988 resultados para Polyelectrolyte- Surfactant-Complexes


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We have carried out small-angle X-ray diffraction studies on complexes formed by the anionic polyelectrolytes, namely, sodium salts of double and single stranded (ds and ss) DNA, poly( glutamic acid) ( PGA), poly( acrylic acid) (PAA), and poly( styrene sulfonate) (PSS) with a cationic surfactant system consisting of cetyltrimethylammonium bromide ( CTAB) and sodium 3-hydroxy-2-naphthoate (SHN). All complexes have a two-dimensional (2D) hexagonal structure at low SHN concentrations. DNA-CTAB-SHN complexes exhibit a hexagonal to lamellar transition near the SHN concentration at which CTAB-SHN micelles show a cylinder to bilayer transformation. On the other hand, PGA and PAA complexes form a 2D centered rectangular phase at higher SHN concentrations, and PSS complexes show a primitive rectangular structure. These results provide a striking example of polyion specificity in polyelectrolytesurfactant interactions.

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In this study, we used a rheological method to study the shape of DNA-cationic lipid complexes and model polyelectrolyte-lipid complexes. We introduced two kinds of anionic polyelectrolytes, sodium polygalacturonate (PGU) and sodium dextran sulfate (DSS), of varying size, as models for DNA. The prepared complexes were incubated under laminar flow conditions. The results show the same quantitative relation between the shape parameter of lipoplexes and the length of anionic polyelectrolytes, including DNA. The rheological behavior of PGU and DSS were similar to that of DNA. (C) 2004 Elsevier Inc. All rights reserved.

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Order-disorder transition (ODT) behavior in eicosylated polyethyleneimine (PEI20C) comblike polymer obtained by grafting n-eicosyl group on polyethyleneimine backbone was systematically investigated by the combination of differential scanning calorimetry (DSC), wide-angle X-ray diffraction (WAXD), Fourier transform infrared (FTIR) spectroscopy as well as solid-state high resolution nuclear magnetic resonance (NMR) spectroscopy. DSC investigations showed two obvious transitions, assigned to the transitions (1) from orthorhombic to hexagonal and (2) from hexagonal to amorphous phase, respectively. These transitions are induced by the variations of alkyl side chain conformation and packing structure with temperature changing, which consequently lead to the destruction of original phase equilibrium. The ODT behavior can also be confirmed by spectroscopic methods like WAXD, FTIR and NMR. The ordered structure and the transition behavior of the alkyl side chains confined by the PEI backbone are obviously different from those of pristine normal alkanes. The transition mechanism of ODT and the origin of the phase transition behavior in PEI20C comblike polymer were discussed in detail in this paper.

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Hochgeladene semiflexible kationische und anionische Polyelektrolyte wurden mit niedermolekularen Tensiden zu Polyelektrolyt-Tensid-Komplexen (PETK) umgesetzt und in organischen Lösungsmitteln mit Streumethoden und Rasterkraftmikroskopie charakterisiert. Die synthetisierten PETK wurden anschließend, mit dem Ziel einer strukturkontrollierten Komplexbildung, für die Bildung von Interpolyelektrolytkomplexen (IPEK) in organischen Lösungsmitteln verwendet und anhand ihres Komplexbildungsverhaltens mit wässrigen Systemen verglichen. Die Umsetzung von zylindrischen Polymerbürsten mit Poly(styrolsulfonat)-, bzw. Poly(2-vinylpyridinium)-Seitenketten mit entgegengesetzt geladenen Tensiden verlief, trotz einer Graftingdichte von eins, quantitativ. Mit Streumethoden konnte gezeigt werden, dass die gebildeten PETK in Lösung als molekulare Zylinder vorliegen. Die Synthese von pUC19-DNA-Tensidkomplexen (DNA-TK), die sich in Alkoholen gut lösen, ist nur in stark basischer Lösung gelungen. Während der Charakterisierung der DNA-TK mit Streumethoden zeigte sich eine starke Abhängigkeit des Trägheitsradius von dem Verhältnis DNA-/Salz+. Die Bildung von IPEK aus hochgeladenen Polyelektrolyt-Bürsten bzw. PETK-Bürsten wurde an verschiedenen Beispielen in Wasser und DMF durchgeführt und mit Streumethoden verfolgt. Alle Systeme zeigten ein zu der IPEK-Bildung von linearen Polyelektrolyten analoges Komplexbildungsverhalten. Bei der Komplexierung von Poly(styrolsulfonat)-Bürsten-Tensidkomplexen mit kommerziellen Polyamidoamin-G5-Dendrimeren (PAMAM) oder Poly(ethylenoxid) modifizierten Poly(ethylenimin)-Bürsten hingegen wurden über den gesamten Gewichtsbruchbereich mit Streumethoden und AFM zylindrische Aggregate gefunden, die den Dimensionen der Poly(styrolsulfonat)-Bürsten-Tensidkomplexe entsprechen. Durch statistische Höhenanalyse der AFM-Bilder wurde ein linearer Zusammenhang zwischen der Komplexhöhe und dem Gewichtsbruch an PAMAM, bzw. PEI-PEO gefunden, der auf die Zunahme der Molmasse der Komplexe durch Wachstum entlang des Zylinderdurchmessers hindeutet. Die Bildung von Aggregaten, mit mehr als einem Polyanion, wurde nicht beobachtet.

