2006
DOI: 10.1021/jp056528d
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Effect of Bending Rigidity and Interfacial Permeability on the Dynamical Behavior of Water-in-Water Emulsions

Abstract: Phase separation in aqueous biopolymer mixtures results in the formation of an interface, separating two aqueous bulk phases. The properties of that interface are key parameters to understand and predict phenomena, such as the phase-separation process and deformation of droplets in a flow field. In these processes, the structures and sizes of the morphologies depend on the balance between viscous and interfacial forces. Normally, one assumes that the interfacial tension is the only important parameter regardin… Show more

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Cited by 40 publications
(44 citation statements)
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References 51 publications
(62 reference statements)
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“…Sample 6 is almost insensitive to the value of the bending rigidity. In this system relaxation is clearly dominated by permeability and surface tension, and we find A L 2 x = p 0 , also in agreement with [5]. This analysis shows conclusively that mass transfer has an important effect on the dynamic behavior of water-inwater emulsions, like phase-separated (bio)polymer solutions, liposomes, polymersomes, or coloidosomes.…”
Section: 066105 (2007) P H Y S I C a L R E V I E W L E T T E R Ssupporting
confidence: 89%
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“…Sample 6 is almost insensitive to the value of the bending rigidity. In this system relaxation is clearly dominated by permeability and surface tension, and we find A L 2 x = p 0 , also in agreement with [5]. This analysis shows conclusively that mass transfer has an important effect on the dynamic behavior of water-inwater emulsions, like phase-separated (bio)polymer solutions, liposomes, polymersomes, or coloidosomes.…”
Section: 066105 (2007) P H Y S I C a L R E V I E W L E T T E R Ssupporting
confidence: 89%
“…3 we have plotted the relaxation time for dextran, for both systems, and values of the bending rigidity of 0, 100, and 200k B T. We see that A in system 2 (close to the critical point) is very sensitive to variations in k. The relaxation in this system is dominated by the permeability and bending rigidity, and we find that A scales as ÿ1 A p kq 4 x . With q x 1=L x , where L x is the wavelength of the perturbations, we find A L 4 x = p k , a scaling that is in agreement with the scaling found for rigidity and permeability dominated coarsening during phase separation in [5]. Sample 6 is almost insensitive to the value of the bending rigidity.…”
Section: 066105 (2007) P H Y S I C a L R E V I E W L E T T E R Ssupporting
confidence: 84%
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