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J. Heu and M. Durand, “Order-disorder transition in thermal soft cellular systems”, to be submitted (2018).
We numerically explored the order-disorder transition of monodisperse, two-dimensional cellular systems under thermal agitation. We highlight the existence of a hexatic intermediate phase in which positional order vanishes but orientational order is preserved. However, the two-dimensional melting scenario seems to follow a dislocation condensation scenario rather than the Kosterlitz-Thouless-Halperin-Nelson-Young theory. Each phase (liquid-hexatic-solid) has been highlighted with the use of both static and dynamic order parameters. |
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E. Babilio, F. Fabbrocino, M. Durand and F. Fraternalli, “On the design of 2D stiffest elastic networks with tetrakis-like architecture”, Extreme Mechanics Letters 15, 57-62 (2017).
We derive general conditions for the design of two-dimensional stiffest elastic networks with tetrakis-like (or "Union Jack"-like) topology. Upon generalizing recent results for tetrakis structures composed of two different rod geometries (length and cross-sectional area), we derive the elasticity tensor of a lattice with generalized tetrakis architecture, which is composed of three kinds of rods and generally exhibits anisotropic response. This study is accompanied by an experimental verification of the theoretical prediction for the longitudinal modulus of the lattice. In addition, the introduction of a third rod geometry allows to extend considerably the possible lattice geometries for isotropic, stiffest elastic lattices with tetrakis-like topology. The potential of the analyzed structures as innovative metamaterials featuring extremely high elastic moduli vs. density ratios is highlighted. |
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M. Durand and E. Guesnet, “An efficient Cellular Potts Model algorithm that forbids cell fragmentation”, Computer Physics Communications 208, 54-63 (2016).
The Cellular Potts Model (CPM) is a lattice based modeling technique which is widely used for simulating cellular patterns such as foams or biological tissues. Despite its realism and generality, the standard Monte Carlo algorithm used in the scientific literature to evolve this model works on a limited range of simulation temperature in order to preserve the connectivity of the cells. We present a new algorithm in which cell fragmentation is forbidden for all simulation temperatures. This allows to significantly enhance realism of the simulated patterns. It also increases the computational efficiency compared with the standard CPM algorithm even at same simulation temperature, thanks to the time spared in not doing unrealistic moves. Moreover, this algorithm restores the detailed balance equation, ensuring that the long-term stage is independent of the chosen acceptance rate and chosen path in the temperature space. |
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A. Callan-Jones, M. Durand, and J.-B. Fournier, “Hydrodynamics of bilayer membranes with diffusing transmembrane proteins”, Soft Matter 12, 1791-1800 (2016).
We consider the hydrodynamics of lipid bilayers containing transmembrane proteins of arbitrary shape. This biologically-motivated problem is relevant to the cell membrane, whose fluctuating dynamics play a key role in phenomena ranging from cell migration, intercellular transport, and cell communication. Using Onsager's variational principle, we derive the equations that govern the relaxation dynamics of the membrane shape, of the mass densities of the bilayer leaflets, and of the diffusing proteins' concentration. With our generic formalism, we obtain several results on membrane dynamics. We find that proteins that span the bilayer increase the intermonolayer friction coefficient. The renormalization, which can be significant, is in inverse proportion to the protein's mobility. Second, we find that asymmetric proteins couple to the membrane curvature and to the difference in monolayer densities. For practically all accessible membrane tensions ($\sigma> 10^{-8}$ N/m) we show that the protein density is the slowest relaxing variable. Furthermore, its relaxation rate decreases at small wavelengths due to the coupling to curvature. We apply our formalism to the large-scale diffusion of a concentrated protein patch. We find that the diffusion profile is not self-similar, owing to the wavevector dependence of the effective diffusion coefficient. |
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M. Durand, “Statistical mechanics of two-dimensional shuffled foams: physical foundations of the model”, European Physical Journal E 38, 137 (2015).
