Phase behavior of synthetic amphiphile vesicles investigated by calorimetry and fluorescence methods

The understanding of biological membranes may be improved by investigating physical properties of vesicles from natural or synthetic amphiphiles. The application of vesicles as mimetic agents depends on the knowledgment of their structure and properties. Vesicles having different curvature and size may be obtained using different preparation protocols. We have used differential scanning calorimetry (DSC) and steady-state fluorescence to investigate the gel to liquid-crystal phase transition of vesicles prepared by sonication (SUV) and non-sonication (GUV) of the synthetic dioctadecyldimethylammonium bromide (DODAB) in aqueous solution. DSC thermograms for a non-sonicated dispersion show a well-defined pre- and main transition corresponding to two narrow peaks at 36 and 45°C in the first upscan, while in a second upscan, only the main peak was observed. The sharpness of the peaks indicate a cooperative phase behavior for GUV. For a sonicated DODAB dispersion, the first upscan shows a third peak at 40.3°C, whereas for the second upscan the peaks are not well-defined, indicating a less cooperative phase behavior. Alternatively, the fluorescence quantum yield (Φ f) and the anisotropy (r) of trans, trans, trans-1-[4-(3-carboxypropyl)-phenyl]-6-[4-butylphenyl]-1,3,5-hexatriene (4H4A) and the ratio I 1/I 3 of the first to the third vibronic peaks of the pyrene emission spectrum as function of temperature are used as well to describe the phase behavior of DODAB sonicated and non-sonicated dispersions. It is in good agreement with the DSC results that the cooperativity of the thermotropic process is diminished under sonication of the DODAB dispersion, meaning that sonication changes from homogeneous to heterogeneous populations of the amphiphile aggregates. The pre- and main transitions obtained from these techniques are in fairly good accord with results from the literature.

Droplet formation in cold asymmetric nuclear matter in the quark-meson-coupling model

The quark-meson-coupling model is used to study droplet formation from the liquid-gas phase transition in cold asymmetric nuclear matter. The critical density and proton fraction for the phase transition are determined in the mean field approximation. Droplet properties are calculated in the Thomas-Fermi approximation. The electromagnetic field is explicitly included and its effects on droplet properties are studied. The results are compared with the ones obtained with the NL1 parametrization of the non-linear Walecka model. © 2000 Elsevier Science B.V.

Raman scattering study of the PbZr1-xTixO3 system: Rhombohedral-monoclinic-tetragonal phase transitions

In this paper we present a Raman-scattering study of the phase transitions in the PbZr1-xTixO3 systems around the morphotropic phase boundary over a wide temperature range. The boundary between rhombohedral and monoclinic phases was found to be a quasivertical line between x = 0.46 and x = 0.47. We also studied the monoclinic-tetragonal phase boundary and our spectroscopic results agree very well with those reported by using x-ray diffraction.

Metal-insulator transition in Nd1-xEuxNiO 3 compounds

Polycrystalline Nd1-xEuxNiO3 (0≤x≤0.5) compounds were synthesized in order to investigate the character of the metal-insulator (MI) phase transition in this series. Samples were prepared through the sol-gel route and subjected to heat treatments at ∼1000 °C under oxygen pressures as high as 80bar. X-ray diffraction (XRD) and neutron powder diffraction (NPD), electrical resistivity ρ(T), and magnetization M(T) measurements were performed on these compounds. The NPD and XRD results indicated that the samples crystallize in an orthorhombic distorted perovskite structure, space group Pbnm. The analysis of the structural parameters revealed a sudden and small expansion of ∼0.2% of the unit cell volume when electronic localization occurs. This expansion was attributed to a small increase of ∼0.003 of the average Ni-O distance and a simultaneous decrease of ∼-0.5° of the Ni-O-Ni superexchange angle. The ρ(T) measurements revealed a MI transition occurring at temperatures ranging from TMI∼193 to 336K for samples with x ≤ 0 and 0.50, respectively. These measurements also show a large thermal hysteresis in NdNiO3 during heating and cooling processes, suggesting a first-order character of the phase transition at TMI. The width of this thermal hysteresis was found to decrease appreciably for the sample Nd 0.7Eu0.3NiO3. The results indicate that cation disorder associated with increasing substitution of Nd by Eu is responsible for changing the first-order character of the transition in NdNiO3. © 2006 IOP Publishing Ltd.