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Interpolyelektrolytkomplexe bilden sich spontan bei Mischung von Lösungen entgegengesetzt geladener Polyelektrolyte. Dabei sind die Haupttriebkräfte der Entropiegewinn durch die Freisetzung von niedermolekularen Gegenionen sowie die elektrostatischen Wechselwirkungen. In der letzten Zeit sind sie aufgrund ihrer zahlreichen biologischen und technischen Anwendungen in den Fokus des wissenschaftlichen Interesses gerückt. Vor allem die Anwendung von Komplexen aus DNA und kationischen Polyelektrolyten in der nonviralen Gentherapie wird vielfältig diskutiert. rnIn dieser Arbeit wird eine Polystyrolsulfonat-Bürste mit einer Pfropfdichte von 100 % mit einem kationischen Tensid komplexiert und der Komplex in verschiedenen organischen Lösungsmitteln charakterisiert. Dabei zeigt sich eine signifikante Abhängigkeit des Lösungsverhaltens von der Art und der Konzentration zugesetzter Salze. Dieser Polyelektrolyt-Tensid-Komplex wird anschließend als vereinfachtes Modellsystem für die Komplexierung von DNA verwendet. Als kationische Komponente dient zunächst ein kommerzielles PAMAM-Dendrimer der 5. Generation. Dabei steht die Erhaltung der zylindrischen Topologie der anionischen Polyelektrolytbürste in den gebildeten Komplexen im Vordergrund. Durch Variation des Lösungsmittels und des Protonierungsgleichgewichts werden die experimentellen Bedingungen eingegrenzt, bei denen eine solche topologische Kontrolle möglich ist. Es zeigt sich, dass durch die Verwendung von aprotischen organischen Lösungsmitteln gute Erfolge erzielt werden können. Des Weiteren wird das Komplexierungsverhalten stark durch den Zusatz einer Säure oder einer Base beeinflusst, sodass eine topologische Kontrolle mit einem großen Überschuss einer organischen Base auch in protischen Lösungsmitteln wie Wasser und Methanol möglich wird. Anschließend wird das gleiche Polyanion noch mit einer geschützten Polylysin-Bürste in DMF komplexiert, was zur Bildung von kinetisch kontrollierten Aggregaten führt. Die Bildung dieser Aggregate kann durch den Zusatz eines großen Überschusses an Base verhindert werden und es werden zylindrische Komplexe erhalten, die nur aus einer Polylysin-Bürste bestehen. rn

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The introduction of ionic single-tailed surfactants to aqueous solutions of EO18BO10 [EO = poly(ethylene oxide), BO = poly(1,2-butylene oxide), subscripts denote the number of repeating units] leads to the formation of vesicles, as probed by laser scanning confocal microscopy. Dynamic light scattering showed that the dimensions of these aggregates at early stages of development do not depend on the sign of the surfactant head group charge. Small-angle X-ray scattering (SAXS) analysis indicated the coexistence of smaller micelles of different sizes and varying polymer content in solution. In strong contrast to the dramatic increase of size of dispersed particles induced by surfactants in dilute solution, the d-spacing of corresponding mesophases reduces monotonically upon increasing surfactant loading. This effect points to the suppression of vesicles as a consequence of increasing ionic strength in concentrated solutions. Maximum enhancements of storage modulus and thermal stability of hybrid gels take place at different compositions, indicating a delicate balance between the number and size of polymer-poor aggregates (population increases with surfactant loading) and the number and size of polymer−surfactant complexes (number and size decrease in high surfactant concentrations).

