Cracking Of Petroleum Residues By Reactive Molecular Distillation

It is known that the Brazilian oils are more heavy - super heavy - viscous, its operation is difficult, especially its production, including all stages - elevation, runoff and primary processing - in addition to their transfer, and refining itself. Studies indicate the existence of oil fields as heavy lifting and that the simple flow of the base of the pit to the surface seems impossible at first sight, especially in off-shore fields, compromising both technically and economically a project to produce a new field. Therefore, efforts are needed to develop alternatives aimed at reducing the API gravity, viscosity and sulfur content of extra-heavy oil, adding a higher commercial value for these oils. This work aims to study, propose and develop enhanced hybrid process that transforms the extra-heavy oil, or part thereof, in lighter crude oil to generate a mixture: lower sulfur content, lower density, lower viscosity, lower content of volatile (aromatics and asphaltenes), greater resistance to the processes of purification. The process studied is the Reactive molecular distillation with the addition of tetralin that suffer from high temperature cracking of molecules, providing protons that help the breakdown of asphaltenes and residues will suffer as a consequence physicochemical changes, such as those mentioned above. This way you can improve the problems associated with the deposition of asphaltenes at high temperatures. The conversion of light with immediate reduction of API gravity and sulfur content promoted a better use of extra-heavy oil and the DMR is a product of high-value oil and very interesting for the oil industry and the environment. The experimental work proposed in this study was conducted to cracking and separation of fractions and petroleum. The evaluation and characterization of the cracking results were obtained after analysis of properties such as density, viscosity, sulfur content, molar mass and mass balance of the currents. © 2012 Published by Elsevier Ltd.42329334Erciyes, A.T., Ishikawa, H., Inuzuka, M., Hiraoka, S., Mori, H.E., Yamada, I., Vaporization of binary liquid mixtures from surface at reduced pressure (1987) Chem Eng Symp Series, 1, pp. A359-A371Moraes, E.B., Batistella, C.B., Torres Alvarez, M.E., Maciel Filho, R., Wolf Maciel, M.R., Evaluation of tocopherol recovery through simulation of molecular distillation process (2004) Appl Biochem Biotech, 114, pp. 689-711Noeres, C., Kenig, E.Y., Górak, A., Modelling of reactive separation processes (2003) Reactive Absorption and Reactive Distillation. Chem Eng Process, 42, pp. 157-178Duarte, F.A., Mello, P.A., Bizzi, C.A., Nunes, M.A.G., Moreira, E.M., Alencar, M.S., Motta, H.N., Flores, E.M.M., Sulfur removal from hydrotreated petroleum fractions using ultrasound-assisted oxidative desulfurization process (2001) Fuel, 90, pp. 2158-216

How does the substrate affect the Raman and excited state spectra of a carbon nanotube?

We study the optical properties of a single, semiconducting single-walled carbon nanotube (CNT) that is partially suspended across a trench and partially supported by a SiO2-substrate. By tuning the laser excitation energy across the E33 excitonic resonance of the suspended CNT segment, the scattering intensities of the principal Raman transitions, the radial breathing mode (RBM), the G-mode and the D-mode show strong resonance enhancement of up to three orders of magnitude. In the supported part of the CNT, despite a loss of Raman scattering intensity of up to two orders of magnitude, we recover the E33 excitonic resonance suffering a substrate-induced red shift of 50 meV. The peak intensity ratio between G-band and D-band is highly sensitive to the presence of the substrate and varies by one order of magnitude, demonstrating the much higher defect density in the supported CNT segments. By comparing the E33 resonance spectra measured by Raman excitation spectroscopy and photoluminescence (PL) excitation spectroscopy in the suspended CNT segment, we observe that the peak energy in the PL excitation spectrum is red-shifted by 40 meV. This shift is associated with the energy difference between the localized exciton dominating the PL excitation spectrum and the free exciton giving rise to the Raman excitation spectrum. High-resolution Raman spectra reveal substrate-induced symmetry breaking, as evidenced by the appearance of additional peaks in the strongly broadened Raman G band. Laser-induced line shifts of RBM and G band measured on the suspended CNT segment are both linear as a function of the laser excitation power. Stokes/anti-Stokes measurements, however, reveal an increase of the G phonon population while the RBM phonon population is rather independent of the laser excitation power.Comment: Revised manuscript, 20 pages, 8 figure

Análise retrospectiva do resultado do tratamento com iodo radioativo em 120 pacientes tirotóxicos por doença de Basedow-graves

