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Surface Tension Scars Soft Solids

    John Kolinski

    • Swiss Federal Institute of Technology (EPFL), Engineering Mechanics of Soft Interfaces, Lausanne, Switzerland

• Physics 14, 110

A mechanism arising from liquid wetting may cause a folded area in a mushy stable to stay caught to itself on the microscale, leading to scars on the fabric floor that may information its morphological evolution.

Valentina R./inventory.adobe.com

Figure 1: A mechanism arising from liquid wetting on an uneven floor can clarify the creases that kind in mushy solids together with organic tissues like fruit, pores and skin, and even brains.

In every day life, we’re surrounded by mushy supplies. Most organic tissue includes supplies which are mushy, which means that they readily deform below typical mechanical stresses. Large deformations of soppy solids result in advanced morphologies that come up when the free floor succumbs, accordion-like, to a compressive power. Under sufficient compressive pressure, a free interface will bend right into a crease, producing deep, folded valleys and, in the end, areas of self-contacting surfaces. Creases fashioned through compression in organic tissues permeate nature and embody the sulci of the mind and the folds of a bent elbow. Such creases typically persist within the type of a everlasting “scar” on the floor of the mushy materials. However, regardless of the ubiquity of such options, it isn’t clear why scars stay as soon as the stress is relaxed. Nor is it clear why creases kind at a selected location in a homogenous materials that’s compressed uniformly. Michiel van Limbeek, of the Max Planck Institute for Dynamics and Self-Organization in Germany, and his colleagues [1] now discover that mushy supplies subjected to repeated cycles of deformation develop scars from a folding-unfolding asymmetry resulting from liquid wetting (Fig. 1).

One risk that has beforehand been proposed to elucidate the looks and persistence of scars on mushy solids is a mechanism seen in different techniques, corresponding to folded or crumpled paper [2, 3]. In these instances, everlasting weakening or harm alters the fabric’s mechanical properties domestically, leaving particular websites weak to subsequent creasing. Alternatively, adhesion between the 2 sides of a fold may trigger the surfaces within the crease to stay collectively, producing a configuration that is still even when the stress is eliminated. But neither plastic deformation nor adhesion can account for sensitivity to liquid-solid floor rigidity.

To perceive the phenomenon of creases in mushy supplies, van Limbeek and his colleagues carried out an experiment involving a layer of soppy polymer gel deposited on prime of a pre-stretched rubber sheet. The mushy polymer gel was then immersed in liquids with larger or lesser floor rigidity. By step by step enjoyable the stress on the rubber sheet, they compressed the gel layer uniformly, one micrometer at a time. Eventually, the gel floor started to bend, in the end forming a crease as the 2 sides of the bend got here into contact with one another. Then the researchers launched the compression step by step and noticed how the floor uncreased—and the way it didn’t—when the gel was immersed in numerous liquids.

Observations of the gel’s floor morphology with confocal microscopy allowed the researchers to measure immediately the extent and angle of the gel’s deformation on the crease. Fluorescently labeled nanoparticles affixed to the gel’s floor highlighted the gel-liquid interface, making it doable to observe the crease constantly as the 2 sides of the crease made contact and have become in any other case inaccessible to direct measurement.

The experiments confirmed a hysteresis within the crease’s response to compression and leisure. Specifically, the depth of the crease for a given pressure relied on whether or not the gel was within the compression or leisure phase of the cycle. Such a end result can be anticipated if the system’s dynamics had been managed by adhesion between the 2 sides. However, adhesion alone can not clarify the way in which the floor profile modified whereas the complete vary of compression was utilized and eliminated when the gel was immersed in numerous fluids. Under compression, the crease in cross part resembled the letter Y, with the Y’s “stalk” representing the self-contacting area and the “arms” representing the folded floor of the gel. When the compression was relaxed, the crease appeared extra just like the letter T, with the floor bending sharply into the world of self-contact (Fig. 2). The totally different shapes recommend that the unfolding course of required extra power than was wanted to kind the crease within the first place when the floor rigidity elevated. This power distinction might be accounted for by the necessity to overcome surface-tension forces along with adhesion between the 2 sides.

