50 resultados para ship emission


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Many cities in Europe have difficulties to meet the air quality standards set by the European legislation, most particularly the annual mean Limit Value for NO2. Road transport is often the main source of air pollution in urban areas and therefore, there is an increasing need to estimate current and future traffic emissions as accurately as possible. As a consequence, a number of specific emission models and emission factors databases have been developed recently. They present important methodological differences and may result in largely diverging emission figures and thus may lead to alternative policy recommendations. This study compares two approaches to estimate road traffic emissions in Madrid (Spain): the COmputer Programme to calculate Emissions from Road Transport (COPERT4 v.8.1) and the Handbook Emission Factors for Road Transport (HBEFA v.3.1), representative of the ‘average-speed’ and ‘traffic situation’ model types respectively. The input information (e.g. fleet composition, vehicle kilometres travelled, traffic intensity, road type, etc.) was provided by the traffic model developed by the Madrid City Council along with observations from field campaigns. Hourly emissions were computed for nearly 15 000 road segments distributed in 9 management areas covering the Madrid city and surroundings. Total annual NOX emissions predicted by HBEFA were a 21% higher than those of COPERT. The discrepancies for NO2 were lower (13%) since resulting average NO2/NOX ratios are lower for HBEFA. The larger differences are related to diesel vehicle emissions under “stop & go” traffic conditions, very common in distributor/secondary roads of the Madrid metropolitan area. In order to understand the representativeness of these results, the resulting emissions were integrated in an urban scale inventory used to drive mesoscale air quality simulations with the Community Multiscale Air Quality (CMAQ) modelling system (1 km2 resolution). Modelled NO2 concentrations were compared with observations through a series of statistics. Although there are no remarkable differences between both model runs, the results suggest that HBEFA may overestimate traffic emissions. However, the results are strongly influenced by methodological issues and limitations of the traffic model. This study was useful to provide a first alternative estimate to the official emission inventory in Madrid and to identify the main features of the traffic model that should be improved to support the application of an emission system based on “real world” emission factors.

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Particulate matter emissions from paved roads are currently one of the main challenges for a sustainable transport in Europe. Emissions are scarcely estimated due to the lack of knowledge about the resuspension process severely hampering a reliable simulation of PM and heavy metals concentrations in large cities and evaluation of population exposure. In this study the Emission Factors from road dust resuspension on a Mediterranean freeway were estimated per single vehicle category and PM component (OC, EC, mineral dust and metals) by means of the deployment of vertical profiles of passive samplers and terminal concentration estimate. The estimated PM10 emission factors varied from 12 to 47 mg VKT?1 (VKT: Vehicle Kilometer Traveled) with an average value of 22.7 ? 14.2 mg VKT?1. Emission Factors for heavy and light duty vehicles, passenger cars and motorbikes were estimated, based on average fleet composition and EPA ratios, in 187e733 mg VKT?1, 33e131 VKT?1, 9.4e36.9 VKT?1 and 0.8e3.3 VKT?1, respectively. These range of values are lower than previous estimates in Mediterranean urban roads, probably due to the lower dust reservoir on freeways. PM emitted material was dominated by mineral dust (9e10 mg VKT?1), but also OC and EC were found to be major components and approximately 14 e25% and 2e9% of average PM exhaust emissions from diesel passenger cars on highways respectively.

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CO2 Emission from two old mine drillings (Mt. Amiata, Central Italy) as a possible example of storage and leakage of deep-seated CO2

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1. Introduction 2. Air Quality Modeling system 3. Emission Inventories 4. Applications and Results 5. Conclusions

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Modeling is an essential tool for the development of atmospheric emission abatement measures and air quality plans. Most often these plans are related to urban environments with high emission density and population exposure. However, air quality modeling in urban areas is a rather challenging task. As environmental standards become more stringent (e.g. European Directive 2008/50/EC), more reliable and sophisticated modeling tools are needed to simulate measures and plans that may effectively tackle air quality exceedances, common in large urban areas across Europe, particularly for NO2. This also implies that emission inventories must satisfy a number of conditions such as consistency across the spatial scales involved in the analysis, consistency with the emission inventories used for regulatory purposes and versatility to match the requirements of different air quality and emission projection models. This study reports the modeling activities carried out in Madrid (Spain) highlighting the atmospheric emission inventory development and preparation as an illustrative example of the combination of models and data needed to develop a consistent air quality plan at urban level. These included a series of source apportionment studies to define contributions from the international, national, regional and local sources in order to understand to what extent local authorities can enforce meaningful abatement measures. Moreover, source apportionment studies were conducted in order to define contributions from different sectors and to understand the maximum feasible air quality improvement that can be achieved by reducing emissions from those sectors, thus targeting emission reduction policies to the most relevant activities. Finally, an emission scenario reflecting the effect of such policies was developed and the associated air quality was modeled.