In a recent series of papers, a statistical model that accounts for correlations between topological and geometrical properties of a two-dimensional shuffled foam has been proposed and compared with experimental and numerical data. Here, the various assumptions on which the model is based are exposed and justified: the equiprobability hypothesis of the foam configurations is argued. The range of correlations between bubbles is discussed, and the mean field approximation that is used in the model is detailed. The two self-consistency equations associated with this mean field description can be interpreted as the conservation laws of number of sides and bubble curvature, respectively. Finally, the use of a "Grand-Canonical" description, in which the foam constitutes a reservoir of sides and curvature, is justified. |
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S. Gauchet, M. Durand, and D. Langevin, “Foam drainage: possible influence of a non-newtonian surface shear viscosity”, Journal of Colloid and Interface Science 449, 373-376 (2015).
We describe forced drainage experiments of foams made with model surfactant solutions with different surface rheology. We analyze the origin of two distinct drainage transitions reported in the literature, between regimes where the bubble surfaces are mobile or rigid. We propose that both transitions are related to the surface shear viscosity and to its shear thinning behavior. Shear thinning could also account for the huge discrepancies between measurements reported in the literature. The role of surface tension gradients, i.e. Marangoni effect, could not possibly explain the behavior observed with the different solutions. |
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M. Durand, A. M. Kraynik, F. van Swol, J. Käfer, C. Quilliet, S. Cox, S. Ataei Talebi, and F. Graner, “Statistical mechanics of two-dimensional shuffled foams: Geometry-topology correlation in small or large disorder limits”, Physical Review E 89, 062309 (2014).
Bubble monolayers are model systems for experiments and simulations of two-dimensional packing problems of deformable objects. We explore the relation between the distributions of the number of bubble sides (topology) and the bubble areas (geometry) in the low liquid fraction limit. We use a statistical model [M. Durand, Europhys. Lett. 90, 60002 (2010)] which takes into account Plateau laws. We predict the correlation between geometrical disorder (bubble size dispersity) and topological disorder (width of bubble side number distribution) over an extended range of bubble size dispersities. Extensive data sets arising from shuffled foam experiments, SURFACE EVOLVER simulations, and cellular Potts model simulations all collapse surprisingly well and coincide with the model predictions, even at extremely high size dispersity. At moderate size dispersity, we recover our earlier approximate predictions [M. Durand, J. Kafer, C. Quilliet, S. Cox, S. A. Talebi, and F. Graner, Phys. Rev. Lett. 107, 168304 (2011)]. At extremely low dispersity, when approaching the perfectly regular honeycomb pattern, we study how both geometrical and topological disorders vanish. We identify a crystallization mechanism and explore it quantitatively in the case of bidisperse foams. Due to the deformability of the bubbles, foams can crystallize over a larger range of size dispersities than hard disks. The model predicts that the crystallization transition occurs when the ratio of largest to smallest bubble radii is 1.4. |
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G. Gurtner and M. Durand, “Stiffest elastic networks”, Proceedings of the Royal Society A 470, 20130611 (2014).
The rigidity of a network of elastic beams is closely related to its microstructure. We show both numerically and theoretically that there is a class of isotropic networks, which are stiffer than any other isotropic network of same density. The elastic moduli of these stiffest elastic networks are explicitly given.They constitute upper-bounds, which compete or improve the well-known Hashin–Shtrikman bounds. We provide a convenient set of criteria (necessary and sufficient conditions) to identify these networks and show that their displacement field under uniform loading conditions is affine down to the microscopic scale. Finally, examples of such networks with periodic arrangement are presented, in both two and three dimensions. In particular, we present an optimal and isotropic three-dimensional structure which, to our knowledge, is the first one to be presented as such. |
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M. Durand, J. Käfer, C. Quilliet, S. J. Cox, S. Ataei Talebi, and F. Graner, “Statistical mechanics of two-dimensional shuffled foams: Prediction of the correlation between geometry and topology”, Physical Review Letters, 107, 168304 (2011).
