REVIEW 2 major objections 2 minor 20 references
Suction on an elastic half-space produces tensile wrinkling and creasing while pressure does not.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.3
2026-06-30 16:16 UTC pith:2LU4H2C4
load-bearing objection 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. the 2 major comments →
Tensile wrinkling and creasing of an elastic half-space under a suction load
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
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.
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.
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.
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.
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.
Where Pith is reading between the lines
- 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.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
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)
- [§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.
- [§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)
- 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.
- 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
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
-
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
-
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
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.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption The material is incompressible neo-Hookean
- domain assumption Uniform surface pressure or suction produces a uniaxial or biaxial prestress state
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.
Reference graph
Works this paper leans on
-
[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
work page 1963
-
[2]
Biot, Mechanics of Incremental Deformations, John Wiley & Sons, Inc., 1965
M.A. Biot, Mechanics of Incremental Deformations, John Wiley & Sons, Inc., 1965
work page 1965
-
[3]
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
work page 1993
-
[4]
D. Bigoni, Nonlinear Solid Mechanics: Bifurcation Theory and Material Instability, Cambridge University Press, 2012
work page 2012
-
[5]
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
work page 1990
-
[6]
M. Hayes, R.S. Rivlin, Surface waves in deformed elastic materials, Arch. Ration. Mech. Anal. 8 (1961) 358–380
work page 1961
-
[7]
R. Hill, J. Hutchinson, Bifurcation phenomena in the plane tension test, J. Mech. Phys. Solids 23 (4) (1975) 239–264
work page 1975
-
[8]
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
work page 1987
- [9]
-
[10]
E. Hohlfeld, L. Mahadevan, Unfolding the sulcus, Phys. Rev. Lett. 106 (2011) 105702
work page 2011
-
[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
work page 2011
-
[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
work page 2018
-
[13]
P. Ciarletta, L. Truskinovsky, Soft nucleation of an elastic crease, Phys. Rev. Lett. 122 (2019) 248001
work page 2019
-
[14]
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
work page 2022
-
[15]
W. Hong, X. Zhao, Z. Suo, Formation of creases on the surfaces of elastomers and gels, Appl. Phys. Lett. 95 (11) (2009) 111901
work page 2009
- [16]
-
[17]
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)
work page 2013
-
[18]
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
work page 2023
-
[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
work page 2025
-
[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
work page 2021
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.