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J. De Coninck

Publications and source records attributed to J. De Coninck.

14 recordsLinked to original sources

How heterogeneous wettability enhances boiling

For super-heated water on a substrate with hydrophobic patches immersed in a hydrophilic matrix, one can choose the temperature so that micro-bubbles will form, grow and merge on the hydrophobic patches and not on the hydrophilic matrix. Until covering a patch, making a pinned macro-bubble, a bubble has a contact angle $π-θ_2$, where $θ_2$ is the receding contact angle of water on the patch material. This pinned macro-bubble serves as the initial condition of a quasi-static growth process, à la Landau, leading to detachment through the formation of a neck, so long as depinning and dewetting of the hydrophilic matrix was avoided during the growth of the pinned bubble: the bubble contact angle should not exceed $π-θ_1$, where $θ_1$ is the receding contact angle of water on the matrix material. The boiling process may then enter a cycle of macro-bubbles forming and detaching on the patches; the radii of these patches can be optimized for maximizing the heat transfer for a given substrate area. For this analysis to become quantitative, we revisit the Young-Laplace quasi-static evolution of key physical quantities, such as bubble energy, as functions of bubble growing volume, when gravity is either significative or negligible: this concerns both pinned bubbles on a fixed circular footprint (Dirichlet boundary conditions) and free un-pinned bubbles with a fixed contact angle (Neumann boundary conditions).

physics.flu-dyn

Optimizing fog harvesting by biomimicry

Inspired by the stenocara beetle, we study an ideal flat surface composed of a regular array of hydrophilic circular patches in a hydrophobic matrix on an incline of tilt $α$ with respect to the horizontal. Based on an exact solution of the Laplace-Young equation at first order in the Bond number, the liquid storage capacity of the surface is maximized as function of the patch radius, for suitable ranges of hydrophilic and hydrophobic contact angles, for tilt angles such as $45^{\circ}$ or $90^\circ$. It is found that the optimal radius equally prevents dewetting from the top of the patches and overflow at the bottom. These theoretical considerations are validated by several experiments for the glass/octadecyltrichlorosilane (OTS) system involving different patch sizes and different inclinations. In a simple dynamical model, taking into account the flux of fog onto the surface or condensation on a suitably cooled surface, we find that the conditions for maximum harvest agree with the ones of maximum static storage. The method could be developed for drop storage and drop transport applications such as water-harvesting systems.

cond-mat.soft

Composite states of wetting

The analytical expressions of liquid-vapor macroscopic contact angles are analyzed for various simple geometries and arrangements of the substrate, in particular when the latter exhibits two or more scales. It concerns the Wenzel state of wetting when the substrate is completely wet, the Cassie-Baxter state when the liquid hangs over the substrate, but also intermediate states of wetting which are shown to be relevant and in competition with the two other ones. Under a separation of scales hypothesis, a composition rule of contact angles is developed whose interest is illustrated in a close packing setup of rasperry-like particles.

cond-mat.soft

Shape of pendant droplets under a tilted surface

For a pendant drop whose contact line is a circle of radius $r_0$, we derive the relation $mg\sinα={π\over2}γr_0\,(\cosθ^{\rm min}-\cosθ^{\rm max})$ at first order in the Bond number, where $θ^{\rm min}$ and $θ^{\rm max}$ are the contact angles at the back (uphill) and at the front (downhill), $m$ is the mass of the drop and $γ$ the surface tension of the liquid. The Bond (or Eötvös) number is taken as $Bo=mg/(2r_0γ)$. The tilt angle $α$ may increase from $α=0$ (sessile drop) to $α=π/2$ (drop pinned on vertical wall) to $α=π$ (drop pendant from ceiling). The focus will be on pendant drops with $α=π/2$ and $α=3π/4$. The drop profile is computed exactly, in the same approximation. Results are compared with surface evolver simulations, showing good agreement up to about $Bo=1.2$, corresponding for example to hemispherical water droplets of volume up to about $50\,μ$L. An explicit formula for each contact angle $θ^{\rm min}$ and $θ^{\rm max}$ is also given and compared with the almost exact surface evolver values.

physics.flu-dyn

Intrinsic Friction of Monolayers Adsorbed on Solid Surfaces

We overview recent results on intrinsic frictional properties of adsorbed monolayers, composed of mobile hard-core particles undergoing continuous exchanges with a vapor phase. In terms of a dynamical master equation approach we determine the velocity of a biased impure molecule - the tracer particle (TP), constrained to move inside the adsorbed monolayer probing its frictional properties, define the frictional forces exerted by the monolayer on the TP, as well as the particles density distribution in the monolayer.

cond-mat.stat-mech

Intrinsic friction of adsorbed monolayers

In the present paper we overview our recent results on intrinsic frictional properties of adsorbed monolayers, composed of mobile hard-core particles undergoing continuous exchanges with a vapor phase. Within the framework of a dynamical master equation approach, describing the time evolution of the system, we determine in the most general form the terminal velocity of some biased impure molecule - the tracer particle (TP), constrained to move inside the adsorbed monolayer probing its frictional properties, define the frictional forces as well as the particles density distribution in the monolayer. Results for one-dimensional solid substrates, appropriate to adsorbtion on polymer chains, are compared against the Monte Carlo simulation data, which confirms our analytical predictions.

cond-mat.soft

Force-velocity relation and density profiles for biased diffusion in an adsorbed monolayer

In this paper, which completes our earlier short publication [Phys. Rev. Lett. 84, 511 (2000)], we study dynamics of a hard-core tracer particle (TP) performing a biased random walk in an adsorbed monolayer, composed of mobile hard-core particles undergoing continuous exchanges with a vapor phase. In terms of an approximate approach, based on the decoupling of the third-order correlation functions, we obtain the density profiles of the monolayer particles around the TP and derive the force-velocity relation, determining the TP terminal velocity, V_{tr}, as the function of the magnitude of external bias and other system's parameters. Asymptotic forms of the monolayer particles density profiles at large separations from the TP, and behavior of V_{tr} in the limit of small external bias are found explicitly.