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The interactions of sodium dodecyl sulfate (SDS) with poly(ethylene oxide)/poly(alkylene oxide) (E/A) block copolymers are explored in this study: With respect to the specific compositional characteristics of the copolymer, introduction of SDS can induce fundamentally different effects to the self-assembly behavior of E/A copolymer solutions. In the case of the E18B10-SDS system (E = poly(ethylene oxide) and B = poly(butylene oxide)) development of large surfactant-polymer aggregates was observed. In the case of B20E610-SDS, B12E227B12-SDS, E40B10E40-SDS, E19P43E19-SDS (P = poly(propylene oxide)), the formation of smaller particles compared to pure polymeric micelles points to micellar suppression induced by the ionic surfactant. This effect can be ascribed to a physical binding between the hydrophobic block of unassociated macromolecules and the non-polar tail of the surfactant. Analysis of critical micelle concentrations (cmc*) of polymer-surfactant aqueous solutions within the framework of regular solution theory for binary surfactants revealed negative deviations from ideal behavior for E40B10E40-SDS and E19P43E19-SDS, but positive deviations for E18B10-SDS. Ultrasonic studies performed for the E19P43E19-SDS system enabled the identification of three distinct regions, corresponding to three main steps of the complexation; SDS absorption to the hydrophobic backbone of polymer, development of polymer-surfactant complexes and gradual breakdown of the mixed aggregates. (C) 2008 Elsevier Inc. All rights reserved.

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An investigation is made of the influence from small amounts of the protein bovine serum albumin (BSA) on the lateral organization of low molecular weight surfactant sodium bis-2-ethylhexyl sulfosuccinate (AOT) at the air-water interface. Surface pressure (pi - A), surface potential (DeltaV - A) and Brewster angle microscopy (BAM) experiments were carried out, with particular emphasis on the monolayer stability under successive compression-expansion cycles. AOT monolayer is not stable at the air-water interface, which means that the majority of AOT molecules go into the aqueous subphase as monomers and/or normal micelles. When a waiting time elapses between spreading and compression, the surfactant monolayer tends to reorganize partially at the air-water interface, with a monolayer expansion being observed for waiting times as large as 12 h. The incorporation of very small amount of BSA (10(-9) M) at the interface, also inferred from BAM, increases the monolayer stability as revealed by pi - A and DeltaV - A results. For a waiting time of circa 3 h, the mixed monolayer reaches its maximum stability. This must be related to protein (and/or protein-surfactant complexes) adsorbed onto the AOT monolayer, thus altering the BSA conformation to accommodate its hydrophobic/hydrophilic residues. Furthermore, the effects from such small amounts of BSA in the monolayer formation and stabilization mean that the AOT monolayer responds cooperatively to BSA. (C) 2004 Elsevier B.V. All rights reserved.

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As técnicas de fluorimetria, condutometria, viscosimetria, turbidimetria, espalhamento de luz e espalhamento de raios-X a baixo ângulo (SAXS) foram empregadas no estudo da agregação de diferentes surfactantes aniônicos em presença de soluções aquosas diluídas de (hidroxipropil)celulose (HPC) 0,25% m/m, (hidroxipropilmetil)celulose (HPMC) 0,20% m/m e HPMC 0,10% m/m / NaCl 0,10 mol L-1. Também foram investigadas através de SAXS soluções concentradas de HPC (30, 40 e 50% m/m). Admitindo-se uma faixa geral de concentração, entre 10-4 e 10-1 mol L-1, foram utilizados neste estudo os surfactantes colato de sódio (CS), deoxicolato de sódio (DC), derivados dos sais biliares, e o alquilsintético dodecilsulafato de sódio (SDS). Observou-se que os polímeros contribuem diferentemente no processo de agregação de cada surfactante, evidenciado pela mudança dos valores da concentração de agregação crítica (CAC) em relação à concentração micelar crítica (CMC). Os resultados condutométricos confirmaram a interação éteres de celulose/sais biliares, embora a mesma tenha se mostrado mais fraca em relação a éteres de celulose/SDS. Os dados termodinâmicos demonstraram que a formação de agregados polímero/surfactante apresenta maior estabilidade do que as próprias micelas livres. Os resultados de viscosimetria e turbidimetria evidenciaram as diferenças estruturais entre HPC e HPMC, assim como entre os surfactantes. Através do espalhamento de luz dinâmico, verificou-se a existência de dois modos de correlação, rápido e lento. O primeiro é atribuído à cadeia polimérica isolada, agregados polímero/surfactante intramoleculares ou mesmo a micelas livres. Por sua vez, o modo lento relaciona-se a clusters poliméricos ou agregados polímero/surfactante intermoleculares. Adicionalmente, as curvas de distribuição dos tempos de relaxação demonstraram a influência de cada surfactante sobre a dinâmica dos polímeros. Tal influência é percebida antes mesmo da CAC, contrariando o modelo da interação polímero/surfactante proposto por Cabane. Os resultados de SAXS acusaram a formação de domínios líquido-cristalinos em xx soluções concentradas de HPC, assim como confirmaram a presença de micelas livres a altas concentrações de surfactantes nos sistemas diluídos. Em linhas gerais, os resultados indicaram a interação dos polímeros com SDS mais efetiva do que os mesmos polímeros e os sais biliares. No que tange à natureza do polímero, a HPC mostrou uma maior estabilidade na sua interação com os surfactantes do que a HPMC.

