510 resultados para SAXS


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In the present work, nanostructured blends were prepared from double crystalline diblock copolymer poly(ɛ-caprolactone)-block-poly(ethylene oxide) and homopolymer poly(4-vinyl phenol) (PVPh). The diblock copolymer PEO-b-PCL consists of two immiscible crystallizable blocks wherein both PEO and PCL blocks can form hydrogen bonds with PVPh. In these A-b-B/C diblock copolymer/homopolymer blends, microphase separation takes place due to the disparity in intermolecular interactions; specifically, PVPh and PEO block interact strongly whereas PVPh and PCL block interact weakly. The TEM and SAXS results show that the cubic PEO-b-PCL diblock copolymer changes into ordered hexagonal cylindrical morphology upon addition of 20 wt % PVPh followed by disordered bicontinuous phase in the blend with 40 wt % PVPh and then to homogeneous phase at 60 wt % PVPh and above blends. Up to 40 wt % PVPh there is only weak interaction between PVPh and PCL due to the selective hydrogen bonding between PVPh and PEO. However, with higher PVPh concentration, the blends become homogeneous since a sufficient amount of PVPh is available to form hydrogen bonds with both PEO and PCL. A structural model was proposed to explain the self-assembly and microphase morphology of these blends based on the experimental results obtained. The formation of nanostructures and changes in morphologies depend on the relative strength of hydrogen bonding interaction between each block of the block copolymer and the homopolymer.

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This paper investigates the effect of both the mixing technique and heating rate during cure on the dispersion of montmorillonite (MMT) clay in an epoxy resin. The combination of sonication and using a 10. °C/min heating rate during cure was found to facilitate the dispersion of nanoclay in epoxy resin. These processing conditions provided a synergistic effect, making it possible for polymer chains to penetrate in-between clay galleries and detach platelets from their agglomerates. As the degree of dispersion was enhanced, the flexural modulus and strength properties were found to decrease by 15% and 40%, respectively. This is thought to be due to individual platelets fracturing in the nanocomposite. Complementary techniques including X-ray diffraction (XRD), small angle X-ray scattering (SAXS), scanning electron microscopy-energy dispersive X-ray spectroscopy (SEM-EDX), transmission electron microscopy (TEM) and optical microscopy were essential to fully characterise localised and spatial regions of the clay morphologies.

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Here we report a facile method for controlling the morphology and porosity of porous siloxane membranes through manipulation of the water content of precursor microemulsions. The polymerizable microemulsion precursors consisted of a methacrylate-terminated siloxane macromonomer (MTSM) as the oil phase, nonionic surfactant (Teric G9A8), water, and cosurfactant (isopropanol). Photo-polymerization of the oil phase in the parent microemulsion solutions resulted in polymeric solids, and subsequent removal of the extractable components yielded porous PDMS membranes. The pre-cured parent microemulsion solutions and post-cured polymers were characterized by small angle X-ray scattering (SAXS) while the nanostructures of extracted porous polymer membranes were characterized by SAXS, scanning electron microscopy (SEM) and mercury porosimetry. The results indicated that nano- and micro-structures of the membranes could be modulated by the water content of the precursor microemulsions. Further, in situ photo-rheometry was used to follow the microemulsion polymerization process. The rate of polymerization and the mechanical properties of the resulting PDMS membranes also depend on the water content of precursor microemulsions. This study demonstrates a simple approach to the fabrication of a variety of novel porous PDMS membranes with controllable morphology and porosity.

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The intergallery expansion development of a series of differently modified montmorillonite polystyrene nanocomposites was directly observed with time-resolved in situ small-angle X-ray scattering (SAXS) using synchrotron radiation. The results indicated that the interlayer expansion varied depending on the clay modification and the chemical compatibility of the clay modifiers with the styrene monomer. The influence of the differently modified clays on the free radical polymerization was also investigated, particularly the effect on the conversion of styrene and molecular weight evolution of the polymer. On the basis of the kinetic study of the polymerization of styrene in the presence of varied modified clay particles, the intergallery expansion mechanism was postulated and discussed for different composite morphologies. Such studies provide an important guideline for the design of clay modifiers and development of clay–polymer nanocomposites.

