964 resultados para Air Pollutants, Occupational
Resumo:
<p>An economic air pollution control model, which determines the least cost of reaching various air quality levels, is formulated. The model takes the form of a general, nonlinear, mathematical programming problem. Primary contaminant emission levels are the independent variables. The objective function is the cost of attaining various emission levels and is to be minimized subject to constraints that given air quality levels be attained.</p> <p>The model is applied to a simplified statement of the photochemical smog problem in Los Angeles County in 1975 with emissions specified by a two-dimensional vector, total reactive hydrocarbon, (RHC), and nitrogen oxide, (NO<sub>x</sub>), emissions. Air quality, also two-dimensional, is measured by the expected number of days per year that nitrogen dioxide, (NO<sub>2</sub>), and mid-day ozone, (O<sub>3</sub>), exceed standards in Central Los Angeles.</p> <p>The minimum cost of reaching various emission levels is found by a linear programming model. The base or "uncontrolled" emission levels are those that will exist in 1975 with the present new car control program and with the degree of stationary source control existing in 1971. Controls, basically "add-on devices", are considered here for used cars, aircraft, and existing stationary sources. It is found that with these added controls, Los Angeles County emission levels [(1300 tons/day RHC, 1000 tons /day NO<sub>x</sub>) in 1969] and [(670 tons/day RHC, 790 tons/day NO<sub>x</sub>) at the base 1975 level], can be reduced to 260 tons/day RHC (minimum RHC program) and 460 tons/day NO<sub>x</sub> (minimum NO<sub>x</sub> program).</p> <p>"Phenomenological" or statistical air quality models provide the relationship between air quality and emissions. These models estimate the relationship by using atmospheric monitoring data taken at one (yearly) emission level and by using certain simple physical assumptions, (e. g., that emissions are reduced proportionately at all points in space and time). For NO<sub>2</sub>, (concentrations assumed proportional to NO<sub>x</sub> emissions), it is found that standard violations in Central Los Angeles, (55 in 1969), can be reduced to 25, 5, and 0 days per year by controlling emissions to 800, 550, and 300 tons /day, respectively. A probabilistic model reveals that RHC control is much more effective than NO<sub>x</sub> control in reducing Central Los Angeles ozone. The 150 days per year ozone violations in 1969 can be reduced to 75, 30, 10, and 0 days per year by abating RHC emissions to 700, 450, 300, and 150 tons/day, respectively, (at the 1969 NO<sub>x</sub> emission level).</p> <p>The control cost-emission level and air quality-emission level relationships are combined in a graphical solution of the complete model to find the cost of various air quality levels. Best possible air quality levels with the controls considered here are 8 O<sub>3</sub> and 10 NO<sub>2</sub> violations per year (minimum ozone program) or 25 O<sub>3</sub> and 3 NO<sub>2</sub> violations per year (minimum NO<sub>2</sub> program) with an annualized cost of $230,000,000 (above the estimated $150,000,000 per year for the new car control program for Los Angeles County motor vehicles in 1975).</p>
Resumo:
<p>Part I</p> <p>Regression analyses are performed on in vivo hemodialysis data for the transfer of creatinine, urea, uric acid and inorganic phosphate to determine the effects of variations in certain parameters on the efficiency of dialysis with a Kiil dialyzer. In calculating the mass transfer rates across the membrane, the effects of cell-plasma mass transfer kinetics are considered. The concept of the effective permeability coefficient for the red cell membrane is introduced to account for these effects. A discussion of the consequences of neglecting cell-plasma kinetics, as has been done to date in the literature, is presented. </p> <p>A physical model for the Kiil dialyzer is presented in order to calculate the available membrane area for mass transfer, the linear blood and dialysate velocities, and other variables. The equations used to determine the independent variables of the regression analyses are presented. The potential dependent variables in the analyses are discussed. </p> <p>Regression analyses were carried out considering overall mass-transfer coefficients, dialysances, relative dialysances, and relative permeabilities for each substance as the dependent variables. The independent variables were linear blood velocity, linear dialysate velocity, the pressure difference across the membrane, the elapsed time of dialysis, the blood hematocrit, and the arterial plasma concentrations of each substance transferred. The resulting correlations are tabulated, presented graphically, and discussed. The implications of these correlations are discussed from the viewpoint of a research investigator and from the viewpoint of