Université PSL



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Micro fl uidic actuators based on temperature-responsive hydrogels
Laboratoire Microfluidique MEMS et nanostructures - Loïc D'Eramo, Benjamin Chollet, Marie Leman, Ekkachai Martwong, Mengxing Li, Hubert Geisler, Jules Dupire, Margaux Kerdraon, Clémence Vergne, Fabrice Monti, Yvette Tran and Patrick Tabeling
- 4 17069 - doi:10.1038/micronano.2017.69 - 2019
The concept of using stimuli-responsive hydrogels to actuatefluids in microfluidic devices is particularly attractive, but limitations,in terms of spatial resolution, speed, reliability and integration, have hindered its development during the past two decades. By patterning and grafting poly(N-isopropylacrylamide) PNIPAM hydrogel films on plane substrates with a 2μm horizontal resolution and closing the system afterward, we have succeeded in unblocking bottlenecks that thermo-sensitive hydrogel technology has
been challenged with until now. In this paper, we demonstrate, for thefi rst time with this technology, devices with up to 7800
actuated micro-cages that sequester and release solutes, along with valves actuated individually with closing and opening switching
times of 0.6 ± 0.1 and 0.25± 0.15 s, respectively. Two applications of this technology are illustrated in the domain of single cell
handling and the nuclear acid amplification test (NAAT) for the Human Synaptojanin 1 gene, which is suspected to be involved in several neurodegenerative diseases such as Parkinson’s disease. The performance of the temperature-responsive hydrogels we
demonstrate here suggests that in association with their moderate costs, hydrogels may represent an alternative to the actuation orhandling techniques currently used in microfluidics, that are, pressure actuated polydimethylsiloxane (PDMS) valves and droplets

Droplet generation at Hele-Shaw microfluidic T-junction
Laboratoire Microfluidique MEMS et nanostructures - I. Chakraborty, J. Ricouvier, P. Yazghur, P. Tabeling, A. Leshansky
Phys. Fluids - 31(2) 22010 - - 2019
Universal diagram for the kinetics of particle deposition in micro channels
Laboratoire Microfluidique MEMS et nanostructures - C.M. Cejas, F. Monti, M. Truchet, J.-P. Burnouf, P. Tabeling
Phys. Rev. E - 98 62606 - - 2019
Universal diagram for the kinetics of particle deposition in micro channels.
Foam as a self-assembling amorphous photonic band gap material
Laboratoire Microfluidique MEMS et nanostructures - View ORCID ProfileJoshua Ricouvier, Patrick Tabeling, and Pavel Yazhgur
Phys. Fluids - 116 (19) 9202-9207 - doi.org/10.1073/pnas.1820526116 - 2019
We show that slightly polydisperse disordered 2D foams can be used as a self-assembled template for isotropic photonic band gap (PBG) materials for transverse electric (TE) polarization. Calculations based on in-house experimental and simulated foam structures demonstrate that, at sufficient refractive index contrast, a dry foam organization with threefold nodes and long slender Plateau borders is especially advantageous to open a large PBG. A transition from dry to wet foam structure rapidly closes the PBG mainly by formation of bigger fourfold nodes, filling the PBG with defect modes. By tuning the foam area fraction, we find an optimal quantity of dielectric material, which maximizes the PBG in experimental systems. The obtained results have a potential to be extended to 3D foams to produce a next generation of self-assembled disordered PBG materials, enabling fabrication of cheap and scalable photonic devices.