We propose an analytical model for the statistical mechanics of shuffled two-dimensional foams with moderate bubble size polydispersity. It predicts without any adjustable parameters the correlations between the number of sides $n$ of the bubbles (topology) and their areas $A$ (geometry) observed in experiments and numerical simulations of shuffled foams. Detailed statistics show that in shuffled cellular patterns $n$ correlates better with $A$ (as claimed by Desch and Feltham) than with $A$ (as claimed by Lewis and widely assumed in the literature). At the level of the whole foam, standard deviations $\Delta n$ and $\Delta A$ are in proportion. Possible applications include correlations of the detailed distributions of $n$ and $A$, three-dimensional foams, and biological tissues. |
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M. Durand, "Statistical Mechanics of Two-dimensional Foams", EPL 90, 60002 (2010).
abstract: The methods of statistical mechanics are applied to two-dimensional foams under macroscopic agitation. A new variable —the total cell curvature— is introduced, which plays the role of energy in conventional statistical thermodynamics. The probability distribution of the number of sides for a cell of given area is derived. This expression allows to correlate the distribution of sides (“topological disorder”) to the distribution of sizes (“geometrical disorder”) in a foam. The model predictions agree well with available experimental data. |
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G. Gurtner and M. Durand, "Structural Properties of Stiff Elastic Networks", EPL 87, 24001 (2009).
abstract: Networks of elastic beams can deform either by stretching or bending of their members. The primary mode of deformation (bending or stretching) crucially depends on the specific details of the network architecture. In order to shed light on the relationship between microscopic geometry and macroscopic mechanics, we characterize the structural features of networks which deform uniformly, through the stretching of the beams only. We provide a convenient set of geometrical criteria to identify such networks, and derive the values of their effective elastic moduli. The analysis of these criteria elucidates the variability of mechanical response of elastic networks. In particular, our study rationalizes the difference in mechanical behavior of cellular and fiber networks. |
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M. Durand, "Low-density cellular materials with optimal conductivity and bulk modulus", Congrès Français de Mécanique. i-revues http://hdl.handle.net/2042/15750 (2007).
abstract: Optimal upper bounds on the average conductivity and the bulk modulus of low density cellular materials are established. These bounds are tighter than the classical Hashin-Shtrikman upper bounds, and can be applied to anisotropic materials. Furthermore, necessary and sufficient conditions on the microgeometry of the cellular materials to maximize (for a given solid volume fraction) either the average conductivity or the bulk modulus are derived. The conditions are found to be identical for both quantities, so that the bounds are attained simultaneously: a low-density cellular material with maximal average conductivity will have maximal bulk modulus as well. |
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M. Durand, "Structure of optimal pipe networks subject to a global constraint", Phys. Rev. Lett. 98, 088701 (2007).
abstract: The structure of pipe networks minimizing the total energy dissipation rate is studied analytically. Among all the possible pipe networks that can be built with a given total pipe volume (or pipe lateral surface area), the network which minimizes the dissipation rate is shown to be loopless. Furthermore, such an optimal network is shown to contain at most $N-2$ nodes in addition to the $N$ sources plus sinks that it connects. These results are valid whether the possible locations for the additional nodes are chosen freely or from a set of nodes (such as points of a grid). Applications of these results to various physical situations and to the efficient computation of optimal pipe networks are also discussed. |
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M. Durand and H. A. Stone, "Relaxation time of the topological T1 process in a two-dimensional foam", Phys. Rev. Lett. 97, 226101 (2006).
abstract: The elementary topological T1 process in a two-dimensional foam corresponds to the flip of one film with respect to the geometrical constraints, and is a process by which the structure of an out-of-equilibrium foam evolves. We study both experimentally and theoretically the T1 dynamics in a dry two-dimensional foam. The dynamics is controlled by the surface viscoelastic properties of the films (surface shear plus dilatational viscosity, μs+κ, and Gibbs elasticity ϵ), and is independent of the shear viscosity of the bulk liquid. Moreover, the dynamics of the T1 process provides a tool for measuring the surface rheological properties: we obtained ϵ=32±8mN/m and μs+κ=1.3±0.7mPa·m·s for sodium dodecyl sulfate, and ϵ=65±12mN/m and μs+κ=31±12mPa·m·s for bovine serum albumin, in good agreement with literature values. |
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M. Durand, "Architecture of optimal transport networks", Phys. Rev. E 73, 016116 (2006).