We studied retrospectively the outcome of radioactive iodine therapy (RAI) in 120 thyrotoxic patients with Graves' disease (96 F/ 24 M) who were primarily treated with anti-thyroid drugs (ATD). The decision to use RAI was due either to relapse after ATD-induced remission, lack of compliance on ATD, goiter larger than 60g, old age or association with severe diseases. ATD were discontinued one week before RAI administration, calculated by the formula: glandular volume (g) vs. effective radiation (80 mCi/g of tissue) divided by 24h thyroid uptake (%). We reexamined the patients for 48 months after RAI. Medians of age, goiter size and 24h thyroid uptake were 34y (17-69), 54.5g (20-210) and 73% (21-99), respectively. After RAI, patients became gradually hypothyroid on a rate of 15%/ 6mo until the first 18mo, followed by a rate of 2-5%/ 6mo until the end of 48mo. The number of patients in thyrotoxicosis decreased continuously, being 52.2% 6mo after RAI, 25% after 18mo and 6.7% after 48mo; at the end of the study 8 patients were still thyrotoxic. The total of patients without thyrotoxicosis at the end of observation, that is, the sum of those in euthyroidism and hypothyroidism on T4 therapy (cure of thyrotoxicosis) reached 46.8% in 6mo, 63.3% in 12mo, 81.7% in 24mo, 87.5% in 36mo and 93.3% in 48mo. Transient hypothyroidism, that is, elevation of TSH higher than 4.5 mU/L until 12mo after RAI, followed by normalization of TSH was found in 7.5% of patients. The following correlations were found in this study: a) initial T3 values and absence of cure of thyroxicosis (p=0.2); b) total RAI doses in relation to time for cure of thyrotoxicosis (p=0.01); c) dose of 131l/thyroid volume in relation to time for cure of thyrotoxicosis (p=0.02). Adverse effects included exarcebation of thyrotoxicosis in 3 patients and pain in the anterior cervical area in one, all reversible and of short duration. Two patients became pregnant after RAI but both gestations and their outcomes were normal.Estudamos retrospectivamente 120 pacientes (96 F/ 24 M) portadores de tirotoxicose por doença de Basedow-Graves submetidos à terapia com iodo radioativo (131I), que receberam inicialmente, para compensação da moléstia, drogas anti-tiroidianas (DAT). A indicação terapêutica posterior de radioiodo deveu-se a uma das seguintes condições clínicas: recidiva após compensação com DAT, falta de compensação devida à baixa aderência às DAT, bócios maiores que 60g, idade avançada ou doença grave associada. As DAT foram suspensas uma semana antes da administração da dose de 131I, calculada pela fórmula: volume glandular (em g) X radiação efetiva (80 mCi/g de tecido) ¸ captação tiroideana de 24hs. Reavaliamos os pacientes por até 48 meses após a radioiodoterapia. As medianas iniciais de idade, bócio e captação tiroideana de 24hs dos 120 pacientes foram, respectivamente, 34 anos (17-69), 54,5g (20-210) e 73% (21-99). A evolução para hipotiroidismo foi gradual, com 15% dos pacientes a cada 6m até o 18º mês, seguidos de 2 a 5% dos pacientes a cada 6m até o 48º mês. O número de pacientes em tirotoxicose decresceu continuamente, representando 52,2% do total inicial após 6m, 25% após 18m e 6,7% após 48m. Ao final, 8 pacientes continuaram em tirotoxicose. O número de pacientes sem tirotoxicose após o tratamento com 131I, ou seja a soma daqueles em eutiroidismo com aqueles em hipotiroidismo com reposição com T4 (denominada por nós de cura da tirotoxicose), alcançou 46,8% dos pacientes em óm, 63,3% em 12m, 81,7% em 24m, 87,5% em 36m e 93,3% em 48m. O número de pacientes que apresentaram hipotiroidismo transitório, ou seja, elevação do TSH acima de 4,5 mU/L até 12m após a dose de 131I, com normalização posterior, foi 7,5%. Correlacionaram-se positivamente: a) valores iniciais de T3 e ausência de evolução para a cura da tirotoxicose (p=0,02); b) doses totais de 131I administradas, únicas ou múltiplas, em relação ao tempo de cura da tirotoxicose (p=0,01); c) dose de 131 l/volume glandular em relação ao tempo de cura da tirotoxicose (p=0,02). Os efeitos adversos incluíram exacerbação da tirotoxicose em 3 pacientes e dor na região cervical anterior em um, com reversão dos quadros em todos. Outras duas pacientes engravidaram após o dose terapêutica de 131I para a tirotoxicose e tiveram gestações sem intercorrência e recém-nascidos normais.Universidade Federal de São Paulo (UNIFESP) Escola Paulista de Medicina Departamento de MedicinaUNIFESP, EPM, Depto. de MedicinaSciEL