Droplet generation at Hele-Shaw microfluidic T-junction
Laboratoire Microfluidique MEMS et nanostructures - I. Chakraborty, J. Ricouvier, P. Yazhgur, P. Tabeling, and A. M. Leshansky,
Phys. Fluids - 31 2 - doi.org/10.1063/1.5086808 - 2019
We proposed the combined numerical and experimental study of the dynamics of droplets generation at shallow microfluidic T-junction, where the flow is strongly confined in the vertical direction. The numerical simulation is performed by employing quasi-2D Hele-Shaw approximation with an interface capturing procedure based on coupled Level-Set and Volume-of-Fluid methods. We investigate the effect of the capillary number, Ca, the channel geometry (cross section aspect ratio, χ), and the flow rate (disperse-to-continuous phases) ratio, Γ, on the dynamics of the droplet breakup. Depending on Ca, three distinct flow regimes are identified: squeezing, tearing and jetting. In the squeezing regime at low Ca, the size of the generated droplets depends on χ and Γ, while it is almost insensitive to Ca in agreement to previous studies. In the tearing regime at moderate Ca, the droplet size decreases as ∼Ca−1/3, while it is only a weak function of χ and Γ. Finally, in the jetting regime, the steady co-flow of both phases takes place at high enough Ca. The numerical predictions based on the Hele-Shaw flow approximation are in excellent agreement with our in-house experimental results, demonstrating that the proposed approach can be effectively used for computationally inexpensive and adequately accurate modeling of biphasic flows in shallow microfluidic devices.
Pairwise frictional profile between particles determines discontinuous shear thickening transition in non‐colloidal suspensions
Laboratoire Micromégas - J. Comtet, G. Chatté, A. Niguès, L. Bocquet, A. Siria, and A. Colin
Nat Commun - 8 15633 - DOI: 10.1038/ncomms15633 - 2019
The process by which sheared suspensions go through a dramatic change in viscosity is known as discontinuous shear thickening. Although well-characterized on the macroscale, the microscopic mechanisms at play in this transition are still poorly understood. Here, by developing new experimental procedures based on quartz-tuning fork atomic force microscopy, we measure the pairwise frictional profile between approaching pairs of polyvinyl chloride and cornstarch particles in solvent. We report a clear transition from a low-friction regime, where pairs of particles support a finite normal load, while interacting purely hydrodynamically, to a high-friction regime characterized by hard repulsive contact between the particles and sliding friction. Critically, we show that the normal stress needed to enter the frictional regime at nanoscale matches the critical stress at which shear thickening occurs for macroscopic suspensions. Our experiments bridge nano and macroscales and provide long needed demonstration of the role of frictional forces in discontinuous shear thickening.
Nanorheology of Interfacial Water during Ice Gliding
Laboratoire Micromégas - L. Canale, J. Comtet, A. Niguès, C. Cohen, C. Clanet, A. Siria, and L. Bocquet
Phys. Rev. E - - doi.org/10.1103/PhysRevX.9.041025 - 2019
The slipperiness of ice is an everyday-life phenomenon, which, surprisingly, remains controversial despite a long scientific history. The very small friction measured on ice is classically attributed to the presence of a thin self-lubricating film of meltwater between the slider and the ice. But while the macroscale friction behavior of ice and snow has been widely investigated, very little is known about the interfacial water film and its mechanical properties. In this work, we develop a stroke-probe force measurement technique to uncover the microscopic mechanisms underlying ice lubrication. We simultaneously measure the shear friction of a bead on ice and quantify the in situ mechanical properties of the interfacial film, as well as its thickness, under various regimes of speed and temperature. In contrast with standard views, meltwater is found to exhibit a complex viscoelastic rheology, with a viscosity up to 2 orders of magnitude larger than pristine water. The unconventional rheology of meltwater provides a new, consistent, rationale for ice slipperiness. Hydrophobic coatings are furthermore shown to strongly reduce friction due to a surprising change in the local viscosity, providing an unexpected explanation for waxing effects in winter sports. Beyond ice friction, our results suggest new avenues towards self-healing lubricants to achieve ultralow friction.
