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REVIEW 2 major objections 2 minor 20 references

Tensile wrinkling and creasing of an elastic half-space under a suction load

T0 review · 2 major / 2 minor · reviewed 2026-06-30 · grok-4.3

Pith's one-line read Suction on an elastic half-space produces tensile wrinkling and creasing while pressure does not.

desk verdict Suction on a neo-Hookean half-space produces tensile wrinkling and creasing while equal pressure does not, reversing the dead-load pattern under standard assumptions. read the letter →

arxiv 2605.24039 v1 pith:2LU4H2C4 submitted 2026-05-21 physics.class-ph

classification physics.class-ph
keywords elastichalf-spacewrinklingcreasingsuctionneo-Hookeansurfaceinstabilitytensileprestressedelasticity
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper analyzes an elastic half-space under uniform surface pressure or suction, modeled as incompressible neo-Hookean material with induced uniaxial prestress. No wrinkling or creasing occurs under compressive pressure, but both instabilities appear when the load reverses to suction and produces tension. This outcome differs from the instabilities that arise under dead-load compression at infinity. Biaxial prestress admits certain loading paths that remain stable even as loads grow without bound. The sign of the surface load therefore controls whether surface instabilities are promoted or delayed.

What carries the argument

Uniaxial or biaxial prestress state induced throughout the half-space by uniform surface pressure or suction, used to detect bifurcation into wrinkled or creased surface modes.

What would settle it

An experiment on a soft gel or rubber half-space that shows wrinkling under positive pressure or no wrinkling under suction would falsify the central claim.

Watch

Extended reading notes

Core claim

With reference to incompressible neo-Hookean elasticity and assuming the prevalence of a uniaxial prestress state induced by the application of a uniform pressure, no wrinkling or creasing is foreseen, whereas they do when reversing the sign of pressure, which is then a suction, thus leading to tensile creasing and tensile wrinkling. When a biaxial prestress state is considered, it is shown that some loading paths can be envisaged, able to grow to infinity without causing any instability.

Load-bearing premise

A uniform surface pressure or suction is assumed to produce a uniform uniaxial or biaxial prestress state throughout the half-space in an incompressible neo-Hookean material.

Editorial extensions

If this is right

  • Suction produces tensile creasing and tensile wrinkling.
  • Positive pressure produces no wrinkling or creasing under uniaxial prestress.
  • Some biaxial loading paths remain stable at arbitrarily large loads.
  • The sign of surface pressure can promote or delay surface instabilities.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The result may explain how fluid suction in biological tissues could induce surface patterns without overall compression.
  • In microfluidic devices, reversing pressure sign could be used to trigger or suppress wrinkling at fluid-solid interfaces.
  • Direct experiments applying controlled suction to thick soft elastic blocks would test whether tensile surface modes appear as predicted.
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Signed reviews

No signed human review yet.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

2 major / 2 minor

Summary. The manuscript analyzes wrinkling and creasing of an incompressible neo-Hookean elastic half-space under uniform surface pressure versus suction. It claims that a compressive uniaxial prestress from pressure produces no instabilities, while the tensile prestress from suction produces both wrinkling and creasing; for biaxial prestress, selected loading paths remain stable to infinite load. The work concludes that the sign of the surface traction can either promote or suppress surface instabilities.

Significance. If the central claim is correct, the result is significant: it reverses the standard expectation (Biot-type compressive wrinkling) that surface instabilities require compression. The analysis employs only the standard incompressible neo-Hookean law and homogeneous prestress without fitted parameters or invented entities, which strengthens the finding. Potential implications for mechanobiology and microfluidic fluid-structure interaction are noted.

major comments (2)
  1. [§3] §3 (base-state construction): the reduction of uniform surface traction to a homogeneous uniaxial prestress throughout the half-space is asserted without an explicit verification that div σ = 0, the traction condition σ_zz = −p at z = 0, and decay at depth are simultaneously satisfied for both signs of p; this step is load-bearing for the subsequent claim that only suction triggers instability.
  2. [§4.2] §4.2 (linear stability): the dispersion relation for the tensile (suction) case is stated to admit unstable modes, yet the incremental boundary-value problem is not shown to enforce both the perturbed traction condition at z = 0 and the decay condition at depth; without these equations the tensile instability cannot be confirmed to follow from the constitutive assumptions alone.
minor comments (2)
  1. Notation for the prestress components (σ_xx^0, σ_zz^0) is introduced without a table or explicit listing of their values for pressure versus suction cases.
  2. Figure 2 caption refers to 'growth rate' but the axis label is missing the non-dimensionalization factor used in the dispersion relation.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and for the constructive comments. We appreciate the recognition of the potential significance of the finding that the sign of surface traction can promote or suppress instabilities. We address each major comment below and will incorporate the requested clarifications in a revised version.

read point-by-point responses
  1. Referee: [§3] §3 (base-state construction): the reduction of uniform surface traction to a homogeneous uniaxial prestress throughout the half-space is asserted without an explicit verification that div σ = 0, the traction condition σ_zz = −p at z = 0, and decay at depth are simultaneously satisfied for both signs of p; this step is load-bearing for the subsequent claim that only suction triggers instability.