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A new material, C12A7 : electride, which might present a work function as low as 0.6 eV and moderately high temperature stability, was recently proposed as coating for floating bare tethers. Arising from heating under space operation, current is emitted by thermionic emission along a thus coated cathodic segment. A preliminary study on the space-charge-limited (SCL) double layer in front of the cathodic segment is presented using Langmuir’s SCL electron current between cylindrical electrodes and orbital-motion-limited ion-collection sheath. A detailed calculation of current and bias profiles along the entire tether length is carried out with ohmic effects and the transition from SCL to full Richardson-Dushman emission included. Analysis shows that in the simplest drag mode, under typical orbital and tether conditions, thermionic emission leads to a short cathodic section and may eliminate the need for an active cathodic device and its corresponding gas feed requirements and power subsystem, which results in a truly “propellant-less” tether system for such basic applications as de-orbiting low earth orbit satellites.

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El trabajo se desarrolló en tres etapas de investigación, las dos primeras fueron realizadas en la Unidad Básica de Producción Cooperativa “El Palmar” perteneciente a la Empresa de Cultivos Varios "Paquito Rosales Benítez" del municipio de Yara, provincia de Granma, Cuba, el cual se llevó a cabo en el período de abril de 2005 a enero de 2008; y de noviembre de 2012 a febrero de 2013 respectivamente; la tercera se ejecutó de mayo a junio de 2013 en un canal de suelo ubicado en la nave de maquinaria del Departamento de Ingeniería Rural de la Universidad Politécnica de Madrid. En la primera etapa se evaluaron los conjuntos tractor-apero que intervienen en la realización de cuatro sistemas de labranza para el cultivo de la yuca, variedad Enana Rosada. Los sistemas de laboreo fueron: T1, labor de aradura (alzado) con un arado de discos seguidas de un pase de grada de discos un pase cruzado de un escarificador y un pase con una grada de discos (5 labores); T2, laboreo mínimo que comprende una labor profunda con un escarificador con saetas seguido por una labor de grada de discos (2 labores); T3, laboreo mínimo en el que se realizaron dos pases cruzados con escarificador y una labor de fresado con una fresadora de eje horizontal (3 labores) y; T4, dos labores cruzadas con la grada de discos seguidas por otras dos pases cruzados con el escarificador y una última labor con la grada de discos (5 labores). Se realizaron cinco observaciones de la jornada laboral para cada uno de los conjuntos tractorapero de cada sistema de laboreo en tres campañas, evaluando el consumo de combustible, las diferentes productividades, los índices y coeficientes tecnológicos y de explotación, el rendimiento del cultivo el balance energético del mismo, y la emisión de CO2 equivalente. En la segunda etapa se determinó la fuerza de tiro requerida por un órgano de trabajo de un escarificador con saetas en condiciones de campo, en tres profundidades (15, 25 y 35 cm) y a cuatro velocidades de trabajo (1,30; 1,49; 1,65 y 2,32 m s-1). En la tercera etapa se determinaron las fuerzas horizontales y verticales en una maqueta experimental de un órgano de trabajo de un escarificador con saetas (1:5 del tamaño real del apero) en cuatro contenidos de humedad (60, 90, 120 y 150 g kg-1), tres densidades del suelo (1,1; 1,2 y 1,3 Mg m-3) y una velocidad de 40 mm s-1. Se comparan los resultados del apero a tamaño real y la maqueta experimental. Los mejores resultados relacionados con los indicadores evaluados a la maquinaria correspondieron al sistema de laboreo mínimo T2, el cual presenta la mejor productividad por hora de tiempo limpio (1,34 ha h-1) y de tiempo operativo (1,27 ha h-1), con diferencias significativas respecto al resto de los sistemas de labranza evaluados; así como el menor consumo de combustible (32,4 L ha-1) y el mejor comportamiento energético, con diferencias significativas respecto a las demás, resultando inferior en un 63, 30 y 58 % con relación a T1, T3 y T4. La fuerza de tiro del órgano de trabajo del escarificador con saetas se incrementa con la densidad del suelo y con la profundidad, y velocidad de trabajo. Las fuerzas horizontales y verticales de la maqueta se incrementan linealmente con la densidad y humedad del suelo. Existe una relación lineal entre las fuerzas de tiro y horizontales medidas en el apero real y en el apero a escala con el contenido de humedad del suelo. ABSTRACT The work was developed