Sol phase and sol-gel transition in SnO2 colloidal suspensions

The effect of concentration on the structure of SnO2 colloids in aqueous suspension, on their spatial correlation and on the gelation process was studied by small angle x-ray scattering (SAXS). The shape of the experimental SAXS curves varies with suspension concentration. For diluted suspensions ([SnO2] less than or equal to 0.13 mol L-1), SAXS results indicate the presence of colloidal fractal aggregates with an internal correlation length xi congruent to 20 Angstrom, without any noticeable spatial correlation between them. This suggests that the aggregates are spatially arranged without any significant interaction like in ideal gas structures. For higher concentrations ([SnO2] = 0.16, 0.32, and 0.64 mol L-1), the colloidal aggregates are larger (xi = 24 Angstrom) and exhibit a certain degree of spatial correlation between them. The pair correlation function corresponding to the sol with the highest concentration (0.92 mol L-1) reveals a rather strong short range order between aggregates, characteristic of a fluid-like structure, with an average nearest-neighbor distance between aggregates d(1) = 125 Angstrom and an average second-neighbor distance d(2) = 283 Angstrom. The pair distribution function remains essentially invariant during the sol-gel transition, suggesting that gelation involves the formation of a few points of connection between the aggregates resulting in a gel network constituted by essentially linear chains of clusters..

Synthesis and properties of branched polyethylene/high-density polyethylene blends using a homogeneous binary catalyst system composed of early and late transition metal complexes

Branched polyethylene/high-density polyethylene blends (BPE/HDPE) with a wide range of molecular weights, melt flow indexes (MFI), and intrinsic viscosity were prepared using the homogeneous binary catalyst system composed by Ni(alpha-diimine)Cl-2 (1) (alpha-diimine = 1,4-bis(2,6-diisopropylphenyl)-acenaphthenediimine) and {Tp(Ms*)} TiCl3 (2) (Tp(Ms*)=hydridobis(3-mesitylpyrazol-1-yl)(5-mesityl-pyrazol-1-yl)) activated with MAO and/or TIBA in hexane at two different polymerization temperatures (30 and 55 degreesC) and by varying the nickel loading molar fraction (x(Ni)). At all Temperatures, a non-linear correlation between the x(Ni) and the productivity was observed, suggesting the occurrence of a synergistic effect between the nickel and the titanium catalyst precursors, which is more pronounced at 55 degreesC. The molecular weight of the BPE/HDPE blends considerably decreases with increasing Al/M molar ratio. The melt flow indexes (MFI) and intrinsic viscosities (eta) are strongly affected by x(Ni), but the melting temperatures are nearly constant, 132 +/- 3 degreesC. Dynamic mechanical thermal analysis (DMTA) shows the formation of different polymeric materials where the stiffness vanes according, to the x(Ni) and temperature used in the polymerization reaction. The surface morphology of the BPE/HDPE blends studied by scanning electron microscopy (SEM) revealed a low miscibility between the PE phases resulting in the formation of a sandwich structure after etching with o-xylene.

Investigation on the structural properties in Er-doped PbTiO3 compounds: A correlation between experimental and theoretical results

The aim of this work is to investigate the structural properties of the (Pb1-xErx)TiO3 (PET) powders, with x varying from 0.01 to 0.08, prepared by the polymeric precursor method. Combined X-ray diffraction, Raman spectroscopy and ab initio calculation reveal a diffuse phase-transition of a tetragonal to a cubic phase. The crystalline models built allowed to calculate electronic properties and to analyze the behavior of the doping element in the structure of the material, which are consistent with the experimental results that indicate the beginning of phase-transition from tetragonal to cubic. (C) 2007 Elsevier B.V. All rights reserved.

Microscopic studies on the transition between the sigmoid sinus, the superior bulb of the jugular vein and the first portion of the internal jugular vein

The author studied the structure of the tissue components of the tunicae of the terminal segment of the sigmoid sinus, particularly at the level of the transition between the sigmoid sinus, the superior bulb of the jugular vein and the first portion of the human internal jugular vein; it was established that the transition between the sigmoid sinus and the first portion of the internal jugular vein occupies the whole extension of the superior bulb of the jugular vein up to the inferior third of the first portion of this vessel. These vascular walls exhibit a structure similar to that of the dura, i.e. the tunica adventitia is formed by fascicles of collagenic fibers which describe discontinuous spirals, more open proximal to the beginning of the first portion of the internal jugular vein. Approximately in the inferior third of the first portion of the internal jugular vein, there appear fascicles of smooth muscle fibers which are arranged similarly to those of the venous walls. The tunica intima of these vascular segments exhibits an endothelium resting on a network of elastic fibers which may play the role of an internal elastic lamina. From the bony border of the jugular foramen there originates a connective system whose fascicles of collagenic and elastic fibers incorporate to the wall of the internal jugular vein after describing a stretch in spiral around the vascular lumen.