abstract: We analyze the structure of networks minimizing the global resistance to flow (or dissipative energy) with respect to two different constraints: fixed total channel volume and fixed total channel surface area. First, we show that channels must be straight and have uniform cross-sectional areas in such optimal networks. We then establish a relation between the cross-sectional areas of adjoining channels at each junction. Indeed, this relation is a generalization of Murray's law, originally established in the context of local optimization. We establish a relation too between angles and cross-sectional areas of adjoining channels at each junction, which can be represented as a vectorial force balance equation, where the force weight depends on the channel cross-sectional area. A scaling law between the minimal resistance value and the total volume or surface area value is also derived from the analysis. Furthermore, we show that no more than three or four channels meet at each junction of optimal bidimensional networks, depending on the flow profile (e.g., Poiseuille-like or pluglike) and the considered constraint (fixed volume or surface area). In particular, we show that sources are directly connected to wells, without intermediate junctions, for minimal resistance networks preserving the total channel volume in case of plug flow regime. Finally, all these results are compared with the structure of natural networks. |
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M. Durand, "Optimizing the bulk modulus of low-density cellular networks", Phys. Rev. E. 72, 011114 (2005).
abstract: We present an alternative derivation of upper-bounds for the bulk modulus of both two-dimensional and three-dimensional cellular materials. For two-dimensional materials, we recover exactly the expression of the Hashin-Shtrikman (HS) upper-bound in the low-density limit, while for three-dimensional materials we even improve the HS bound. Furthermore, we establish necessary and sufficient conditions on the cellular structure for maximizing the bulk modulus, for a given solid volume fraction. The conditions are found to be exactly those under which the electrical (or thermal) conductivity of the material reaches its maximal value as well. These results provide a set of straightforward criteria allowing us to address the design of optimized cellular materials, and shed light on recent studies of structures with both maximal bulk modulus and maximal conductivity. Finally, we discuss the specific case of spring networks, and analyze the compatibility of the criteria presented here with the geometrical constraints caused by minimization of surface energy in a real foam. |
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M. Durand and D. Weaire, "Optimizing transport in a homogeneous network", Phys. Rev. E 70, 046125 (2004).
abstract: Many situations in physics, biology, and engineering consist of the transport of some physical quantity through a network of narrow channels. The ability of a network to transport such a quantity in every direction can be described by the average conductivity associated with it. When the flow through each channel is conserved and derives from a potential function, we show that there exists an upper bound of the average conductivity and explicitly give the expression for this upper bound as a function of the channel permeability and channel length distributions. Moreover, we express the necessary and sufficient conditions on the network structure to maximize the average conductivity. These conditions are found to be independent of the connectivity of the vertices. |
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M.Durand, J.-F. Sadoc, and D. Weaire, "Maximum electrical conductivity of a network of uniform wires : the Lemlich law as an upper bound", Proc. R. Soc. Lond. A 460, 1269-1285 (2004).
abstract: The Lemlich law provides a simple estimate of the relative conductivity of a three-dimensional foam, as one third of its liquid fraction. This is based on an expression for the conductivity of a network of uniform wires (conducting lines). We show this to be an exact upper bound for the conductivity, orientationally averaged in the case of anisotropic systems. We discuss the dependance of conductivity on the geometry of the network structure and establish two necessary and sufficient conditions to maximize the conductivity. We note the connection between this problem and that of line-length minimization and also that between anisotropic conductivity and stress for a two-dimensional foam. These results are illustrated by various numerical simulations of network conductivities. The theorems presented in this paper may also be applied to the thermal conductivity and the permeability of a network. |
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H.A. Stone, S.A. Koehler, S. Hilgenfeldt, and M. Durand, "Perspectives on foam drainage and the influence of interfacial rheology", J. Phys. : Condens. Matter, 15, S283-S290 (2003).
abstract: Recent research related to foam drainage is surveyed with emphasis on the influence of interfacial rheology. Active research directions are highlighted and the possible impact of these studies on macroscopic rheology is indicated. |
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M. Durand, "Contibutions théorique et expérimentale à l'étude du drainage d'une mousse aqueuse", Thèse (2002).
