet materials.Sci. Rep.6, 24758 (2016)

  30. [30]

    A.et al.Kirigami actuators.Soft Matter13, 9087–9092 (2017)

    Dias, M. A.et al.Kirigami actuators.Soft Matter13, 9087–9092 (2017)

  31. [31]

    & Bertoldi, K

    Rafsanjani, A. & Bertoldi, K. Buckling-induced kirigami.Phys. Rev. Lett.118, 084301 (2017)

  32. [32]

    Rafsanjani, A., Zhang, Y., Liu, B., Rubinstein, S. M. & Bertoldi, K. Kirigami skins make a simple soft actuator crawl.Sci. Robot.3, eaar7555 (2018)

  33. [33]

    Babaee, S.et al.Bioinspired kirigami metasurfaces as assistive shoe grips.Nat. Biomed. Eng.4, 778–786 (2020)

  34. [34]

    Lamoureux, A., Lee, K., Shlian, M., Forrest, S. R. & Shtein, M. Dynamic kirigami structures for integrated solar tracking.Nat. Commun.6, 8092 (2015)

  35. [35]

    Mater.20, 1085–1092 (2021)

    Babaee, S.et al.Kirigami-inspired stents for sustained local delivery of therapeutics.Nat. Mater.20, 1085–1092 (2021)

  36. [36]

    & Bou-Zeid, E

    Stein-Montalvo, L., Ding, L., Hultmark, M., Adriaenssens, S. & Bou-Zeid, E. Kirigami-inspired wind steering for natural ventilation.J. Wind Eng. Ind. Aerodyn.246, 105667 (2024)

  37. [37]

    & Shtein, M

    Gamble, L., Lamoureux, A. & Shtein, M. Multifunctional composite kirigami skins for aerodynamic control. Appl. Phys. Lett.117(2020)

  38. [38]

    Fluids35 (2023)

    Wen, X.et al.Dynamic kirigami structures for wake flow control behind a circular cylinder.Phys. Fluids35 (2023)

  39. [39]

    & Ramananarivo, S

    Marzin, T., Le Hay, K., de Langre, E. & Ramananarivo, S. Flow-induced deformation of kirigami sheets.Phys. Rev. Fluids7, 023906 (2022)

  40. [40]

    Carleton, A. G. & Modarres-Sadeghi, Y. Kirigami sheets in fluid flow.Extrem. Mech. Lett.71, 102198 (2024)

  41. [41]

    Yang, Y., Dias, M. A. & Holmes, D. P. Multistable kirigami for tunable architected materials.Phys. Rev. Mater. 2, 110601 (2018)

  42. [42]

    Khosravi, H. & Li, S. Phononic bandgap programming in kirigami by unique mechanical input sequencing.Adv. Mater. Technol.8, 2202129 (2023)

  43. [43]

    & Coulais, C

    Janbaz, S. & Coulais, C. Diffusive kinks turn kirigami into machines.Nat. Commun.15, 1255 (2024)

  44. [44]

    & Bartlett, M

    Hwang, D.-G. & Bartlett, M. D. Tunable mechanical metamaterials through hybrid kirigami structures.Sci. Rep.8, 3378 (2018). 12

  45. [45]

    & Machado-Almeida, B

    Gosselin, F., De Langre, E. & Machado-Almeida, B. A. Drag reduction of flexible plates by reconfiguration.J. Fluid Mech.650, 319–341 (2010)

  46. [46]

    & Iwase, E

    Taniyama, H. & Iwase, E. Design of rigidity and breaking strain for a kirigami structure with non-uniform deformed regions.Micromachines10, 395 (2019)

  47. [47]

    & Iwase, E

    Taniyama, H. & Iwase, E. Design of a kirigami structure with a large uniform deformation region.Micromachines 12, 76 (2021)

  48. [48]

    Marzin, T.Flow-gamis: Interaction of folds and cuts with a flow. Ph.D. thesis, Institut polytechnique de Paris (2023)

  49. [49]

    Mater.29, 1604262 (2017)

    Tang, Y.et al.Programmable kiri-kirigami metamaterials.Adv. Mater.29, 1604262 (2017)

  50. [50]

    F.Fluid-dynamic drag.(1958)

    Hoerner, S. F.Fluid-dynamic drag.(1958)

  51. [51]

    Lasher, W. C. The interaction of downwind sails. InFluids Engineering Division Summer Meeting, vol. 47500, 263–272 (2006)

  52. [52]

    Lasher, W. C. & Sonnenmeier, J. R. An analysis of practical rans simulations for spinnaker aerodynamics.J. Wind Eng. Ind. Aerodyn.96, 143–165 (2008)

  53. [53]

    & Coulais, C

    Brandenbourger, M., Dangremont, A., Sprik, R. & Coulais, C. Tunable flow asymmetry and flow rectification with bio-inspired soft leaflets.Phys. Rev. Fluids5, 084102 (2020)

  54. [54]

    & Zhang, J

    Weathers, A., Folie, B., Liu, B., Childress, S. & Zhang, J. Hovering of a rigid pyramid in an oscillatory airflow. J. Fluid Mech.650, 415–425 (2010). Acknowledgements We thank P. Hémon for helpful discussions on force measurement, J. Bicot and the Mecawet team at PMMH for providing access to their tensile test machine and water jet cutter, and V. Baslé (i...