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UV-visible spectra of polyaniline and its polyelectrolyte complexes show evidence for different degree of protonation when equilibrated with different ionic strength at a particular pH, due to the Donnan effect. For pure polyaniline, when the fixed charge on the film is positive, protonation is higher ionic strength whereas, when the polyaniline is doped with a polyelectrolyte resulting in a net negative fixed charge on the film, the protonation is less at higher ionic strength.

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Polyelectrolyte complexes of polyaniline with both strong and weak anionic polyelectrolytes have been prepared. It has been found that the swellability of the complexes depends on the charge content of polyaniline, i.e., on the intercrosslinking between polyaniline (which is a polyacation) and polyanions. It has also been observed that polyaniline in the polyaniline-polystresulfonic acid complex exists in the conducting state when equilibrated with basic pH in aqueous media of moderately high ionic strength.

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Polyelectrolyte complex formation involving carboxymethylcellulose and quaternized poly(vinylpyridine) as the polyions has been studied using viscosity and u.v. spectroscopic methods. The influence of charge density and molecular weight of two polycations on the composition of the complex has been investigated at two different concentrations. The charge density of the polycation is found to have different influences on the composition at different concentrations. The molecular weight of the polycation and the location of the ionic site on the polycation do not show any effect on the composition. A drastic increase in the viscosity of the polyion mixture containing quaternized poly(2-vinylpyridine) in the non-stoichiometric ratio shows evidence for the existence of the soluble polyelectrolyte complex. The results are analysed on the basis of the relative extension of the polyelectrolyte chains.

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We report large scale deposition of tapered zinc oxide (ZnO) nanorods on Si(100) substrate by using newly designed metal-organic complex of zinc (Zn) as the precursor, and microwave irradiation assisted chemical synthesis as a process. The coatings are uniform and high density ZnO nanorods (similar to 1.5 mu m length) grow over the entire area (625 mm(2)) of the substrate within 1-5 min of microwave irradiation. ZnO coatings obtained by solution phase deposition yield strong UV emission. Variation of the molecular structure/molecular weight of the precursors and surfactants influence the crystallinity, morphology, and optical properties of ZnO coatings. The precursors in addition with the surfactant and the solvent are widely used to obtain desired coating on any substrate. The growth mechanism and the schematics of the growth process of ZnO coatings on Si(100) are discussed. (c) 2013 Elsevier B.V. All rights reserved.

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Polyelectrolyte complexes (PECs) of chitosan and phosphotungstic acid have been prepared and evaluated as novel proton-conducting membranes for direct methanol fuel cells. Phosphotungstic acid can be fixed within PECs membranes through strong electrostatic interactions, which avoids the decrease of conductivity caused by the dissolving of phosphotungstic acid as previously reported. Scanning electron microscopy (SEM) shows that the PECs membranes are homogeneous and dense. Fourier transform infrared spectroscopy (FTIR) demonstrates that hydrogen bonding is formed between chitosan and phosphotungstic acid. Thermogravimetric analysis (TGA) shows that the PECs membranes have good thermal stability up to 210 degrees C. The PECs membranes exhibit good swelling properties and low methanol permeability (P, 3.3 x 10(-7) cm(2) s(-1)). Proton conductivity (sigma) of the PECs membranes increases at elevated temperature, reaching the value of 0.024 S cm(-1) at 80 degrees C.

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Surface-modified Nafion (R) membrane was prepared by casting proton-conducting polyelectrolyte complexes on the surface of Nafion (R). The casting layer is homogeneous and its thickness is about 900 nm. The proton conductivity of modified Nafion (R) is slightly lower than that of plain Nafion (R); however, its methanol permeability is 41% lower than that of plain Nafion (R). The single cells with modified Nafion (R) exhibit higher open circuit voltage (OCV = 0.73 V) and maximal power density (P-max = 58 mW cm(-2)) than the single cells with plain Nafion (R) (OCV = 0.67 V, P x = 49 mW cm-2). It is a simple, efficient, cost-effective approach to modifying Nafion (R) by casting proton-conducting materials on the surface of Nafion (R).