Figure 2: When a mushy materials is compressed, the floor comes into contact with itself and types a crease after some important pressure 𝜖c. When the pressure 𝜖 is launched and the floor uncreases, the floor doesn’t fully unfold. Instead, a pinned contact line types a scar. The crease stays pinned such that in unfolding it doesn’t cut back the scale of the self-contact area by a size ΔL. Instead, due to floor rigidity, the scar stays on the floor even when 𝜖 returns to 0.When a mushy materials is compressed, the floor comes into contact with itself and types a crease after some important pressure 𝜖c. When the pressure 𝜖 is launched and the floor uncreases, the floor doesn’t fully unfold. Instead, a pinned conta… Show more

The researchers suggest that the function of floor rigidity on this system parallels a phenomenon widespread in interfacial fluid mechanics often called contact-line pinning. When a liquid-air interface meets a stable floor—corresponding to a liquid droplet resting on a tabletop—the three-phase junction types what’s often called a contact line. The angle between the tabletop and the tangent to the liquid-air interface can be utilized to measure floor rigidity when the droplet is at equilibrium. When not at equilibrium, this stress drives the contact line to maneuver; nonetheless, due to tiny floor heterogeneities, the contact-line movement is usually not easy. Experiments present that on the smallest scales, contact traces shift in matches and begins as a result of they continue to be domestically caught or pinned in place [4]. Van Limbeek’s end result reveals that this identical pinning of a contact line is liable for the persistence of creases on mushy solids.

As techniques that exhibit strongly nonlinear habits and huge deformation, creases and interfacial folds have develop into helpful instruments for probing questions as mundane as “why does desiccated fruit wrinkle?” and as wealthy as “why does the brain have folds?” [5]. By figuring out one other nonlinear phenomenon that arises from contact-line pinning, van Limbeek and his colleagues have added to that investigative toolbox.

The discovery of another mechanism for floor scarring in an analogous (although not mechanically an identical) technique to how paper creases when repeatedly crumpled [6] might even have sensible functions—for instance, in soft-robotics units that fold [7] or in floor engineering for fluid transport [8]. Indeed, one might envision manipulating the floor rigidity of soppy solids to “program” their creasing sample with a view to controlling the transport of liquids over such surfaces. Manipulating the native floor rigidity of a mushy materials that may develop by swelling may additionally supply a technique to direct its morphological evolution, thus guiding a swelling floor to tackle a desired form [9]. By figuring out the important thing function of contact-line pinning within the formation of such creases, van Limbeek and colleagues have opened the door for such functions.


  1. M. A. J. van Limbeek et al., “Pinning-induced folding-unfolding asymmetry in adhesive creases,” Phys. Rev. Lett. 127, 028001 (2021).
  2. T. Tallinen et al., “The effect of plasticity in crumpling of thin sheets,” Nat. Mater. 8, 25 (2008).
  3. O. Gottesman et al., “Furrows in the wake of propagating d-cones,” Nat. Commun. 6, 7232 (2015).
  4. D. M. Kaz et al., “Physical ageing of the contact line on colloidal particles at liquid interfaces,” Nat. Mater. 11, 138 (2011).
  5. E. Hohlfeld and L. Mahadevan, “Unfolding the sulcus,” Phys. Rev. Lett. 106, 105702 (2011).
  6. J. Andrejevic et al., “A model for the fragmentation kinetics of crumpled thin sheets,” Nat. Commun. 12, 1470 (2021).
  7. A. Firouzeh and J. Paik, “Robogami: A fully integrated low-profile robotic origami,” J. Mech. Robot. 7, 021009 (2015).
  8. M. Coux and J. M. Kolinski, “Surface textures suppress viscoelastic braking on soft substrates,” Proc. Natl. Acad. Sci. U.S.A. 117, 32285 (2020).
  9. Y. Klein et al., “Shaping of elastic sheets by prescription of non-Euclidean metrics,” Science 315, 1116 (2007).

About the Author

Image of John Kolinski

John Kolinski studied utilized arithmetic (Sc.M.) and utilized physics (Ph.D.) at Harvard University, finishing a Ph.D. below the supervision of L. Mahadevan and Shmuel Rubinstein on the function of air in droplet influence. John did his postdoc on the Hebrew University of Jerusalem in Israel (HUJI) supported by the Fulbright postdoctoral fellowship. At HUJI, he labored on interfacial instabilities in mushy matter within the labs of Eran Sharon and Jay Fineberg. John continues his analysis on interfacial mechanics on the Swiss Federal Institute of Technology (EPFL) in his newly based laboratory for the research of engineering mechanics of soppy interfaces.

Subject Areas

Soft MatterMaterials Science

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