25 research outputs found
Phase coexistence in the hard-sphere Yukawa chain fluid with chain length polydispersity: High temperature approximation
High temperature approximation (HTA) is used to describe the phase behavior
of polydisperse multi-Yukawa hard-sphere chain fluid mixtures with chain length
polydispersity. It is demonstrated that in the frames of the HTA the model
belongs to the class of ``truncatable free energy models'', i.e. the models
with thermodynamical properties (Helmholtz free energy, chemical potential and
pressure) defined by the finite number of generalized moments. Using this
property we were able to calculate the complete phase diagram (i.e., cloud and
shadow curves as well as binodals) and chain length distribution functions of
the coexisting phases.Comment: 18 pages, 13 figure
Phase coexistance in polydisperse mixture of hard-sphere colloidal and flexible chain particles
A theoretical scheme for the calculation of the full phase diagram (including
cloud and shadow curves, binodals and distribution functions of the coexisting
phases) for colloid-polymer mixtures with polymer chain length polydispersity
and hard-sphere colloidal and polymeric monomer sizes polydispersity is
proposed. The scheme combines thermodynamic perturbation theory for associating
fluids and recently developed method used to determine the phase diagram of
polydisperse spherical shape colloidal fluids (L.Bellier-Castella {\it et al.},
{\it J.Chem.Phys.} {\bf 113}, 8337(2000)). By way of illustration we present
and discuss the full phase diagram for the mixture with polydispersity in the
size of the hard-sphere colloidal particles.Comment: 6 pages, 4 figure
Colloidal brazil nut effect in sediments of binary charged suspensions
Equilibrium sedimentation density profiles of charged binary colloidal
suspensions are calculated by computer simulations and density functional
theory. For deionized samples, we predict a colloidal ``brazil nut'' effect:
heavy colloidal particles sediment on top of the lighter ones provided that
their mass per charge is smaller than that of the lighter ones. This effect is
verifiable in settling experiments.Comment: 4 pages, 4 figure
Aging and memory properties of topologically frustrated magnets
The model 2d kagome system (H3O)Fe3(SO4)2(OH)6 and the 3d pyrochlore Y2Mo2O7
are two well characterized examples of low-disordered frustrated
antiferromagnets which rather then condensing into spin liquid have been found
to undergo a freezing transition with spin glass-like properties. We explore
more deeply the comparison of their properties with those of spin glasses, by
the study of characteristic rejuvenation and memory effects in the
non-stationary susceptibility. While the pyrochlore shows clear evidence for
these non-trivial effects, implying temperature selective aging, that is
characteristic of a wide hierarchical distribution of equilibration processes,
the kagome system does n not show clearly these effects. Rather, it seems to
evolve towards the same final state independently of temperature.Comment: submitted for the proceedings of the 46th MMM conference (Seattle,
2001
Polydisperse hard spheres at a hard wall
The structural properties of polydisperse hard spheres in the presence of a
hard wall are investigated via Monte Carlo simulation and density functional
theory (DFT). Attention is focussed on the local density distribution
, measuring the number density of particles of diameter
at a distance from the wall. The form of is
obtained for bulk volume fractions and for two
choices of the bulk parent distribution: a top-hat form, which we study for
degrees of polydispersity and , and a truncated
Schulz form having . Excellent overall agreement is found between
the DFT and simulation results, particularly at . A detailed
analysis of confirms the presence of oscillatory size
segregation effects observed in a previous DFT study (Pagonabarraga {\em et
al.}, Phys. Rev. Lett. {\bf 84}, 911 (2000)). For large , the character
of these oscillation is observed to depend strongly on the shape of the parent
distribution. In the vicinity of the wall, attractive -dependent
depletion interactions are found to greatly enhance the density of the largest
particles. The local degree of polydispersity is suppressed in this
region, while further from the wall it exhibits oscillations.Comment: 12 pages revte
The relative influences of disorder and of frustration on the glassy dynamics in magnetic systems
The magnetisation relaxations of three different types of geometrically
frustrated magnetic systems have been studied with the same experimental
procedures as previously used in spin glasses. The materials investigated are
YMoO (pyrochlore system), SrCrGaO (piled
pairs of Kagom\'e layers) and (HO)Fe(SO)(OH) (jarosite
compound). Despite a very small amount of disorder, all the samples exhibit
many characteristic features of spin glass dynamics below a freezing
temperature , much smaller than their Curie-Weiss temperature .
The ageing properties of their thermoremanent magnetization can be well
accounted for by the same scaling law as in spin glasses, and the values of the
scaling exponents are very close. The effects of temperature variations during
ageing have been specifically investigated. In the pyrochlore and the
bi-Kagom\'e compounds, a decrease of temperature after some waiting period at a
certain temperature re-initializes ageing and the evolution at the new
temperature is the same as if the system were just quenched from above .
However, as the temperature is raised back to , the sample recovers the
state it had previously reached at that temperature. These features are known
in spin glasses as rejuvenation and memory effects. They are clear signatures
of the spin glass dynamics. In the Kagom\'e compound, there is also some
rejuvenation and memory, but much larger temperature changes are needed to
observe the effects. In that sense, the behaviour of this compound is
quantitatively different from that of spin glasses.Comment: latex VersionCorrigee4.tex, 4 files, 3 figures, 5 pages (Proceedings
of the International Conference on Highly Frustrated Magnetism (HFM2003),
August 26-30, 2003, Institut Laue Langevin (ILL), Grenoble, France
Équilibre de phases dans les systèmes de colloïdes polydisperses et de molécules discotiques
Nous présentons une étude sur les équilibres de phases de fluides complexes tels que les colloïdes polydisperses et les molécules discotiques. L'étude théorique sur les colloïdes polydisperses a trait à l'influence de la polydispersité sur les comportements de phases fluides, dans le cadre d'une approximation de fluides de Van der Waals et grâce à la théorie de la fonctionnelle de densité. Elle met en évidence l'existence de caractéristiques originales comme la présence de plusieurs points critiques, la possibilité d'avoir des coexistences à plus de deux phases ainsi que d'autres modifications importantes du diagramme de phases. Nous nous intéressons également aux interfaces entre deux phases fluides polydisperses et plus particulièrement à l'influence de la polydispersité sur la tension de surface et les propriétés d'adsorption. Enfin, nous abordons un autre exemple de luides polydisperses inhomogènes : celui de fluides soumis au champ de pesanteur. Cette étude de la sédimentaiton met en évidence des phénomènes de ségrégation provenant d'une compétition entre les effets de volume exclu, ceux dus à l'attraction et l'influence du champ de psesanteur. D'autre part, une étude par simulations Monte-Carlo de molécules discotiques permet de s'intéresser non plus à l'influence de la polydispersité mais à celle du carctère anisotrope des molécules, à l'originie des phase nématiques et colonnaires. Plus précisément, nous étdions l'nluence du confinement sur la structuration en colonnes et le déplacement à plus haute ou plus basse température de la transition nématique-colonnaire en fonction du type de parois considéréLYON1-BU.Sciences (692662101) / SudocSudocFranceF
Phase diagrams of polydisperse van der Waals fluids
The phase diagrams for fluids composed of spherical particles with a monomodal size distribution is presented. These phase diagrams are obtained on the basis of the van der Waals approximation for the free-energy of a polydisperse fluid. It is found that the largest modifications to the phase diagram of the polydisperse fluid, as compared to its monodisperse counterpart, result from the amplitude polydispersity of the interaction potential.SCOPUS: ar.jinfo:eu-repo/semantics/publishe