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Microphase separation through competitive hydrogen bonding interactions in ABC/D triblock copolymer/ homopolymer complexes is studied for the first time. This study investigated self-assembled nanostructures that are obtained in the bulk, by the complexation of a semicrystalline polystyrene-block-poly(4-vinylpyridine)-block-poly(ethylene oxide) (SVPEO) triblock copolymer with a poly(4-vinyl phenol) (PVPh) homopolymer in tetrahydrofuran (THF). In these complexes, microphase separation takes place due to the disparity in intermolecular interactions among PVPh/P4VP and PVPh/PEO pairs. At low PVPh concentrations, PEO interacts relatively weakly with PVPh, whereas in the complexes containing more than 30 wt% PVPh, the PEO block interacts considerably with PVPh, leading to the formation of composition-dependent nanostructures. SAXS and TEM results indicate that the cylindrical morphology of a neat SVPEO triblock copolymer changes into lamellae structures at 20 wt% of PVPh then to disordered lamellae with 40 wt% PVPh. Wormlike structures are obtained in the complex with 50 wt%PVPh, followed by disordered spherical microdomains with size in the order of 40–50 nm in the complexes with 60–80 wt% PVPh. Moreover, when the content of PVPh increases to 80 wt%, the complexes show a completely homogenous phase of PVPh/P4VP and PVPh/PEO with phase separated spherical PS domains. The fractional crystallization behavior in SVPEO and complexes at lower PVPh content was also examined. A structural model was proposed to explain the microphase separation and self-assembled morphologies of these complexes based on the experimental results obtained. The formation of nanostructures and changes in morphologies depend on the relative strength of hydrogen bonding interactions between each component block of the copolymer and the homopolymer.

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The effect of varying the position of the azobenzene group within two comparable photoresponsive amphiphiles on their capability to form lyotropic liquid crystals (LLCs) was investigated in detail in this study. Two photoresponsive amphiphiles having comparable structures were designed and synthesized consisting of hydrophilic oligooxyethylene units, a hydrophobic alkyl chain and a light-sensitive azobenzene moiety. When the azobenzene group was located in the middle of the hydrophobic alkyl chain, multiple LLC phases were observed at various water contents in the azo-surfactant–water binary system. In contrast, when the azobenzene group was directly attached to the hydrophilic domain, the azo-surfactant–water binary system exhibited only lamellar phases. The temperature dependence of these self-organised nanostructures was also investigated by the combination of small angle X-ray scattering (SAXS), differential scanning calorimetry (DSC), and rheology. Under alternating UV and visible light irradiation, reversible trans–cis photoisomerization of the azobenzene group occurred efficiently in dilute solution for both azo-surfactants. However, only photoisomerization of the surfactant possessing the azobenzene group localized in the middle of the alkyl chain induced significant changes in the self-assembled structure and its bulk properties. This study demonstrates that self-assembly and photoresponsive behaviour of photosensitive amphiphiles is extremely sensitive to the position of the photoactive moiety within the surfactant molecular architecture.

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Immiscible and miscible blends of poly(vinylidene fluoride) (PVDF) and acrylic rubber (ACM) were subjected to dynamic vulcanization to investigate the effect of crosslinking on phase separation. As a result of different processability, mixing torque behavior of miscible and immiscible blends was significantly different from one another. Scanning electron microscopy (SEM) was used to investigate the morphology of the system. After dynamic vulcanization, submicron ACM droplets were observed in the samples near the binodal curve of the system under mixing conditions. Small angle X-ray scattering (SAXS) and differential scanning calorimetry (DSC) analysis were used to investigate the effect of dynamic vulcanization on the lamellar structure of the system. It was shown that for samples near the boundary of phase separation, increasing the crosslink density led to a decrease in the lamellar long period (L) as a sign of increment of crosslink density induced phase decomposition. Effects of shear rate on the final morphology of the system were investigated by changing the mixing temperature and by comparing the results of dynamic vulcanization at one phase and two phase regions.