Smooth landscape solvent dynamics in electron transfer reactions

Solvent effects play a major role in controlling electron-transfer reactions. The solvent dynamics happens on a very high-dimensional surface, and this complex landscape is populated by a large number of minima. A critical problem is to understand the conditions under which the solvent dynamics can be represented by a single collective reaction coordinate. When this unidimensional representation is valid, one recovers the successful Marcus theory. In this study the approach used in a previous work [V. B. P. Leite and J. N. Onuchic; J. Phys. Chem. 100, 7680 (1996)] is extended to treat a more realistic solvent model, which includes energy correlation. The dynamics takes place in a smooth and well behaved landscape. The single shell of solvent molecules around a cavity is described by a two-dimensional system with periodic boundary conditions with nearest neighbor interaction. It is shown how the polarization-dependent effects can be inferred. The existence of phase transitions depends on a factor y proportional to the contribution from the two parameters of the model. For the present model, γ suggests the existence of weak kinetic phase transitions, which are used in the analysis of solvent effects in charge-transfer reactions. © 1999 American Institute of Physics.

Dynamics of the deconfinement transition

We estimate the dissipation coefficient Γ that appears in Ginzburg-Landau-Langevin equations that describe phenomenologically the deconfinement transition in QCD. This is done through the implementation of Glauber dynamics of pure SU(3) lattice gauge theory. The coefficient Γ is extracted from the short-time exponential growth of the equal time correlation function of the order parameter. Although the absolute determination of Γ is ambiguous due to the difficulties in relating real time and Monte Carlo time, its relative temperature dependence can be obtained with much less arbitrariness. © 2007 American Institute of Physics.

Depinning and vortex-glass-like transition in Nb with uncorrelated disorder

Studies of the third harmonic of the AC-susceptibility were conducted to detect the boundaries of the linear regime of the magnetic response of granular Nb samples. These studies reveal the extent of the region, on the phase diagram, where the magnetic response is linear, which corresponds to the disordered phase of Vortex Matter. The present work addresses the correlation between a linear response and experimental parameters such as the frequency and the amplitude of the excitation field. The order-disorder border has been extracted from the onset temperature of the third harmonic measured at low-frequencies and low-excitation fields in the presence of dc magnetic fields. © 2008 IOP Publishing Ltd.

Geologia, mineralogia e geoquímica dos fosfatos de Sapucaia (Bonito - PA)