abstract: In this thesis manuscript, we report theoretical and experimental results on drainage of aqueous foams. Two experimental setups were built to study foam drainage, the first one based on conductivity measurements and the second one based on multiple light scattering. These two devices enabled us to highlight the effect of the physical chemistry on the drainage of foam, and thus to reconcile in a qualitative way the two existing models of foam drainage. This effect of physical chemistry corresponds to the important role played by the surface viscoelasticity parameters of the channels on the drainage. Moreover, the experimental results show that the bubble size also has an influence on the drainage regime. This result can be understood in terms of competition between the dissipation at the surface and the dissipation in the bulk. Measurements of the dynamical surface tension were also made with the pendant drop technique. We proved this way that the surface of the channels remains locally in thermodynamic equilibrium with the bulk. On the theoretical level, a new model for the drainage explicitly including the surface viscoelastic parameters and the bubble size is proposed. The dependence of the drainage with these parameters is qualitatively in agreement with the experimental results. Finally, the effect of the disorder has been studied by calculating the effective conductivity of periodic foams. The conclusion of this study is that the laws governing the local structure of a foam (Plateau's laws) naturally imply a uniform distribution and orientation of the channels in the foam. |
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D. Langevin, A. St-Jalmes, M. Durand, and M. Safouane, "Les Mousses" , bulletin de la SFP, 134, 11-16 (2002).
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M.Durand and D. Langevin, "Physicochemical approach to the theory of foam drainage" , Eur. Phys. J. E , 7, 35-44 (2002).
abstract: We have investigated theoretically the effect of surface viscoelasticity on the drainage of an aqueous foam. Former theories consider that the flow in Plateau borders is either Poiseuille flow or plug-flow. In the last case, the dissipation is attributed to flow in the nodes connecting Plateau borders. Although we do not include this dissipation in our model, we obtain a drainage equation that includes terms equivalent to those of the earlier models. We show that when the water solubility of the surfactant stabilizing the foam is low, the control parameter M for the transition between the two regimes is the ratio , where μ is the bulk viscosity, Ds the surface diffusion coefficient, R the radius of curvature of the Plateau border and ɛ the surface elasticity. When the surfactant is more soluble M is rather related to the bulk diffusion coefficient. Within the frame of this approach and in view of the estimated M values, we show that the flow in Plateau borders is Poiseuille-like. |
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M. Safouane, M. Durand, A. St-Jalmes, D. Langevin, and V. Bergeron, "Aqueous foam drainage. Role of the rheology of the foaming fluid", J. Phys. IV, 11, Pr6-275 – Pr6-280 (2001).
abstract: We have studied the drainage of foams made with viscous solutions. In this way, drainage is slowed down, and microgravity conditions are approached. The behaviour of mixtures of water and glycerol follows the theoretical predictions, but that of aqueous solutions of a polymer (polyethylene oxide) do not: drainage is much faster than for water-glycerol mixtures of the same bulk viscosity. The origin of this puzzling behavior is still not understood. |
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N. Rivier and M. Durand,"Variable-range hopping conductivity in quasicrystals", Mat. Sci. Eng. A 294-296, 584-587 (2000).
abstract: The electronic density of states (DOS) of 1D quasicrystals looks like that of a highly doped, p-type semiconductor: the Fermi level lies in the “impurity band”, which consists of localized states. At low temperatures, the conductivity of an electronic structure of this type is by variable-range hopping, as observed recently in i-Al–Pd–Re. |
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M. Durand,G. Martinoty G., and D. Langevin, "Liquid flow through aqueous foams: from the Plateau border-dominated regime to the node-dominated regime" , Phys. Rev. E, 60, R6307 (1999).
abstract: The velocity of gravity-driven flow through aqueous foams forced drainage has been determined by using electrical conductivity measurements in foams made with solutions of different surfactants. There is always a scaling behavior power law between the drainage velocity $V$ and the imposed flow rate $Q$: $V \sim Q^\alpha$, but the $\alpha$ coefficient varies between the different surfactant solutions and increases with surface viscosity. An explanation of this behavior will be given in terms of a transition between a node-dominated and a Plateau border-dominated viscous dissipation, for which theory predicts respectively $\alpha=1/3$ and $\alpha=1/2$. |
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