patient treatment. </p> <p>Recommendations for further experimental work are presented. </p> <p>Part II</p> <p>The interfacial structure of concurrent air-water flow in a two-inch diameter horizontal tube in the wavy flow regime has been measured using resistance wave gages. The median water depth, r.m.s. wave height, wave frequency, extrema frequency, and wave velocity have been measured as functions of air and water flow rates. Reynolds numbers, Froude numbers, Weber numbers, and bulk velocities for each phase may be calculated from these measurements. No theory for wave formation and propagation available in the literature was sufficient to describe these results. </p> <p>The water surface level distribution generally is not adequately represented as a stationary Gaussian process. Five types of deviation from the Gaussian process function were noted in this work. The presence of the tube walls and the relatively large interfacial shear stresses precludes the use of simple statistical analyses to describe the interfacial structure. A detailed study of the behavior of individual fluid elements near the interface may be necessary to describe adequately wavy two-phase flow in systems similar to the one used in this work. </p>
Resumo:
<p>This study proposes a wastewater electrolysis cell (WEC) for on-site treatment of human waste coupled with decentralized molecular H<sub>2</sub> production. The core of the WEC includes mixed metal oxides anodes functionalized with bismuth doped TiO<sub>2</sub> (BiO<sub>x</sub>/TiO<sub>2</sub>). The BiO<sub>x</sub>/TiO<sub>2</sub> anode shows reliable electro-catalytic activity to oxidize Cl- to reactive chlorine species (RCS), which degrades environmental pollutants including chemical oxygen demand (COD), protein, NH4<sup>+</sup>, urea, and total coliforms. The WEC experiments for treatment of various kinds of synthetic and real wastewater demonstrate sufficient water quality of effluent for reuse for toilet flushing and environmental purposes. Cathodic reduction of water and proton on stainless steel cathodes produced molecular H2 with moderate levels of current and energy efficiency. This thesis presents a comprehensive environmental analysis together with kinetic models to provide an in-depth understanding of reaction pathways mediated by the RCS and the effects of key operating parameters. The latter part of this thesis is dedicated to bilayer hetero-junction anodes which show enhanced generation efficiency of RCS and long-term stability.</p> <p>Chapter 2 describes the reaction pathway and kinetics of urea degradation mediated by electrochemically generated RCS. The urea oxidation involves chloramines and chlorinated urea as reaction intermediates, for which the mass/charge balance analysis reveals that N<sub>2</sub> and CO<sub>2</sub> are the primary products. Chapter 3 investigates direct-current and photovoltaic powered WEC for domestic wastewater treatment, while Chapter 4 demonstrates the feasibility of the WEC to treat model septic tank effluents. The results in Chapter 2 and 3 corroborate the active roles of chlorine radicals (Cl•/Cl<sub>2</sub><sup>-</sup>•) based on iR-compensated anodic potential (thermodynamic basis) and enhanced pseudo-first-order rate constants (kinetic basis). The effects of operating parameters (anodic potential and [Cl<sup>-</sup>] in Chapter 3; influent dilution and anaerobic pretreatment in Chapter 4) on the rate and current/energy efficiency of pollutants degradation and H<sub>2</sub> production are thoroughly discussed based on robust kinetic models. Chapter 5 reports the generation of RCS on Ir<sub>0.7</sub>Ta<sub>0.3</sub>O<sub>y</sub>/Bi<sub>x</sub>Ti<sub>1-x</sub>O<sub>z</sub> hetero-junction anodes with enhanced rate, current efficiency, and long-term stability compared to the Ir<sub>0.7</sub>Ta<sub>0.3</sub>O<sub>y</sub> anode. The effects of surficial Bi concentration are interrogated, focusing on relative distributions between surface-bound hydroxyl radical and higher oxide.</p>
Resumo:
Northern Ireland has approximately 1670 lakes, which cover 4.4% of the land surface. However, most of the water area is accounted for by the large lakes such as Lough Neagh (385 km2) and Lower Lough Erne (109.5 km ). The majority of lakes are less than 100 hectares in area. They tend to be distributed towards the south and west of the Province, where extensive drumlin swarms are rich in small waterbodies. In 1988-1991, 610 of the 708 lakes between one and 100 hectares were sampled by the Northern Ireland Lake Survey. The objective was to assess their conservation status based on their aquatic macrophyte flora, but in addition to extensive plant surveys, the water of each lake was analysed for a range of chemical variables. This article reports on a full-scale survey carried out in early March 2002. The survey was taken with help of two helicopters. The authorise summarise the results of the chemical analysis of the survey.