O depósito mineral de Sapucaia, situado no município de Bonito, região nordeste do Estado do Pará, é parte de um conjunto de ocorrências de fosfatos de alumínio lateríticos localizados predominantemente ao longo da zona costeira dos estados do Pará e Maranhão. Estes depósitos foram alvos de estudo desde o início do século passado, quando as primeiras descrições de “bauxitas fosforosas” foram mencionadas na região NW do Maranhão. Nas últimas décadas, com o crescimento acentuado da demanda por produtos fertilizantes pelo mercado agrícola mundial, diversos projetos de exploração mineral foram iniciados ou tiveram seus recursos ampliados no território brasileiro, dentre estes destaca-se a viabilização econômica de depósitos de fosfatos aluminosos, como o de Sapucaia, que vem a ser o primeiro projeto econômico mineral de produção e comercialização de termofosfatos do Brasil. Este trabalho teve como principal objetivo caracterizar a geologia, a constituição mineralógica e a geoquímica do perfil laterítico alumino-fosfático do morro Sapucaia. A macrorregião abrange terrenos dominados em sua maioria por rochas pré-cambrianas a paleozóicas, localmente definidas pela Formação Pirabas, Formação Barreiras, Latossolos e sedimentos recentes. A morfologia do depósito é caracterizada por um discreto morrote alongado que apresenta suaves e contínuos declives em suas bordas, e que tornam raras as exposições naturais dos horizontes do perfil laterítico. Desta forma, a metodologia aplicada para a caracterização do depósito tomou como base o programa de pesquisa geológica executada pela Fosfatar Mineração, até então detentora dos respectivos direitos minerais, onde foram disponibilizadas duas trincheiras e amostras de 8 testemunhos de sondagem. A amostragem limitou-se à extensão litológica do perfil laterítico, com a seleção de 44 amostras em intervalos médios de 1m, e que foram submetidas a uma rota de preparação e análise em laboratório. Em consonância com as demais ocorrências da região do Gurupi, os fosfatos de Sapucaia constituem um horizonte individualizado, de geometria predominantemente tabular, denominado simplesmente de horizonte de fosfatos de alumínio ou crosta aluminofosfática, que varia texturalmente de maciça a cavernosa, porosa a microporosa, que para o topo grada para uma crosta ferroalumino fosfática, tipo pele-de-onça, compacta a cavernosa, composta por nódulos de hematita e/ou goethita cimentados por fosfatos de alumínio, com características similares aos do horizonte de fosfatos subjacente. A crosta aluminofosfática, para a base do perfil, grada para um espesso horizonte argiloso caulinítico com níveis arenosos, que repousa sobre sedimentos heterolíticos intemperizados de granulação fina, aspecto argiloso, por vezes sericítico, intercalados por horizontes arenosos, e que não possuem correlação aparente com as demais rochas aflorantes da geologia na região. Aproximadamente 40% da superfície do morro é encoberta por colúvio composto por fragmentos mineralizados da crosta e por sedimentos arenosos da Formação Barreiras. Na crosta, os fosfatos de alumínio estão representados predominantemente pelo subgrupo da crandallita: i) série crandallita-goyazita (média de 57,3%); ii) woodhouseíta-svanbergita (média de 15,8%); e pela iii) wardita-millisita (média de 5,1%). Associados aos fosfatos encontram-se hematita, goethita, quartzo, caulinita, muscovita e anatásio, com volumes que variam segundo o horizonte laterítico correspondente. Como os minerais pesados em nível acessório a raro estão zircão, estaurolita, turmalina, anatásio, andalusita e silimanita. O horizonte de fosfatos, bem como a crosta ferroalumínio-fosfática, mostra-se claramente rica em P₂O₅, além de Fe₂O₃, CaO, Na₂O, SrO, SO₃, Th, Ta e em terras-raras leves como La e Ce em relação ao horizonte saprolítico. Os teores de SiO₂ são consideravelmente elevados, porém muito inferiores aqueles identificados no horizonte argiloso sotoposto. No perfil como um todo, observa-se uma correlação inversa entre SiO₂ e Al₂O₃; entre Al₂O₃ e Fe₂O₃, e positiva entre SiO₂ e Fe₂O₃, que ratificam a natureza laterítica do perfil. Diferente do que é esperado para lateritos bauxíticos, os teores de P₂O₅, CaO, Na₂O, SrO e SO₃ são fortemente elevados, concentrações consideradas típicas de depósitos de fosfatos de alumínio ricos em crandallita-goyazita e woodhouseítasvanbergita. A sucessão dos horizontes, sua composição mineralógica, e os padrões geoquímicos permitem correlacionar o presente depósito com os demais fosfatos de alumínio da região, mais especificamente Jandiá (Pará) e Trauíra (Maranhão), bem como outros situados além do território brasileiro, indicando portanto, que os fosfatos de alumínio de Sapucaia são produtos da gênese de um perfil laterítico maturo e completo, cuja rocha fonte pode estar relacionada a rochas mineralizadas em fósforo, tais como as observadas na Formação Pimenteiras, parcialmente aflorante na borda da Bacia do Parnaíba. Possivelmente, o atual corpo de minério integrou a paleocosta do mar de Pirabas, uma vez que furos de sondagem às proximidades do corpo deixaram claro a relação de contato lateral entre estas unidades.

Effects of Dextrose and Lipopolysaccharide on the Corrosion Behavior of a Ti-6Al-4V Alloy with a Smooth Surface or Treated with Double-Acid-Etching

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Usual interstitial pneumonia and smoking-related interstitial fibrosis display epithelial to mesenchymal transition in fibroblastic foci

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Does water level affect benthic macro-invertebrates of a marginal lake in a tropical river-reservoir transition zone?