Dielectric tunability in (1-x)[Pb(Mg 1/3Nb 2/3)O 3]-xPbTiO 3 ceramics for tunable devices application

The dielectric properties of the 0.65[Pb(Mg 1/3Nb 2/3)O 3]-0.35PbTiO 3 ferroelectric ceramic composition were investigated viewing the capability to be used for tunable microwave applications. The dielectric response has been studied for three selected temperatures (300 K, 370 K and 400 K), below the paraelectric- ferroelectric phase transition temperature, as a function of the applied 'bias' electric field. The obtained dielectric tunability was found to be around 60 %, under an electric field of 19 kV/cm, which makes the studied ceramic composition an excellent candidate for application in the electro-electronic industry, as tunable devices. © 2010 IEEE.

Effect of air-particle abrasion protocols on the biaxial flexural strength, surface characteristics and phase transformation of zirconia after cyclic loading

This study evaluated the effect of air-particle abrasion protocols on the biaxial flexural strength, surface characteristics and phase transformation of zirconia after cyclic loading. Disc-shaped zirconia specimens (Ø: 15mm, thickness: 1.2mm) (N=32) were submitted to one of the air-particle abrasion protocols (n=8 per group): (a) 50μm Al2O3 particles, (b) 110μm Al2O3 particles coated with silica (Rocatec Plus), (c) 30μm Al2O3 particles coated with silica (CoJet Sand) for 20s at 2.8bar pressure. Control group received no air-abrasion. All specimens were initially cyclic loaded (×20,000, 50N, 1Hz) in water at 37°C and then subjected to biaxial flexural strength testing where the conditioned surface was under tension. Zirconia surfaces were characterized and roughness was measured with 3D surface profilometer. Phase transformation from tetragonal to monoclinic was determined by Raman spectroscopy. The relative amount of transformed monoclinic zirconia (FM) and transformed zone depth (TZD) were measured using XRD. The data (MPa) were analyzed using ANOVA, Tukey's tests and Weibull modulus (m) were calculated for each group (95% CI). The biaxial flexural strength (MPa) of CoJet treated group (1266.3±158A) was not significantly different than that of Rocatec Plus group (1179±216.4A,B) but was significantly higher than the other groups (Control: 942.3±74.6C; 50μm Al2O3: 915.2±185.7B,C). Weibull modulus was higher for control (m=13.79) than those of other groups (m=4.95, m=5.64, m=9.13 for group a, b and c, respectively). Surface roughness (Ra) was the highest with 50μm Al2O3 (0.261μm) than those of other groups (0.15-0.195μm). After all air-abrasion protocols, FM increased (15.02%-19.25%) compared to control group (11.12%). TZD also showed increase after air-abrasion protocols (0.83-1.07μm) compared to control group (0.59μm). Air-abrasion protocols increased the roughness and monoclinic phase but in turn abrasion with 30μm Al2O3 particles coated with silica has increased the biaxial flexural strength of the tested zirconia. © 2013 Elsevier Ltd.

Charge-ordering transition in (TMTTF)2X explored via dilatometry

Charge-ordering phenomena have been highly topical over the past few years. A phase transition towards a charge-ordered state has been observed experimentally in several classes of materials. Among them, many studies have been devoted to the family of quasi-one-dimensional organic charge-transfer salts (TMTTF)2X, where (TMTTF) stands for tetramethyltetrathiafulvalene and X for a monovalent anion (X = PF6, AsF6 and SbF6). However, the relationship between the electron localization phenomena and the role of the lattice distortion in stabilizing the charge-ordering pattern is poorly documented in the literature. Here we present a brief overview of selected literature results, with emphasis placed on recent thermal expansion experiments probing the charge-ordering transition of these salts. © 2013 IOP Publishing Ltd.

Demodulação de sinais interferométricos de saída de sensor eletro-óptico de tensões elevadas utilizando processador digital de sinais

Pós-graduação em Engenharia Elétrica - FEIS

Estudo da formação de domínios em bicamadas lipídicas induzidos por peptídeos antimicrobianos

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Síntese e propriedades físicas de cerâmicas ferroelétricas de PMN-PT

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Influência dos defeitos cristalinos nas propriedades dielétricas e não-ôhmicas do 'CA' 'CU IND.3' 'TI IND.4' 'O IND.12'(CCTO)

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Medidas de espectroscopia Raman em cristais KDP e Nanotubos de Carbono: implementação da técnica