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In this work, the crystallization rates and spherulitic growth rate of miscible blends of poly(vinylidene fluoride) (PVDF) and acrylic rubber (ACM) were determined using differential scanning calorimetry (DSC), real-time FTIR, and optical microscopy. FTIR results suggest that blending does not induce the creation of polymorphic crystalline forms of PVDF. SAXS data demonstrate the formation of interlamellar structure after blending. The fold surface-free energy (σ e) was analyzed and compared using different thermal analysis techniques. The isothermal crystallization curves obtained using real-time FTIR and DSC explored in two different methods: t 1/2 or Avrami equation. While the Avrami equation is more widespread and precise, both analytical methods gave similar free energy of folding values. However, it was found that the direct optical method of measuring spherulitic growth rate yields σ e values 30-50 % lower than those obtained from the overall crystallization rate data. Conversely, the σ e values were found to increase with increasing amorphous ACM phase content regardless of the analytical methods.

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The growth mechanism and kinetics of mesoporous silica nanoparticles (MSNs) were investigated for the first time by using a synchrotron time-resolved small-angle X-ray scattering (SAXS) analysis. The synchrotron SAXS offers unsurpassed time resolution and the ability to detect structural changes of nanometer sized objects, which are beneficial for the understanding of the growth mechanism of small MSNs (∼20 nm). The Porod invariant was used to quantify the conversion of tetraethyl orthosilicate (TEOS) in silica during MSN formation, and the growth kinetics were investigated at different solution pH and temperature through calculating the scattering invariant as a function of reaction time. The growth of MSNs was found to be accelerated at high temperature and high pH, resulting in a higher rate of silica formation. Modeling SAXS data of micelles, where a well-defined electrostatic interaction is assumed, determines the size and shape of hexadecyltrimethylammonium bromide (CTAB) micelles before and after the addition of TEOS. The results suggested that the micelle size increases and the micelle shape changes from ellipsoid to spherical, which might be attributed to the solubilization of TEOS in the hydrophobic core of CTAB micelles. A new "swelling-shrinking" mechanism is proposed. The mechanism provides new insights into understanding MSN growth for the formation of functional mesoporous materials exhibiting controlled morphologies. The SAXS analyses were correlated to the structure of CTAB micelles and chemical reaction of TEOS. This study has provided critical information to an understanding of the growth kinetics and mechanism of MSNs.

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We present a facile method to prepare thermally stable and mechanically robust crosslinked lyotropic liquid crystals (LLCs) through incorporation of a polymerizable amphiphile into a binary LLC system comprising commercially available surfactant Brij 97 and water. Thermal stability and mechanical properties of the polymerized LLCs were significantly enhanced after polymerization of the incorporated polymerizable surfactant. The effect of incorporating a polymerizable amphiphile on the phase behavior of the LLC system was studied in detail. In situ photo-rheology was used to monitor the change in the mechanical properties of the LLCs, namely the storage modulus, loss modulus, and viscosity, upon polymerization. The retention of the LLC nanostructures was evaluated by small angle X-ray scattering (SAXS). The ability to control the thermal stability and mechanical strength of LLCs simply by adding a polymerizable amphiphile, without tedious organic synthesis or harsh polymerization conditions, could prove highly advantageous in the preparation of robust nanomaterials with well-defined periodic structures.

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The formation of purely metallic meso-porous metal thin films by partial interface coalescence of self-assembled metal nano-particles across aqueous solutions of Pluronics triblock lyotropic liquid crystals is demonstrated for the first time. Small angle X-ray scattering was used to study the influence of the thin film composition and processing conditions on the ordered structures. The structural characteristics of the meso-structures formed demonstrated to primarily rely on the lyotropic liquid crystal properties while the nature of the metal nano-particles used as well as the their diameters were found to affect the ordered structure formation. The impact of the annealing temperature on the nano-particle coalescence and efficiency at removing the templating lyotropic liquid crystals was also analysed. It is demonstrated that the lyotropic liquid crystal is rendered slightly less thermally stable, upon mixing with metal nano-particles and that low annealing temperatures are sufficient to form purely metallic frameworks with average pore size distributions smaller than 500 nm and porosity around 45% with potential application in sensing, catalysis, nanoscale heat exchange, and molecular separation.