in three stages of research, the first two were conducted in the Basic Unit of Cooperative Production "El Palmar" belonging to the agricultural farm "Paquito Rosales Benitez" in the municipality of Yara, Granma Province, Cuba, the which was conducted in the period from April 2005 to January 2008 and November 2012 and February 2013 respectively, the third from May to June 2013 on a soilbin located in the ship's machinery of Rural Engineering Department of the Technical University of Madrid. In the first stage were evaluated tractor-implement sets involved in the completion of four tillage systems for cassava, Pink Dwarf variety. Tillage systems were: T1, plowing (elevation) with a disk plow followed by a pass of disc harrow, a cross of scarifier and a pass with a disc harrow (5 labours), T2, minimum tillage comprising a deep work with a scarifier with a bolt followed by a disc harrow work (two labours); T3, minimum tillage which two crossed passes performed with scarifier and milling labour with a horizontal axis milling machine (three labours) and, T4, two crossed labours with disc harrow followed by two crossed passes with the scarifier and a final labour with disc harrow (5 labours). Five observations of the working day for each tractor-implement sets of each tillage system in three seasons were performed, evaluating fuel consumption, different productivities, indexes and technological and operational factors, the crop yield energy balance and the emission of CO2 equivalent. In the second stage we determined the draft force required by a working body of a scarifier with bolt under field conditions at three depths (15, 25 and 35 cm) and four operating speeds (1.30, 1.49 , 1.65 and 2.32 m s-1). In the third stage were determined horizontal and vertical forces on an experimental model of a working body of a scarifier with bolt (1:5 real scale of the implement) in four moisture contents (60, 90, 120 and 150 g kg -1), three soil densities (1.1, 1.2, and 1.3 Mg m-3) and a speed of 40 mm s-1.The results of real scale implement the experimental model were compared. The best results related to evaluated machinery indicators corresponded to T2 minimum tillage system, which presents the best productivity per hour clean time (1.34 ha h-1) and operating time (1.27 ha h-1), with significant differences compared to other tillage systems evaluated; as well as lower fuel consumption (32.4 L ha-1) and the best energy performance, with significant differences from the other, resulting lower by 63, 30 and 58% compared to T1, T3 and T4. The draft force of the working body of the scarifier with bolt increases with soil density and depth, and speed of work. The horizontal and vertical forces of the model increase linearly with density and soil moisture. A linear relationship exists between the shot and horizontal forces measured at the real implement and scale implement with the soil moisture content.

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The purpose of this research is to assess the effectiveness of a ship used as a detached floating breakwater for coastal protection and forming salients of sand or tombolos. Floating breakwaters have been extensively used as port or coastal protection structures and display advantages in terms of construction and ecology, amongst others. However, the greatest problem these structures present is the limited range of wave heights and periods for which they are really effective. Furthermore, ships may be considered as floating structures which, used as breakwaters, would keep the advantages of floating breakwaters and would increase their range of applicability. The possibility of using ships at the conclusion of their useful life for this purpose would also involve greater economic and environmental advantages. Tests were carried out to assess the ship’s effectiveness as a detached floating breakwater using a scaled down physical model to determine the vessel’s transmission coefficient (Kt) as to regular waves with significant periods of 5 sec to 12 sec and significant wave heights of 1.5 m to 4 m at depths from 20 m to 35 m. The ship proves effective for waves up to 4 m significant height and significant periods up to 9 sec. Hanson and Kraus and Pilarzyk’s analytical models, which take transmission coefficients into account, were used to analyse the shore’s response to the breakwater protection. The results obtained show that salients form for waves with periods between 6 sec and 9 sec. It is also concluded that the depths tested are far different from the more usual shallow water involved in constructing detached breakwaters and the shore’s response is therefore scarce.

