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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Evans, Robert
University of Bristol
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2022Density depletion and enhanced fluctuations in water near hydrophobic solutes: identifying the underlying physicscitations
- 2009Strength and Reliability of Wood for the Components of Low-cost Wind Turbines: Computational and Experimental Analysis and Applicationscitations
- 2009Strength and Reliability of Wood for the Components of Low-cost Wind Turbines: Computational and Experimental Analysis and Applicationscitations
- 2006Modelling of a metal-containing hepcidincitations
- 2002Binary star-polymer solutionscitations
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article
Binary star-polymer solutions
Abstract
<p>Using an effective logarithmic-Gaussian pair potential that models the interaction between star polymers, we compare the hypernetted chain (HNC) and random phase approximations (RPA) for calculating the bulk structure (including the Fisher-Widom and Lifshitz lines), thermodynamic functions and phase diagram of a phase-separating binary fluid of star polymers, of two-arm length ratio 2:1. Thereby, the stars considered here are equivalent to linear chains in the mid-point representation of their effective interaction. We find that at densities where the star coronas overlap, the quasi-exact HNC and RPA give very similar results. Using a density functional approach, with a functional which generates the RPA, we calculate properties of the inhomogeneous binary fluid. We determine the surface tension and one-body density profiles at the free fluid-fluid interface. For states well removed from the critical point the profiles exhibit pronounced oscillations. For a purely repulsive planar wall potential that models the effective potential between a star polymer and a hard wall, we find a first-order wetting transition with the associated pre-wetting line.</p>