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In this work, silica embedded with a spirooxazine dye was prepared by hydrolysis of silanes that bear a nonhydrolyzable group of different structures through a sol-gel route in the presence of a spirooxazine dye, and the pore dimension and photochromic properties of photochromic silica coatings on fabric were studied. The pore dimension in the silica was examined by small angle X-ray scattering (SAXS), transmission electron microscopy (TEM), and nitrogen adsorption porosimetry. The SAXS results revealed that the distance between pores was in the range between 0.8 nm and 1.9 nm and it increased with increasing the size of the non-hydrolyzable group. Pore size measured by nitrogen adsorption porosimetry was in the range of 2.1-2.7 nm. The photochromic optical absorption was influenced mainly by the hydrophobicity of the non-hydrolyzable groups, while the color changing rates were influenced by the steric effect of the non-hydrolyzable groups and their interaction with the dye.

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Neste trabalho inicialmente foi sintetizado o precursor organoalcoxisilano 3- anilinapropiltrimetoxisilano, APTMS, a partir da reação entre a anilina e o 3- cloropropiltrimetoxisilano, CPTMS, usando hidreto de sódio, NaH, como ativador de base. O precursor inorgânico tetraetilortosilicato, TEOS, foi polimerizado na presença do precursor orgânico, e catalisador. Durante a etapa de polimerização dos precursores alcóxidos, foram investigadas as influências da temperatura, do tipo e concentração do catalisador e da concentração de precursor orgânico adicionado nas propriedades finais dos híbridos anilinapropilsilica resultantes. Os materiais híbridos foram caracterizados através das técnicas: espectroscopia no infravermelho (FT-IR), técnica de espalhamento de Raios-x a baixos ângulos (SAXS), microscopia eletrônica de varredura (SEM), isotermas de adsorção e dessorção de nitrogênio, análise elementar, espectroscopia de aniquilação de pósitrons (PALS), análise termogravimétrica (TGA), espectroscopia de elétrons dispersos (EDS). A potencialidade de aplicação dos híbridos obtidos como materiais adsorventes na extração dos cátions Cu(II), Zn(II), Cd(II) e Co(II), em solução, foi investigada usando-se isotermas de adsorção pelo método batelada. Através das técnicas de caracterização foi possível observar que as propriedades morfológicas dos materiais como área superficial, distribuição do tamanho de poros, forma e tamanho das partículas, além da estabilidade e grau de incorporação orgânica podem ser controladas em maior ou menor grau, dependendo da variável usada durante a polimerização dos precursores alcóxidos. O material apresentou propriedades promissoras como adsorvente seletivo para o cobre.