Entrance Effects in Concentration-Gradient-Driven Flow Through an Ultrathin Porous Membrane
Laboratoire Micromégas - Daniel J. Rankin, Lydéric Bocquet, David M. Huang
J. Chem. Phys - 151 44705 - DOI:10.1063/1.5108700 - 2019
Transport of liquid mixtures through porous membranes is central to processes such as desalination, chemical separations and energy harvesting, with ultrathin membranes made from novel 2D nanomaterials showing exceptional promise. Here we derive, for the first time, general equations for the solution and solute fluxes through a circular pore in an ultrathin planar membrane induced by a solute concentration gradient. We show that the equations accurately capture the fluid fluxes measured in finite-element numerical simulations for weak solute-membrane interactions. We also derive scaling laws for these fluxes as a function of the pore size and the strength and range of solute-membrane interactions. These scaling relationships differ markedly from those for concentration-gradient-driven flow through a long cylindrical pore or for flow induced by a pressure gradient or electric field through a pore in an ultrathin membrane. These results have broad implications for transport of liquid mixtures through membranes with a thickness on the order of the characteristic pore size.
Osmosis, from molecular insights to large-scale applications
Laboratoire Micromégas - Sophie Marbach, Lyderic Bocquet
Phys. Chem. - 48 3102-3144 - DOI:10.1039/C8CS00420J - 2019
Osmosis is a universal phenomenon occurring in a broad variety of processes and fields. It is the archetype of entropic forces, both trivial in its fundamental expression - the van 't Hoff perfect gas law - and highly subtle in its physical roots. While osmosis is intimately linked with transport across membranes, it also manifests itself as an interfacial transport phenomenon: the so-called diffusio-osmosis and -phoresis, whose consequences are presently actively explored for example for the manipulation of colloidal suspensions or the development of active colloidal swimmers. Here we give a global and unifying view of the phenomenon of osmosis and its consequences with a multi-disciplinary perspective. Pushing the fundamental understanding of osmosis allows to propose new perspectives for different fields and we highlight a number of examples along these lines, for example introducing the concepts of osmotic diodes, active separation and far from equilibrium osmosis, raising in turn fundamental questions in the thermodynamics of separation. The applications of osmosis are also obviously considerable and span very diverse fields. Here we discuss a selection of phenomena and applications where osmosis shows great promises: osmotic phenomena in membrane science (with recent developments in separation, desalination, reverse osmosis for water purification thanks in particular to the emergence of new nanomaterials); applications in biology and health (in particular discussing the kidney filtration process); osmosis and energy harvesting (in particular, osmotic power and blue energy as well as capacitive mixing); applications in detergency and cleaning, as well as for oil recovery in porous media.
Atomic rheology of gold nanojunctions
Laboratoire Micromégas - Jean Comtet, Antoine Lainé, Antoine Niguès, Lydéric Bocquet & Alessandro Siria
Nature - 569 393–397 - DOI : 10.1038/s41586-019-1178-3 - 2019
Despite extensive investigations of dissipation and deformation processes in micro- and nano-sized metallic samples1,2,3,4,5,6,7, the mechanisms at play during the deformation of systems with ultimate (molecular) size remain unknown. Although metallic nanojunctions, which are obtained by stretching metallic wires down to the atomic level, are typically used to explore atomic-scale contacts5,8,9,10,11, it has not been possible until now to determine the full equilibrium and non-equilibrium rheological flow properties of matter at such scales. Here, by using an atomic-force microscope equipped with a quartz tuning fork, we combine electrical and rheological measurements on ångström-size gold junctions to study the non-linear rheology of this model atomic system. By subjecting the junction to increasing subnanometric deformations we observe a transition from a purely elastic regime to a plastic one, and eventually to a viscous-like fluidized regime, similar to the rheology of soft yielding materials12,13,14, although orders of magnitude different in length scale. The fluidized state furthermore exhibits capillary attraction, as expected for liquid capillary bridges. This shear fluidization cannot be captured by classical models of friction between atomic planes15,16 and points to an unexpected dissipative behaviour of defect-free metallic junctions at ultimate scales. Atomic rheology is therefore a powerful tool that can be used to probe the structural reorganization of atomic contacts.

410 publications.