Resumo:
<p>Isoprene (ISO),the most abundant non-methane VOC, is the major contributor to secondary organic aerosols (SOA) formation. The mechanisms involved in such transformation, however, are not fully understood. Current mechanisms, which are based on the oxidation of ISO in the gas-phase, underestimate SOA yields. The heightened awareness that ISO is only partially processed in the gas-phase has turned attention to heterogeneous processes as alternative pathways toward SOA.</p> <p>During my research project, I investigated the photochemical oxidation of isoprene in bulk water. Below, I will report on the λ > 305 nm photolysis of H<sub>2</sub>O<sub>2</sub> in dilute ISO solutions. This process yields C<sub>10</sub>H<sub>15</sub>OH species as primary products, whose formation both requires and is inhibited by O<sub>2</sub>. Several isomers of C<sub>10</sub>H<sub>15</sub>OH were resolved by reverse-phase high-performance liquid chromatography and detected as MH<sup>+</sup> (m/z = 153) and MH<sup>+</sup>-18 (m/z = 135) signals by electrospray ionization mass spectrometry. This finding is consistent with the addition of ·OH to ISO, followed by HO-ISO· reactions with ISO (in competition with O<sub>2</sub>) leading to second generation HO(ISO)<sub>2</sub>· radicals that terminate as C<sub>10</sub>H<sub>15</sub>OH via β-H abstraction by O<sub>2</sub>.</p> <p>It is not generally realized that chemistry on the surface of water cannot be deduced, extrapolated or translated to those in bulk gas and liquid phases. The water density drops a thousand-fold within a few Angstroms through the gas-liquid interfacial region and therefore hydrophobic VOCs such as ISO will likely remain in these relatively 'dry' interfacial water layers rather than proceed into bulk water. In previous experiments from our laboratory, it was found that gas-phase olefins can be protonated on the surface of pH < 4 water. This phenomenon increases the residence time of gases at the interface, an event that makes them increasingly susceptible to interaction with gaseous atmospheric oxidants such as ozone and hydroxyl radicals.</p> <p>In order to test this hypothesis, I carried out experiments in which ISO(g) collides with the surface of aqueous microdroplets of various compositions. Herein I report that ISO(g) is oxidized into soluble species via Fenton chemistry on the surface of aqueous Fe(II)Cl<sub>2</sub> solutions simultaneously exposed to H<sub>2</sub>O<sub>2</sub>(g). Monomer and oligomeric species (ISO)1-8H<sup>+</sup> were detected via online electrospray ionization mass spectrometry (ESI-MS) on the surface of pH ~ 2 water, and were then oxidized into a suite of products whose combined yields exceed ~ 5% of (ISO)1-8H<sup>+</sup>. MS/MS analysis revealed that products mainly consisted of alcohols, ketones, epoxides and acids. Our experiments demonstrated that olefins in ambient air may be oxidized upon impact on the surface of Fe-containing aqueous acidic media, such as those of typical to tropospheric aerosols.</p> <p>Related experiments involving the reaction of ISO(g) with ·OH radicals from the photolysis of dissolved H<sub>2</sub>O<sub>2</sub> were also carried out to test the surface oxidation of ISO(g) by photolyzing H<sub>2</sub>O<sub>2</sub>(aq) at 266 nm at various pH. The products were analyzed via online electrospray ionization mass spectrometry. Similar to our Fenton experiments, we detected (ISO)1-7H<sup>+</sup> at pH < 4, and new m/z<sup>+</sup> = 271 and m/z<sup>-</sup> = 76 products at pH > 5.</p>
Resumo:
<p>Part I</p> <p>A study of the thermal reaction of water vapor and parts-per-million concentrations of nitrogen dioxide was carried out at ambient temperature and at atmospheric pressure. Nitric oxide and nitric acid vapor were the principal products. The initial rate of disappearance of nitrogen dioxide was first order with respect to water vapor and second order with respect to nitrogen dioxide. An initial third-order rate constant of 5.5 (± 0.29) x 10<sup>4</sup> liter<sup>2</sup> mole<sup>-2</sup> sec<sup>-1</sup> was found at 25˚C. The rate of reaction decreased with increasing temperature. In the temperature range of 25˚C to 50˚C, an activation energy of -978 (± 20) calories was found.</p> <p>The reaction did not go to completion. From measurements as the reaction approached equilibrium, the free energy of nitric acid vapor was calculated. This value was -18.58 (± 0.04) kilocalories at 25˚C.</p> <p>The initial rate of reaction was unaffected by the presence of oxygen and was retarded by the presence of nitric oxide. There were no appreciable effects due to the surface of the reactor. Nitric oxide and nitrogen dioxide were monitored by gas chromatography during the reaction.