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A utilidade de alguns polímeros depende principalmente de suas propriedades elétricas, ópticas, bioquímicas e térmicas, porém na maioria dos exemplos a propriedade fundamental para as aplicações reside em suas propriedades mecânicas. Os mecanismos de deformação em polímeros semi-cristalinos são em geral complexos e dependem do arranjo e do tamanho dos cristais. A deformação plástica de polímeros semi-cristalinos é produzida pela força aplicada ao sistema, com modificações de suas propriedades termodinâmicas e morfológicas, obtendo-se materiais com novas propriedades e aplicações. Os sistemas estudados neste trabalho, consistem de amostras de polipropileno isotático, (i-PP) comercial, fornecidas pela OPP Petroquímica (III Pólo Petroquímico – Triunfo / RS). As amostras, na forma de grânulos, foram moldadas pelo processo de injeção onde duas massas molares diferentes foram investigadas. As placas moldadas por injeção, com espessura de aproximadamente 3,0 mm, foram cortadas nas dimensões padrões de 17,2 mm X 4,7 mm e após, deformadas plasticamente por compressão plana uniaxial à temperatura ambiente. A análise da morfologia e cristalinidade deste material foram realizadas utilizando as técnicas de difração raios-X em alto ângulo (WAXD), espalhamento de raios-X em baixo ângulo (SAXS), Microscopia Eletrônica de Varredura (MEV), e Microscopia Eletrônica de Transmissão (MET). Através da técnica de WAXD foi possível a identificação das diferentes fases cristalinas α e β do i-PP, antes e depois das amostras serem deformadas por compressão uniaxial. A determinação da cristalinidade foi realizada via difração de raios-X, utilizando as geometrias θ - 2θ e de Debye Scherrer, sendo a quantificação realizada a partir da área dos picos cristalinos obtidos a partir da indexação das reflexões de Bragg, utilizando o programa FULLPROF. Como resultado obtido, foi verificado uma significativa diminuição da cristalinidade com o aumento da deformação por compressão aplicada sobre as amostras. Com as medidas de SAXS, foram observados os perfis de espalhamento anisotrópicos e isotrópicos para as amostras sem deformação para maior e menor massa molar, respectivamente. O período longo (L) do material, definido pela soma da espessura lamelar do cristal (dc) e a espessura da camada amorfa (da), também foi obtido para estas amostras. A deformação causou uma diminuição do L, o que levou a diminuição da dc, seguido pelo aumento da da. Porém, com o aumento da deformação observa-se uma diminuição das intensidades espalhadas em torno do eixo azimutal. Este efeito pode ser atribuído ao aumento da fase amorfa seguido pela diminuição da fase cristalinidade. As modificações morfológicas ocorridas nas estruturas esferulíticas e lamelares foram avaliadas utilizando a Microscopia Eletrônica de Varredura (MEV), e a Microscopia Eletrônica de Transmissão (MET). O efeito da deformação plana por compressão ficou registrado nas imagens de XXIX MEV e MET, onde verificou-se o alongamento das estruturas esferulíticas na direção de fluxo, seguido da destruição parcial da mesma em deformação por compressão maiores. As imagens obtidas em MEV e MET, foram tratadas a fim de se verificar o grau de orientação e a distribuição da orientação em nível microestrutural por meio do método direto das secantes em um plano e da rosa dos interceptos. Neste caso, quando a rosa apresenta duas pétalas, tem-se um eixo de orientação; com quatro pétalas, dois eixos de orientação, e assim sucessivamente.Em um sistema isométrico sem nenhuma orientação, a rosa dos interceptos apresentará como resultado uma circunferência. Os resultados obtidos para as imagens de MEV e MET em nível esferulítico mostraram que a rosa dos interceptos parte de uma estrutura simétrica com baixo grau de orientação para uma estrutura orientada definida por um sistema de duas pétalas, seguido pelo aumento do grau de orientação para pressões de deformações maiores. Para as imagens de MET em nível lamelar observou-se o aumento do grau de orientação devido o aumento da deformação até 10 MPa. Neste caso, a rosa dos interceptos parte de uma estrutura definida por quatro pétalas (sistema dois eixos de orientação) para uma estrutura de duas pétalas, apresentando um sistema com um eixos de orientação. Porém, para pressões de deformações entre 20-3200 MPa observou-se a diminuição do grau de orientação, pois uma maior desordem é observado nas estruturas devido a amorfização do material, sendo a rosa dos interceptos demostrada por uma estrutura simétrica. Medidas com termopar foram realizadas para verificação do comportamento térmico no momento da deformação. Neste caso, foi verificado um aumento significativo da temperatura com o aumento da deformação. Porém, para as amostras deformadas com 3200 MPa foi observado dois picos de temperatura. Onde o primeiro pico foi atribuído ao comportamento adiabático seguido pela relaxação do material, enquanto o segundo pico foi verificado com grande aumento de temperatura no momento da explosão do material.