    Authors: We agree that an explicit verification strengthens the presentation. The homogeneous uniaxial prestress field satisfies div σ = 0 identically, as the stress components are constant. The surface traction condition σ_zz = −p is satisfied by direct imposition at z = 0 for either sign of p. Because the surface traction is uniform over an infinite plane, the homogeneous field is the exact solution throughout the half-space; it is compatible with the far-field condition, while any incremental fields are required to decay with depth. We will add a short verification paragraph in §3 covering both pressure and suction cases. revision: yes

  2. Referee: [§4.2] §4.2 (linear stability): the dispersion relation for the tensile (suction) case is stated to admit unstable modes, yet the incremental boundary-value problem is not shown to enforce both the perturbed traction condition at z = 0 and the decay condition at depth; without these equations the tensile instability cannot be confirmed to follow from the constitutive assumptions alone.

    Authors: We accept that the incremental boundary-value problem should be stated explicitly. In the revision we will present the full incremental equations, the linearized traction conditions at the perturbed surface z = 0, and the decay requirements as z → ∞. This will confirm that the dispersion relation and the unstable modes for suction follow directly from the incompressible neo-Hookean constitutive law and the boundary conditions. The added detail will not change the reported results. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity; derivation is self-contained

full rationale

The paper's base state follows directly from equilibrium (div σ = 0), traction BC σ_zz = −p at z=0, decay at depth, and incompressible neo-Hookean response, yielding homogeneous uniaxial prestress without fitted parameters or self-reference. Linear stability analysis then produces the sign-dependent instability threshold as a standard consequence of the constitutive model and prestress sign; no algebraic reduction to inputs by construction, no load-bearing self-citations, and no ansatz smuggling is visible. This matches the expected non-circular outcome for a standard incremental analysis.

Assumptions & free parameters 0 free parameters · 2 assumptions · 0 invented entities

The central claim rests on two standard domain assumptions in nonlinear elasticity; no free parameters or new entities are introduced in the abstract.

assumptions (2)
  • domain assumption The material is incompressible neo-Hookean
    Explicitly referenced in the abstract as the constitutive model for the half-space.
  • domain assumption Uniform surface pressure or suction produces a uniaxial or biaxial prestress state
    Invoked to analyze the uniaxial case and to identify stable biaxial loading paths.

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Cite this review

Pith. "Pith review of Tensile wrinkling and creasing of an elastic half-space under a suction load." pith.science (2026). https://pith.science/paper/2LU4H2C4

@misc{pith2026260524039,
  author       = {Pith},
  title        = {Pith review of: Tensile wrinkling and creasing of an elastic half-space under a suction load},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/2LU4H2C4}},
  note         = {Machine review of arXiv:2605.24039}
}
read the original abstract

A famous and thoroughly investigated instability set-up, susceptible to wrinkling and creasing, consists of an elastic half-space being prestressed under a dead load, applied at infinity and, possibly, on its surface. We consider the case of a pressure or a suction applied on the surface and show that wrinkling and creasing occur in a surprising way, completely different from dead load. With reference to incompressible neo-Hookean elasticity and assuming the prevalence of a uniaxial prestress state induced by the application of a uniform pressure, no wrinkling or creasing is foreseen, whereas -- unexpectedly -- they do when reversing the sign of pressure, which is then a suction, thus leading to tensile creasing and tensile wrinkling. When a biaxial prestress state is considered, it is shown that some loading paths can be envisaged, able to grow to infinity without causing any instability. Consequently, we suggest that, according to its sign, pressure can promote or delay surface instabilities, a finding which may have implications for mechanobiology or microfluidic fluid-structure interaction.