</p> <p>Part II</p> <p>The air oxidation of nitric oxide, and the oxidation of nitric oxide in the presence of water vapor, were studied in a glass reactor at ambient temperatures and at atmospheric pressure. The concentration of nitric oxide was less than 100 parts-per-million. The concentration of nitrogen dioxide was monitored by gas chromatography during the reaction.</p> <p>For the dry oxidation, the third-order rate constant was 1.46 (± 0.03) x 10<sup>4</sup> liter<sup>2</sup> mole<sup>-2</sup> sec<sup>-1</sup> at 25˚C. The activation energy, obtained from measurements between 25˚C and 50˚C, was -1.197 (±0.02) kilocalories.</p> <p>The presence of water vapor during the oxidation caused the formation of nitrous acid vapor when nitric oxide, nitrogen dioxide and water vapor combined. By measuring the difference between the concentrations of nitrogen dioxide during the wet and dry oxidations, the rate of formation of nitrous acid vapor was found. The third-order rate constant for the formation of nitrous acid vapor was equal to 1.5 (± 0.5) x 10<sup>5</sup> liter<sup>2</sup> mole<sup>-2</sup> sec<sup>-1</sup> at 40˚C. The reaction rate did not change measurably when the temperature was increased to 50˚C. The formation of nitric acid vapor was prevented by keeping the concentration of nitrogen dioxide low.</p> <p>Surface effects were appreciable for the wet tests. Below 35˚C, the rate of appearance of nitrogen dioxide increased with increasing surface. Above 40˚C, the effect of surface was small. </p>
Resumo:
O presente estudo teve como objetivo quantificar as emissões de Compostos Orgânicos Voláteis do Aterro Controlado Morro do Céu localizado na cidade de Niterói, Rio de Janeiro, Brasil. Para tanto, vinte amostras foram coletadas, usando uma bomba de ar operada a bateria durante dois dias de dezembro de 2009. Uma câmara de fluxo cilÃndrica de PVC de 30L foi inserida 5 cm no solo do aterro, e as amostras foram coletadas através de uma válvula na parte superior da câmera. Os resultados indicaram um valor de 1.980 Kg Km-2 h-1. O modelo Gaussiano de dispersão atmosférica ISCST3 foi utilizado para calcular a difusão e transporte dos poluentes a fim de estimar as concentrações de COV no bairro, usando dados topográficos, meteorológicos e de emissões. Valores de 525 μg m-3 de COV foram encontrados a 500 metros do aterro. As emissões do aterro foram usadas em conjunto com dados meteorológicos, utilizando o modelo de trajetória OZIPR e o mecanismo quÃmico SAPRC para demonstrar o impacto na formação do ozônio troposférico na região. É conhecido que o ozônio é formado pela reação entre COV, NOx e luz solar. A contribuição de valores elevados de COV provenientes das emissões do aterro conduzirá a uma nova situação com valores mais elevados de ozônio na região. Os resultados da modelagem indicaram um aumento maior que 1000% nos nÃveis de ozônio na região do aterro, se comparado com a modelagem do ozônio para a região metropolitana do Rio de Janeiro. Os resultados mostram ser necessário que maior atenção seja dada à polÃtica de gerenciamento de RSU no Brasil, incluindo a escolha adequada para o local de instalação, o monitoramento da área durante e após o perÃodo de operação e técnicas mais adequadas de disposição dos resÃduos sólidos urbanos
Resumo:
Os modelos de dispersão de ar têm sido utilizados amplamente para investigação de padrões de dispersão, comportamento de emissões, estimativas de potenciais riscos a saúde humana, elaboração de propostas de gerenciamento ambiental e, também, na previsão de impacto da qualidade do ar. Alguns modelos, homologados por agência de regulação de alguns paÃses ou comunidades, servem de base para as análises de risco com auxÃlio de simulação. Somente após este tipo de análise uma unidade fabril terá direito à sua instalação e operação nestes paÃses. Nesta dissertação, serão abordados os principais poluentes presentes em uma indústria petroquÃmica básica, uma revisão sobre os principais tipos de modelos existentes no mercado e um estudo de caso será realizado empregando os modelos AERMOD e OZIPR/SAPRC. A indústria petroquÃmica básica a servir de modelo será o Complexo PetroquÃmico do Rio de Janeiro, que deverá ser instalado no municÃpio de Itaboraà e com operação prevista para o ano de 2012. De acordo com as simulações realizadas neste trabalho, o poluente NOx apresentou os resultados mais crÃticos violando em algumas áreas os padrões primários e secundários de emissão. Diante deste fato, o ozônio se tornou um poluente secundário importante a ser analisado. E para sua simulação, premissas tiveram que ser tomadas, devido a ausência de dados, criando cenários que apresentaram resultados dÃspares: Ora violando os limites, ora se mantendo abaixo deles. Apesar disso, estes cenários apontaram a mesma solução para minimizar esta formação de ozônio: controlar as emissões de compostos orgânicos voláteis.