cond-mat.soft

Stokes formula and density perturbances for driven tracer diffusion in an adsorbed monolayer

We study the intrinsic friction of monolayers adsorbed on solid surfaces from a gas phase or vapor. Within the framework of the Langmuir model of delocalized adsorption, we calculate the resistance offered by the mobile adsorbate's particles to some impure tracer molecule, whose diffusive random motion is biased by a constant external force. We find that for sufficiently small driving forces the force exerted on the tracer shows viscous-like behavior. We derive then the analog of the Stokes formula for two-dimensional adsorbates, calculate the corresponding friction coefficient and determine the stationary particle distribution in the monolayer as seen from the driven impurity.

cond-mat.stat-mech

Phase boundary dynamics in a one-dimensional non-equilibrium lattice gas

We study dynamics of a phase boundary in a one-dimensional lattice gas, which is initially put into a non-equilibrium configuration and then is let to evolve in time by particles performing nearest-neighbor random walks constrained by hard-core interactions. Initial non-equilibrium configuration is characterized by an $S$-shape density profile, such that particles density from one side of the origin (sites $X \leq 0$) is larger (high density phase, HDP) than that from the other side (low-density phase, LDP). We suppose that all the lattice gas particles, except for the rightmost particle of the HDP, have symmetric hopping probabilities. The rightmost particle of the HDP, which determines the position of the phase separating boundary, is subject to a constant force $F$, oriented towards the HDP; in our model this force mimics an effective tension of the phase separating boundary. We find that, in the general case, the mean displacement $\bar{X(t)}$ of the phase boundary grows with time as $\bar{X(t)} = α(F) t^{1/2}$, where the prefactor $α(F)$ depends on $F$ and on the initial densities in the HDP and LDP. We show that $α(F)$ can be positive or negative, which means that depending on the physical conditions the HDP may expand or get compressed. In the particular case when $α(F) = 0$, i.e. when the HDP and LDP coexist with each other, the second moment of the phase boundary displacement is shown to grow with time sublinearly, $\bar{X^2(t)} = γt^{1/2}$, where the prefactor $γ$ is also calculated explicitly. Our analytical predictions are shown to be in a very good agreement with the results of Monte Carlo simulations.

cond-mat.stat-mech

Droplet Spreading: Partial Wetting Regime Revisited

We study the time evolution of a sessile liquid droplet, which is initially put onto a solid surface in a non-equilibrium configuration and then evolves towards its equilibrium shape. We adapt here the standard approach to the dynamics of mechanical dissipative systems, in which the driving force, i.e. the gradient of the system's Lagrangian function, is balanced against the rate of the dissipation function. In our case the driving force is the loss of the droplet's free energy due to the increase of its base radius, while the dissipation occurs due to viscous flows in the core of the droplet and due to frictional processes in the vicinity of the advancing contact line, associated with attachment of fluid particles to solid. Within this approach we derive closed-form equations for the evolution of the droplet's base radius, and specify several regimes at which different dissipation channels dominate. Our analytical predictions compare very well with experimental data.

cond-mat.mtrl-sci

Dewetting, partial wetting and spreading of a two-dimensional monolayer on solid surface

We study the behavior of a semi-infinite monolayer, which is placed initially on a half of an infinite in both directions, ideal crystalline surface, and then evolves in time due to random motion of the monolayer particles. Particles dynamics is modeled as the Kawasaki particle-vacancy exchange process in the presence of long-range attractive particle-particle interactions. In terms of an analytically solvable mean-field-type approximation we calculate the mean displacement X(t) of the monolayer edge and discuss the conditions under which such a monolayer spreads (X(t) > 0), partially wets (X(t) = 0) or dewets from the solid surface (X(t) < 0).

cond-mat.soft

Microscopic model for spreading of a two-dimensional monolayer

We study the behavior of a monolayer, which occupies initially a bounded region on an ideal crystalline surface and then evolves in time due to random hopping motion of the monolayer particles. In the case when the initially occupied region is the half-plane $X \leq 0$, we determine explicitly, in terms of an analytically solvable mean-field-type approximation, the mean displacement $X(t)$ of the monolayer edge. We find that $X(t) \approx A \sqrt{D_{0} t}$, in which law $D_{0}$ denotes the bare diffusion coefficient and the prefactor $A$ is a function of the temperature and of the particle-particle interactions parameters. We show that $A$ can be greater, equal or less than zero, and specify the critical parameter which distinguishes between the regimes of spreading ($A > 0)$, partial wetting ($A = 0$) and dewetting ($A < 0$).

cond-mat.soft

Dynamics of a driven probe molecule in a liquid monolayer

We study dynamics of a probe molecule, driven by an external constant force in a liquid monolayer on top of solid surface. In terms of a microscopic, mean-field-type approach, we calculate the terminal velocity of the probe molecule. This allows us to establish the analog of the Stokes formula, in which the friction coefficient is interpreted in terms of the microscopic parameters characterizing the system. We also determine the distribution of the monolayer particles as seen from the stationary moving probe molecule and estimate the self-diffusion coefficient for diffusion in a liquid monolayer.

cond-mat.soft

Direct Energy Transfer in Systems of Polymerized Acceptors

We study the direct incoherent energy transfer from an immobile excited donor molecule to acceptor molecules, which are all attached to polymer chains, randomly arranged in a viscous solvent. The decay forms are found explicitly, in terms of an optimal-fluctuation method, for arbitrary conformations of polymers.

cond-mat