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International audience; We investigate freely expanding sheets formed by ultrasoft gel beads, and liquid and viscoelastic drops, produced by the impact of the bead or drop on a silicon wafer covered with a thin layer of liquid nitrogen that suppresses viscous dissipation thanks to an inverse Leidenfrost effect. Our experiments show a unified behavior for the impact dynamics that holds for solids, liquids, and viscoelastic fluids and that we rationalize by properly taking into account elastocapillary effects. In this framework, the classical impact dynamics of solids and liquids, as far as viscous dissipation is negligible, appears as the asymptotic limits of a universal theoretical description. A novel material-dependent characteristic velocity that includes both capillary and bulk elasticity emerges from this unified description of the physics of impact.

International audience; We study experimentally the impact of ultra soft spherical gel balls of millimetric size d0 on a rigid substrate covered by a thin layer of liquid nitrogen to avoid viscous dissipation .The balls largely deform like a pancake at high impact velocities. We measure the maximally deformed size dmax and the the time needed to reach this maximal size after impact Tmax, versus the impact velocity Ui for various elastic moduli . We do the same type of experiments with liquid droplets of various surface tensions . The experiments reveal a universal scaling behavior of the maximum deformation $\d_{max}/d_0}$ of both solid balls and liquid drops provided that both bulk and surface elasticity are properly taken into account. Moreover, we show that , in absence of viscous dissipation, the dynamics of the system can be understood as a conventional spring-mass system with a stiffness given by a combination of surface tension and bulk elasticity and a mass given by that of the ball (or drop) ; the deformation of the small ball (drop) during the impact linearly depends on the impact velocity, and the contact time scales as the period of this spring-mass system.

International audience; In our work we report the measurement of non-equilibrium interfacial tension of polymer and hard sphere suspensions in contact with their own solvent. By visualizing fingering instability (VF) in radial Hele-Shaw geometry, appearing when the solvent displaces suspensions of colloids or polymers, we measure interfacial tensions in function of the volume fraction of the suspended objects, showing that the internal degrees of freedom of the particles drive the low volume fraction behavior (Figure 1). Our results support the existence of a positive tension between miscible fluids, confirm the quadratic scaling predicted by Korteweg [4] for long linear and crosslinked polymers and show a positive rapidly growing tension for hard sphere suspensions up to maximum packing, whose description necessitates a theoretical framework going beyond the classic square gradient model. We rationalize our findings assuming the suspension/solvent interface in local thermodynamic equilibrium, computing explicitly the square gradient contribution to the interfacial tension for polymer/solvent and simple molecular liquid mixtures and proposing a phenomenological model capturing the compositional dependence of the interfacial tension for large concentration gradients. Finally we include and analyze data reported in literature and obtained via spinning drop tensiometry that validate the model and we propose the analysis of fluid dynamic instability as a new tool to probe interfacial stresses.

We report the measurement of non-equilibrium interfacial tension of polymer and hard sphere suspensions in contact with their own solvent. By visualizing fingering instability (VF) in radial Hele-Shaw geometry, we measure interfacial tension in function of the volume fraction of the suspensions showing that the internal degrees of freedom of the particles drive the magnitude of such tension. We rationalize our findings proposing a phenomenological model capturing the compositional dependence of the non equilibrium interfacial tension for the whole range of concentration gradients and for all the systems at hand. More generally we propose the analysis of fluid dynamic instabilities as a new tool to measure interfacial tensions between complex fluids.

The nature of the interface between two fluids has been the subject of an extensive investigation for more than two centuries [1]. From a mechanical point of view, surface tension can be calculated as an integral of unbalanced tangential stresses over the interface thickness [2] and it is thus of no surprise that, within the assumption of temporal and local equilibrium, such a tension can be ascribed to an interface between two miscible fluids [3] and assumes a nonzero value. The idea that there are capillary forces at work in the layer between miscible liquids goes back at least to an 1871 report of J. Bosscha, cited in a paper of Korteweg [1901], who was the first [4] to introduce stresses due to concentration inhomogeneities in the Navier-Stokes equation, aiming to mimic capillarity effects between two miscible liquids. Only much more recently experimental effort has been made to investigate the existence and the nature (the sign) of such off-equilibrium tension [5-11]. In all cases the authors have pointed out that such interfacial stresses mimic a positive interfacial tension. In analogy with the surface tension of an equilibrium interface between immiscible fluids, the effective surface tension has been rationalized within an approximation of small concentration gradients via the so called square gradient model [6,8,9]. The latter predicts a quadratic dependence of such tension on the compositional mismatch between two miscible fluids.Only very recently colloids and polymer suspensions in contact with a reservoir of solvent have been considered as a model two-fluid system to study off-equilibrium surface tensions [11, 12]: indeed, diffusion is much slower in colloids and polymers as compared to atomic systems, leaving a wider temporal window for probing the transient interface between miscible fluids. In a recent work [11] we have investigated off-equilibrium surface tension between microgel suspensions and their solvent (water) showing that equation (1) holds for low concentration gradients. On the other hand we have also pointed out that the square gradient model is far to catch the volume fraction dependence of the tension for compact hard sphere-like particles [12] up to concentrations close to the maximum packing for spheres. The scenario is then currently controversial.By visualizing viscous fingering instability (VF), appearing when a solvent displaces a suspension in radial Hele-Shaw geometry, we measure interfacial tensions in function of the volume fraction of the suspended colloids or polymers, showing that the internal degrees of freedom of the particles drive the low volume fraction behavior. Our results support the existence of a positive tension between miscible fluids, confirm the quadratic scaling predicted by Korteweg [4] for long linear and crosslinked polymers and show a positive rapidly growing tension for hard sphere suspensions, whose description necessitates a theoretical framework going beyond the classic square gradient model. We rationalize our findings assuming the suspension/solvent interface in local thermodynamic equilibrium, computing explicitly the square gradient contribution to the interfacial tension for polymer/solvent and simple molecular liquid mixtures and proposing a new phenomenological model capturing the compositional dependence of the interfacial tension for large concentration gradients. In addition to that we include and analyze data reported in literature and obtained via spinning drop tensiometry, validating our approach. We conclude proposing very generally the analysis of hydrodynamic instabilities as a new tool to measure interfacial stresses in complex fluids and characterize transient interfacial tensions.

We consider a dilute system of small hard beads or hard fibers immersed in a very soft gel able to withstand large elastic deformations. Because of its low to very low shear modulus, this system is very sensitive to small forces. We calculate the local deformation induced by a constant volume force, the inclusion weight. We explain how this deformation could be put in evidence by using techniques similar to the PIV method (particle image velocimetry) used to show complex velocity fields in transparent fluids.