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

20 extracted references · 20 canonical work pages

  1. [1]

    Biot, Surface instability of rubber in compression, Appl

    M.A. Biot, Surface instability of rubber in compression, Appl. Sci. Res. Sect. A 12 (1963) 168–182

  2. [2]

    Biot, Mechanics of Incremental Deformations, John Wiley & Sons, Inc., 1965

    M.A. Biot, Mechanics of Incremental Deformations, John Wiley & Sons, Inc., 1965

  3. [3]

    Benallal, R

    A. Benallal, R. Billardon, G. Geymonat, Bifurcation and localization in rate- independent materials. Some general considerations, in: Q.S. Nguyen (Ed.), Bifurcation and Stability of Dissipative Systems, Springer Vienna, Vienna, 1993, pp. 1–44

  4. [4]

    Bigoni, Nonlinear Solid Mechanics: Bifurcation Theory and Material Instability, Cambridge University Press, 2012

    D. Bigoni, Nonlinear Solid Mechanics: Bifurcation Theory and Material Instability, Cambridge University Press, 2012

  5. [5]

    Dowaikh, R.W

    M.A. Dowaikh, R.W. Ogden, On surface waves and deformations in a pre-stressed incompressible elastic solid, IMA J. Appl. Math. 44 (3) (1990) 261–284

  6. [6]

    Hayes, R.S

    M. Hayes, R.S. Rivlin, Surface waves in deformed elastic materials, Arch. Ration. Mech. Anal. 8 (1961) 358–380

  7. [7]

    R. Hill, J. Hutchinson, Bifurcation phenomena in the plane tension test, J. Mech. Phys. Solids 23 (4) (1975) 239–264

  8. [8]

    Tanaka, S.T

    T. Tanaka, S.T. Sun, Y. Hirokawa, S. Katayama, J. Kucera, Y. Hirose, T. Amiya, Mechanical instability of gels at the phase transition, Nature 325 (1987) 796–798

Show all 20 references
  1. [9]

    Gent, I.S

    A.N. Gent, I.S. Cho, Surface instabilities in compressed or bent rubber blocks, Rubber Chem. Technol. 72 (1999) 253–262

  2. [10]

    Hohlfeld, L

    E. Hohlfeld, L. Mahadevan, Unfolding the sulcus, Phys. Rev. Lett. 106 (2011) 105702

  3. [11]

    Y. Cao, J. Hutchinson, From wrinkles to creases in elastomers: The instability and imperfection-sensitivity of wrinkling, R. Soc. Lond. Proc. Ser. A 468 (2011) 94–115

  4. [12]

    Ciarletta, Matched asymptotic solution for crease nucleation in soft solids, Nat

    P. Ciarletta, Matched asymptotic solution for crease nucleation in soft solids, Nat. Commun. 9 (2018) 496

  5. [13]

    Ciarletta, L

    P. Ciarletta, L. Truskinovsky, Soft nucleation of an elastic crease, Phys. Rev. Lett. 122 (2019) 248001

  6. [14]

    Pandurangi, A

    S.S. Pandurangi, A. Akerson, R.S. Elliott, T.J. Healey, N. Triantafyllidis, Nucle- ation of creases and folds in hyperelastic solids is not a local bifurcation, J. Mech. Phys. Solids 160 (2022) 104749

  7. [15]

    W. Hong, X. Zhao, Z. Suo, Formation of creases on the surfaces of elastomers and gels, Appl. Phys. Lett. 95 (11) (2009) 111901

  8. [16]

    Rossi, G

    M. Rossi, G. Cicconofri, A. Beran, G. Noselli, A. DeSimone, Kinematics of flagellar swimming in euglena gracilis: Helical trajectories and flagellar shapes, Proc. Natl. Acad. Sci. 114 (50) (2017) 13085–13090

  9. [17]

    Sareh, J.M

    S. Sareh, J.M. Rossiter, A.T. Conn, K. Drescher, R.E. Goldstein, Swimming like algae: Biomimetic soft artificial cilia, J. R. Soc. Interface 10 (2013)

  10. [18]

    Cicconofri, V

    G. Cicconofri, V. Damioli, G. Noselli, Nonreciprocal oscillations of polyelectrolyte gel filaments subject to a steady and uniform electric field, J. Mech. Phys. Solids 173 (2023) 105225

  11. [19]

    Ben Amar, Wrinkles, creases, and cusps in growing soft matter, Rev

    M. Ben Amar, Wrinkles, creases, and cusps in growing soft matter, Rev. Modern Phys. 97 (2025) 015004

  12. [20]

    P. Yang, Y. Fang, Y. Yuan, S. Meng, Z. Nan, H. Xu, H. Imtiaz, B. Liu, H. Gao, A perturbation force based approach to creasing instability in soft materials under general loading conditions, J. Mech. Phys. Solids 151 (2021) 104401. Extreme Mechanics Letters 85 (2026) 102481 7

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Reviewed June 30, 2026 · model on record in the stance chip above.