Limits on anomalous trilinear gauge boson couplings from WW, WZ and Wgamma production in pp-bar collisions at sqrt{s}=1.96 TeV

We present final searches of the anomalous gammaWW and ZWW trilinear gauge boson couplings from WW and WZ production using lepton plus dijet final states and a combination with results from Wgamma, WW, and WZ production with leptonic final states. The analyzed data correspond to up to 8.6/fb of integrated luminosity collected by the D0 detector in pp-bar collisions at sqrt{s}=1.96 TeV. We set the most stringent limits at a hadron collider to date assuming two different relations between the anomalous coupling parameters Delta\kappa_\gamma, lambda, and Delta g_1^Z for a cutoff energy scale Lambda=2 TeV. The combined 68% C.L. limits are -0.057<Delta\kappa_\gamma<0.154, -0.015<lambda<0.028, and -0.008<Delta g_1^Z<0.054 for the LEP parameterization, and -0.007<Delta\kappa<0.081 and -0.017<lambda<0.028 for the equal couplings parameterization. We also present the most stringent limits of the W boson magnetic dipole and electric quadrupole moments.Comment: 10 pages, 5 figures, submitted to PL

Measurement of Z/gamma*+jet+X angular distributions in ppbar collisions at sqrt{s}=1.96 TeV

We present the first measurements at a hadron collider of differential cross sections for Z+jet+X production in delta phi(Z, jet), |delta y(Z, jet)| and |y_boost(Z, jet)|. Vector boson production in association with jets is an excellent probe of QCD and constitutes the main background to many small cross section processes, such as associated Higgs production. These measurements are crucial tests of the predictions of perturbative QCD and current event generators, which have varied success in describing the data. Using these measurements as inputs in tuning event generators will increase the experimental sensitivity to rare signals.Comment: Published in Physics Letters B 682 (2010), pp. 370-380. 15 pages, 6 figure

Search for the standard model Higgs boson in tau final states

We present a search for the standard model Higgs boson using hadronically decaying tau leptons, in 1 inverse femtobarn of data collected with the D0 detector at the Fermilab Tevatron ppbar collider. We select two final states: tau plus missing transverse energy and b jets, and tau+ tau- plus jets. These final states are sensitive to a combination of associated W/Z boson plus Higgs boson, vector boson fusion and gluon-gluon fusion production processes. The observed ratio of the combined limit on the Higgs production cross section at the 95% C.L. to the standard model expectation is 29 for a Higgs boson mass of 115 GeV.Comment: publication versio

Search for W' bosons decaying to an electron and a neutrino with the D0 detector

This Letter describes the search for a new heavy charged gauge boson W' decaying into an electron and a neutrino. The data were collected with the D0 detector at the Fermilab Tevatron proton-antiproton Collider at a center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity of about 1 inverse femtobarn. Lacking any significant excess in the data in comparison with known processes, an upper limit is set on the production cross section times branching fraction, and a W' boson with mass below 1.00 TeV can be excluded at the 95% C.L., assuming standard-model-like couplings to fermions. This result significantly improves upon previous limits, and is the most stringent to date.Comment: submitted to Phys. Rev. Let

Search for a scalar or vector particle decaying into Zgamma in ppbar collisions at sqrt(s) = 1.96 TeV

We present a search for a narrow scalar or vector resonance decaying into Zgamma with a subsequent Z decay into a pair of electrons or muons. The data for this search were collected with the D0 detector at the Fermilab Tevatron ppbar collider at a center of mass energy sqrt(s) = 1.96 TeV. Using 1.1 (1.0) fb-1 of data, we observe 49 (50) candidate events in the electron (muon) channel, in good agreement with the standard model prediction. From the combination of both channels, we derive 95% C.L. upper limits on the cross section times branching fraction (sigma x B) into Zgamma. These limits range from 0.19 (0.20) pb for a scalar (vector) resonance mass of 600 GeV/c^2 to 2.5 (3.1) pb for a mass of 140 GeV/c^2.Comment: Published by Phys. Lett.

Search for Higgs bosons decaying to tautau pairs in ppbar collisions at sqrt(s) = 1.96 TeV

We present a search for the production of neutral Higgs bosons decaying into tautau pairs in ppbar collisions at a center-of-mass energy of 1.96 TeV. The data, corresponding to an integrated luminosity of 5.4 fb-1, were collected by the D0 experiment at the Fermilab Tevatron Collider. We set upper limits at the 95% C.L. on the product of production cross section and branching ratio for a scalar resonance decaying into tautau pairs, and we then interpret these limits as limits on the production of Higgs bosons in the minimal supersymmetric standard model (MSSM) and as constraints in the MSSM parameter space.Comment: 7 pages, 5 figures, submitted to PL