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Correlation between i.r. spectra and thermal decomposition of cobalt(II), nickel(II), copper(II) and mercury(II) complexes with piperidinedithiocarbamate and pyrrolidinedithiocarbamate

The thermal decomposition of pyrrolidinedithiocarbamate and piperidinedithiocarbamate complexes of CoII, NiII, CuII and HgII have been studied by thermogravimetry and differential scanning calorimetry. The decomposition intermediates and final products were identified by their X-ray diffraction patterns. The i.r. spectra are discussed in terms of the thermal decomposition pathways.

Quantum critical scaling at a Bose-glass/superfluid transition: Theory and experiment for a model quantum magnet

In this paper we investigate the quantum phase transition from magnetic Bose Glass to magnetic Bose-Einstein condensation induced by amagnetic field in NiCl2 center dot 4SC(NH2)(2) (dichloro-tetrakis-thiourea-nickel, or DTN), doped with Br (Br-DTN) or site diluted. Quantum Monte Carlo simulations for the quantum phase transition of the model Hamiltonian for Br-DTN, as well as for site-diluted DTN, are consistent with conventional scaling at the quantum critical point and with a critical exponent z verifying the prediction z = d; moreover the correlation length exponent is found to be nu = 0.75(10), and the order parameter exponent to be beta = 0.95(10). We investigate the low-temperature thermodynamics at the quantum critical field of Br-DTN both numerically and experimentally, and extract the power-law behavior of the magnetization and of the specific heat. Our results for the exponents of the power laws, as well as previous results for the scaling of the critical temperature to magnetic ordering with the applied field, are incompatible with the conventional crossover-scaling Ansatz proposed by Fisher et al. [Phys. Rev. B 40, 546 (1989)]. However they can all be reconciled within a phenomenological Ansatz in the presence of a dangerously irrelevant operator.

Extracellular matrix in airway smooth muscle is associated with dynamics of airway function in asthma

Background: Altered deposition of extracellular matrix (ECM) in the airway smooth muscle (ASM) layer as observed in asthma may influence ASM mechanical properties. We hypothesized that ECM in ASM is associated with airway function in asthma. First, we investigated the difference in ECM expression in ASM between asthma and controls. Second, we examined whether ECM expression is associated with bronchoconstriction and bronchodilation in vivo. Methods: Our cross-sectional study comprised 19 atopic mild asthma patients, 15 atopic and 12 nonatopic healthy subjects. Spirometry, methacholine responsiveness, deep-breath-induced bronchodilation (Delta R-rs) and bronchoscopy with endobronchial biopsies were performed. Positive staining of elastin, collagen I, III and IV, decorin, versican, fibronectin, laminin and tenascin in ASM was quantified as fractional area and mean density. Data were analysed using Pearson's or Spearman's correlation coefficient. Results: Extracellular matrix expression in ASM was not different between asthma and controls. In asthmatics, fractional area and mean density of collagen I and III were correlated with methacholine dose-response slope and DRrs, respectively (r = 0.71, P < 0.01; r = 0.60, P = 0.02). Furthermore, ASM collagen III and laminin in asthma were correlated with FEV1 reversibility (r = -0.65, P = 0.01; r = -0.54, P = 0.04). Conclusion: In asthma, ECM in ASM is related to the dynamics of airway function in the absence of differences in ECM expression between asthma and controls. This indicates that the ASM layer in its full composition is a major structural component in determining variable airways obstruction in asthma.

URANS calculations for smooth circular cylinder flow in a wide range of Reynolds Numbers: solution verification and validation

The flow around circular smooth fixed cylinder in a large range of Reynolds numbers is considered in this paper. In order to investigate this canonical case, we perform CFD calculations and apply verification & validation (V&V) procedures to draw conclusions regarding numerical error and, afterwards, assess the modeling errors and capabilities of this (U)RANS method to solve the problem. Eight Reynolds numbers between Re = 10 and Re 5 x 10(5) will be presented with, at least, four geometrically similar grids and five discretization in time for each case (when unsteady), together with strict control of iterative and round-off errors, allowing a consistent verification analysis with uncertainty estimation. Two-dimensional RANS, steady or unsteady, laminar or turbulent calculations are performed. The original 1994 k - omega SST turbulence model by Menter is used to model turbulence. The validation procedure is performed by comparing the numerical results with an extensive set of experimental results compiled from the literature. [DOI: 10.1115/1.4007571]