780 resultados para EXPLOSION


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Femtosecond explosive processes of argon clusters irradiated by linearly chirped ultraintense laser pulses have been investigated by 90 degrees side spectral scattering. The spectral redshift and blueshift, which correlate with the cluster explosion processes have been measured for negatively and positively chirped driving laser pulses, respectively. The evolution of the heated-cluster polarizability indicates that the core of the cluster is shielded from the laser field in the beginning of the explosion and enhanced scattering occurs after the fast explosion initiates. Evidence of resonant heating is found from the coincidence of enhanced scattering with enhanced absorption measured using the transmitted spectra. Anomalously large-size clusters with very low gas density have been observed in this way and can be used as clean and important cluster targets.

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The explosion dynamics of hydrogen clusters driven by an ultrashort intense laser pulse has been analyzed analytically and numerically by employing a simplified Coulomb explosion model. The dependence of average and maximum proton kinetic energy on cluster size, pulse duration, and laser intensity has been investigated respectively. The existence of an optimum cluster size allows the proton energy to reach the maximum when the cluster size matches with the intensity and the duration of the laser pulse. In order to explain our experimental results such as the measured proton energy spectrum and the saturation effect of proton energy, the effects of cluster size distribution as well as the laser intensity distribution on the focus spot should be considered. A good agreement between them is obtained.

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Two overrun effects in the Coulomb explosion dynamics of heteronuclear clusters have been investigated theoretically by the use of a simplified electrostatic model. When the charge-to-mass ratio of light ions is higher than that of heavy ions, the light ions can overtake the heavy ions inside the cluster and acquire a higher kinetic energy. Further, if the charge density of the heavy ions is twice as high as that of the light ions, i.e. a proposed competitive parameter xi = rho BqB/rho AqA > 2, the inner light ions can overtake those light ions on the surface of the cluster and form a shock shell during the explosion, which might drive the intracluster collision and fusion of the light ions. Different regimes of nuclear fusion are discussed and the corresponding neutron yields are estimated. Our analysis indicates that the probability of intracluster fusion is quite low even if deuterated heteronuclear clusters such as (DI)(n) with large size and high competitive parameter are employed. However, heteronuclear clusters are still a better candidate compared with homonuclear clusters for enhancing the total intercluster fusion yield because both a higher energy region and a higher proportion of deuterons distributing in the energy region can be created in the deuterated heteronuclear clusters.

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Actualmente ningún área científica es ajena a la revolución de la nanociencia; las nanopartículas atraen el interés de muchos investigadores desde el punto de vista de la ciencia fundamental y para sus aplicaciones tecnológicas. Las nanopartículas ofrecen la posibilidad de fabricar sensores que sean capaces de detectar desde un virus hasta concentraciones de substancias patógenas que no pueden ser detectadas por los métodos convencionales. Hoy en día existes 82 tratamientos contra el cáncer basadas en la utilización de nanopartículas y los materiales composite con nanopartículas se utilizan como medio de protección frente a la radiación del rango de microondas. En la rama de ciencias ambientales, las nanopartículas metálicas sirven como materiales anticontaminantes. En la primera etapa de este trabajo, se ha estudiado la estructura cristalina y las propiedades magnéticas de las nanopartículas de FeNi, obtenidas por el método EEW, compactadas en forma de toroide. Para el aprendizaje del difractometro utilizado para este trabajo y el método de difracción de Rayos-X, se ha asistido al curso “Caracterización de materiales mediante DRX-P” impartido por SGIker de la UPV/EHU. Con la técnica de Rayos-X se ha determinado que el toroide consiste en dos fases: el FeNi metálico y el NiFe2O4. Ambos se cristalizan en un sistema cúbico FCC. Se ha determinado un valor de 50 nm del tamaño de dominio coherente de difracción en la superficie del toroide y aproximadamente el doble en el interior. Se han empleado los microscopios electrónicos SEM y TEM para obtener imágenes de gran resolución de la muestra y analizar su contenido elemental. Se puede apreciar que el toroide, efectivamente, es el fruto de la compactación de nanopartículas de alrededor de 60 nm. Para la caracterización magnética se ha utilizado el “trazador de ciclos” y el magnetómetro de muestra vibrante. Consiguiendo un valor de saturación, en uno de los toroides, de 140 emu/g con la aplicación de un campo magnético de 0.15 kOe. Estos valores dependen de los tratamientos recibidos. En la segunda etapa, se han realizado distintas mezclas de polímetro y nanopartículas para obtener los composites en forma de lámina y analizar su capacidad de absorción frente a la radiación en el rango de microondas. Todas las medidas de absorción en función del campo magnético externo muestran una absorción pronunciada en el campo cero y un desplazamiento a la izquierda del pico de resonancia respecto a la posición esperada para partículas esféricas. Dicho desplazamiento se interpreta, aparte de otros mecanismos, como el resultado de la existencia de la estructura cristalina tipo “gemelos” en algunas nanopartículas. La absorción en campo cero y el ensanchamiento de la línea de resonancia ferromagnética de los composites tipo polímero/nanopartículas de FeNi forman una solida base de las posibles aplicaciones de estos materiales como absorbentes en el rango de microondas.

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The majority of computational studies of confined explosion hazards apply simple and inaccurate combustion models, requiring ad hoc corrections to obtain realistic flame shapes and often predicting an order of magnitude error in the overpressures. This work describes the application of a laminar flamelet model to a series of two-dimensional test cases. The model is computationally efficient applying an algebraic expression to calculate the flame surface area, an empirical correlation for the laminar flame speed and a novel unstructured, solution adaptive numerical grid system which allows important features of the solution to be resolved close to the flame. Accurate flame shapes are predicted, the correct burning rate is predicted near the walls, and an improvement in the predicted overpressures is obtained. However, in these fully turbulent calculations the overpressures are still too high and the flame arrival times too low, indicating the need for a model for the early laminar burning phase. Due to the computational expense, it is unrealistic to model a laminar flame in the complex geometries involved and therefore a pragmatic approach is employed which constrains the flame to propagate at the laminar flame speed. Transition to turbulent burning occurs at a specified turbulent Reynolds number. With the laminar phase model included, the predicted flame arrival times increase significantly, but are still too low. However, this has no significant effect on the overpressures, which are predicted accurately for a baffled channel test case where rapid transition occurs once the flame reaches the first pair of baffles. In a channel with obstacles on the centreline, transition is more gradual and the accuracy of the predicted overpressures is reduced. However, although the accuracy is still less than desirable in some cases, it is much better than the order of magnitude error previously expected.