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4.3.- Appended papers. In the present work, the solution behaviour <strong>and</strong> surface adsorption properties <strong>of</strong> three different block copolymer (E12S10, E10S10E10 <strong>and</strong> E137S18E137), have been studied. These block copolymers display different volume-to-length ratios <strong>of</strong> the hydrophobic block <strong>and</strong> <strong>of</strong> relative lengths <strong>of</strong> the poly(oxyethylene) block ; <strong>and</strong> also polymer architecture may have an important role in controlling the morphology <strong>of</strong> polymeric aggregates <strong>and</strong> surface adsorption behaviour <strong>of</strong> these copolymers. To known the influence <strong>of</strong> such parameters, we studied the self-assembly properties <strong>and</strong> the different structural aggregates <strong>of</strong> the three copolymers in aqueous solution. For copolymer E12S10, coexistence <strong>of</strong> spherical micelles with vesicular structures is detected. To the best <strong>of</strong> our knowledge, the spontaneous formation <strong>of</strong> vesicles by poly(oxystyrene)- poly(oxyethylene) block copolymers has been first reported here. On the other h<strong>and</strong>, formation <strong>of</strong> elongated micelles upon self-assembly <strong>of</strong> copolymer E10S10E10 in dilute solution is elucidated from light scattering <strong>and</strong> transmission electron techniques. In the case <strong>of</strong> E137S18E137, typical spherical micelles are observed, as expected. The micellization properties <strong>of</strong> the latter copolymer had been already partially studied previously (89)(90), <strong>and</strong> the present study completes this gap. On the other h<strong>and</strong>, fundamental studies <strong>of</strong> polystyrene oxide-based block copolymers performed at either the air-water or the water-organic solvent interface can provide valuable information on their interfacial phase behaviour to further guide their possible use in different biomedical <strong>and</strong> coating applications. To fill this gap, in the present work, we studied the surface behaviour <strong>and</strong> surface properties <strong>of</strong> these three copolymers, E12S10, E10S10E10 <strong>and</strong> E137S18E137, by different techniques. To do this work, different techniques such as surface tension, Langmuir-Blodgett through, drop tensiometry, light scattering, transmission <strong>and</strong> scanning electron microscopies (TEM <strong>and</strong> SEM), atomic force microscopy (AFM), polarized optical microscopy (POM) <strong>and</strong> rheometry were used. 123
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Grupo de Física de Coloides y Pol
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Agradecimientos A mi Familia A mi P
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v List of papers I. Self-assembly p
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2.3 2.4 2.5 2.6 2.7 2.8 2.9 2.10 2.
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5.4 5.5 5.3.2 5.5.1 Chapter 6 Kinet
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amiloides de la proteína albúmina
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vesiculares son el resultado de la
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origina debido a condiciones ambien
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con las fibras vecinas más cercana
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Abstract In the present work, we in
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[Au]/[protein] molar ratio and numb
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synthetic polymers are obtained fro
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On the other hand, in terms of chem
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Additionally, to obtain a better kn
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therefore, characteristic of solid
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presence of electrostatic charge in
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Contents 2.1 2.2 2.3 2.4 2.5 2.6 2.
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where w is the meniscus’ weight d
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that they exert little force one on
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This oscillating dipole acts as an
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(APD) and its associated optics (pi
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where r is the distance of the dipo
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When , the former equation can be s
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autocorrelation function (ACF). In
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and, therefore, . The autocorrelati
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A transmission electron microscope
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2.5.- Atomic force microscopy (AFM)
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ecause of the energy loss in the ex
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Figure 2.15. Schematic representati
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ackbone of proteins. Since proteins
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According to classical mechanics, t
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chemical composition, configuration
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2.9.1.- Viscoelasticity Many materi
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where is the total strain rate, whi
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Using equations 2.40 and 2.41 in eq
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scattering process that incoming X-
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maximum intensity of the peak, Imax
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translation of the reciprocal latti
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Fibrillation Process of Human Serum
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12394 J. Phys. Chem. B, Vol. 113, N
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12398 J. Phys. Chem. B, Vol. 113, N
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5 10 15 20 25 30 35 40 45 Soft Matt
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5 10 15 20 25 r h,app = kT/(6πηD
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5 10 15 20 25 30 35 40 45 50 below,
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5 10 15 20 25 30 55 Figure 3: Selec
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10 15 Soft Matter Cite this: DOI: 1
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5 10 15 Soft Matter Cite this: DOI:
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5 65. L. A. Sikkink, M. Ramirez-Alv
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ions would interact electrostatical
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pubs.acs.org/JPCL Figure 3. (a) Tim
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(54) Almeida, N. L.; Oliveira, C. L
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netospirillum magneticum strain AMB
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One-Dimensional Magnetic Nanowires
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One-Dimensional Magnetic Nanowires
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One-Dimensional Magnetic Nanowires
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temperatures, and solvent polarity.
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Conclusions The work has two parts:
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equire a highly organized and unsta
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References 1. Hiemenz, Paul C. Poly
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33. Wang, Z. L. HANDBOOK OF MICROSC
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67. Polymers Get Organized. Bucknal
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94. Are there Pathways for Protein
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123. Designing conditions for in vi
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151. SERS-based diagnosis and biode