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A numerical description is given for the pulsating emission of droplets from an electrified meniscus of an inviscid liquid of infinite electrical conductivity which is injected at a constant flow rate into a region of uniform, continuous or time periodic, electric field. Under a continuous field, the meniscus attains a periodic regime in which bursts of tiny droplets are emitted from its tip. At low electric fields this regime consists of sequences of emission bursts interspersed with sequences of meniscus oscillations without droplet emission, while at higher fields the bursts occur periodically. These results are in qualitative agreement with experimental results in the literature. Under a time periodic electric field with square waveform, the electric stress that acts on the surface of the liquid while the field is on may generate a tip that emits tiny droplets or may accelerate part of the meniscus and lead to a second emission mode in which a few large droplets are emitted after the electric field is turned off. Conditions under which each emission mode or a combination of the two are realized are discussed for low frequency oscillatory fields. A simplified model is proposed for high electric field frequencies, of the order of the capillary frequency of the meniscus. This model allows computing the average emission rate as a function of the amplitude, duration and bias of the electric field square wave, and shows that droplet emission fails to follow the applied field above a certain frequency

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Existing descriptions of bi-directional ammonia (NH3) land–atmosphere exchange incorporate temperature and moisture controls, and are beginning to be used in regional chemical transport models. However, such models have typically applied simpler emission factors to upscale the main NH3 emission terms. While this approach has successfully simulated the main spatial patterns on local to global scales, it fails to address the environment- and climate-dependence of emissions. To handle these issues, we outline the basis for a new modelling paradigm where both NH3 emissions and deposition are calculated online according to diurnal, seasonal and spatial differences in meteorology. We show how measurements reveal a strong, but complex pattern of climatic dependence, which is increasingly being characterized using ground-based NH3 monitoring and satellite observations, while advances in process-based modelling are illustrated for agricultural and natural sources, including a global application for seabird colonies. A future architecture for NH3 emission–deposition modelling is proposed that integrates the spatio-temporal interactions, and provides the necessary foundation to assess the consequences of climate change. Based on available measurements, a first empirical estimate suggests that 5°C warming would increase emissions by 42 per cent (28–67%). Together with increased anthropogenic activity, global NH3 emissions may increase from 65 (45–85) Tg N in 2008 to reach 132 (89–179) Tg by 2100.

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The aim of this work is to test the present status of Evaluated Nuclear Decay and Fission Yield Data Libraries to predict decay heat and delayed neutron emission rate, average neutron energy and neutron delayed spectra after a neutron fission pulse. Calculations are performed with JEFF-3.1.1 and ENDF/B-VII.1, and these are compared with experimental values. An uncertainty propagation assessment of the current nuclear data uncertainties is performed.

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The determination of the plasma potential Vpl of unmagnetized plasmas by using the floating potential of emissive Langmuir probes operated in the strong emission regime is investigated. The experiments evidence that, for most cases, the electron thermionic emission is orders of magnitude larger than the plasma thermal electron current. The temperature-dependent floating potentials of negatively biased Vpmenor queVpl emissive probes are in agreement with the predictions of a simple phenomenological model that considers, in addition to the plasma electrons, an ad-ditional electron group that contributes to the probe current. The latter would be constituted by a fraction of the repelled electron thermionic current, which might return back to the probe with a different energy spectrum. Its origin would be a plasma potential well formed in the plasma sheath around the probe, acting as a virtual cathode or by collisions and electron thermalization pro-cesses. These results suggest that, for probe bias voltages close to the plasma potential Vp?Vpl, two electron populations coexist, i.e., the electrons from the plasma with temperatureTeand a large group of returned thermionic electrons. These results question the theoretical possibility of measuring the electron temperature by using emissive probes biased to potentials Vp about lower equal than ?Vpl.

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We discuss two different approaches to overcome the power limitations of CW THz generation imposed to conventional photomixers. The increase in power achievable by using arrays of AEs is studied. Then ?large area emitters? are proposed as an alternate approach to overcome the power limitations. In this antenna-free new scheme of photomixing, the THz radiation originates directly from the acceleration of photo-induced charge carriers generated within a large semiconductor area. The quasi-continuous distribution of emitting elements corresponds to a high-density array and results in particularly favorable radiation profiles.