Atualmente, os físicos vêm desenvolvendo novas técnicas de caracterização de materiais, principalmente os novos materiais que os cientistas (de todas as áreas) estão produzindo a partir de outros já existentes como vidros, cerâmicas, polímeros, materiais semicondutores e supercondutores, materiais magnéticos, dentre outros. Seguindo esta linha, o Grupo de Física de Materiais da Amazônia vem adquirindo novas técnicas para caracterização de materiais e este trabalho marca o início da incorporação de mais uma técnica de caracterização junto ao laboratório de física da UFPA, a Espectroscopia Raman. Neste trabalho, utilizamos como amostras para realizar e testar a técnica implantada, cristais KH2PO4 (KDP) e nanotubos de carbono de parede simples (SWNT). O KDP foi escolhido devido ao fato de ter os espectros Raman muito conhecidos e ser um material de simples produção. O KDP puro ou dopado continua sendo alvo de pesquisa (teórica e/ou experimental) atual, principalmente por apresentar uma transição de fase ferroelétrica e ser um material que tem muitas aplicações nas indústrias que utilizam tecnologia de lasers, sensores, gerador de segundo e terceiro harmônico. Já os nanotubos de carbono também foram utilizados como amostras por ser um material de grande interesse científico, tecnológico e de grande aplicação no mundo moderno, pois podem ser empregados em nanotecnologia na produção de transistores e diodos, além disso, podem ser incorporados a certos materiais aumentando, assim, a resistência mecânica dos mesmos.Para as amostras de KDP foram realizadas medidas em temperatura ambiente, pressão uniaxial e temperatura. Nas medidas com a temperatura conseguimos observar o inicio da decomposição e de uma possível transição de fase em alta temperatura no KDP. As medidas com pressão uniaxial mostram que embora não se observe uma transição de fase bem definida é possível se identificar alteração que podem indicar o inicio de uma quebra de simetria devido aos efeitos de pressão. Nas amostras de nanotubos (nanotubos de paredes simples-SWNT) foram realizadas medidas de Raman em temperatura ambiente. Nessas medidas identificamos as bandas D e G bastante conhecidas as quais são reportadas em quase todos os artigos sobre esse tema. O mais importante foi a implantação da nova técnica que é uma técnica forte que pode ser aplicada em diferentes campos do conhecimento científico fortalecendo o Grupo de Física de Materiais da Amazônia.

Condutividade elétrica complexa de rochas

Foram realizadas medidas em laboratório da condutividade elétrica complexa de 28 amostras de testemunhos de sondagem de três furos da área MM1-Alvo 1, Distrito dos Carajás, com o objetivo de auxiliar na interpretação de dados geofísicos de campo, obtidos com os métodos polarização induzida/resistividade e eletromagnético/AFMAG, aplicados na área. As medidas foram tomadas no intervalo de frequências de 10^-3Hz a 10⁴Hz, medindo-se a amplitude e a fase da condutância. O método empregado foi o de medida direta de impedância, utilizando-se um osciloscópio com memória, um gerador de sinais e dois pré-amplificadores diferenciais com alta impedância de entrada. O sistema de eletrodos escolhido para realizar as medidas foi o de 2 eletrodos de platina-platinizada em virtude de sua resposta de frequência ser plana no intervalo utilizado. Todas as medidas foram realizadas à temperatura constante de 24°C ± 1°C. Para interpretar as medidas de condutividade foi realizado estudo petrográfico das amostras, utilizando-se lâminas delgadas, seções polidas e difração de Raios-X. Foi determinado o teor de cobre, sob a forma de sulfeto, nas amostras utilizando-se o método de absorção atômica. Os resultados petrográficos permitiram classificar as amostras em cinco grupos distintos: granito, biotita-xisto, anfibolito, anfibólio-xisto e quartzito ferruginoso-formação ferrífera. O teor de cobre foi variável nos cinco grupos, havendo teores desde 50ppm até 6000ppm. Nas medidas de condutividade observou-se que, dentre os cinco grupos, as amostras da formação ferrífera apresentaram as maiores variações com a frequência. As amostras de granito tiveram espectro mais plano que as dos xistos e anfibolito. A conclusão a que se chegou é que as anomalias eletromagnéticas e de polarização induzida/resistividade observadas no campo próximo aos três furos (F₁, F₂, F₃) são devidas principalmgnte a formação ferrífera magnetitica, a secundariamente à mineralização de baixo teor de calcopirita associada.

Modelos mecânicos para o estudo da dinâmica do DNA

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Structural refinement, optical and electrical properties of [Ba1-x Sm-2x/3](Zr0.05Ti0.95)O-3 ceramics

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)