Tsunami are a fascinating but potentially devastating natural phenomena that have occurred regularly throughout history along New Zealand's shorelines, and around the world. With increasing population and the construction of infrastructure in coastal zones, the effect of these large waves has become a major concern. Many natural phenomena are capable of creating tsunami. Of particular concern is the underwater landslide-induced tsunami, due to the potentially short warning before waves reach the shore. The aims of this research are to generate a quality benchmark dataset suitable for comprehensive comparisons with numerical model results and to increase our understanding of the physical processes involved in tsunami generation. The two-dimensional experimental configuration is based on a benchmark configuration described in the scientific literature, consisting of a semi-elliptical prism sliding down a submerged 15° slope. A unique feature of these experiments is the method developed to measure water surface variation continuously in both space and time. Water levels are obtained using an optical technique based on laser induced fluorescence, which is shown to be comparable in accuracy and resolution to traditional electrical point wave gauges. In the experiments, the landslide density and initial submergence are varied and detailed measurements of wave heights, lengths, propagation speeds, and shore run-up are made. Particle tracking velocimetry is used to record the landslide kinematics and sub-surface water velocities. Particular attention is paid to maintaining a high level of test repeatability throughout the experimental process. The experimental results show that a region of high pressure ahead of the landslide forces up the water over the front half of the landslide to form the leading wave crest, which propagates ahead of the landslide. The accelerating fluid above, and the turbulent wake behind, the moving landslide create a region of low pressure, which draws down the water surface above the rear half of the landslide to form the leading trough. Differences in the phase and group velocities of the components in the wave packet cause waves to be continually generated on the trailing end of the wave train. The downstream position that these waves form continually moves downstream with time and the wave packet is found to be highly dispersive. The interaction of the landslide pressure field with the free surface wave pressure field is important, as the location of the low pressure around the landslide relative to the wave field acts to reinforce or suppress the waves above. This has a substantial effect on the increase or decrease in wave potential energy. When the low pressure acts to draw down a wave trough, the wave potential energy increases. When the low pressure is below a wave crest, it acts to suppress the crest amplitude, leading to an overall decrease in wave potential energy. Measurements of the efficiency of energy transfer from the landslide to the wave field show that the ratio of maximum wave potential energy to maximum landslide kinetic energy is between 0.028 and 0.138, and tends to increase for shallower initial landslide submergences and heavier specific gravities. The ratio of maximum wave potential energy to maximum landslide potential energy ranges between 0.011 and 0.059 and tends to be greater for shallower initial submergences. For two experimental configurations the ratio of maximum wave potential energy to maximum fluid kinetic energy is estimated to be 0.435 and 0.588. The wave trough initially generated above the rear end of the landslide propagates in both onshore and offshore directions. The onshore-propagating trough causes a large initial draw-down at the shore. The magnitude of the maximum draw-down is related to the maximum amplitude of the offshore-propagating first wave trough. A wave crest generated by the landslide as it decelerates at the bottom of the slope causes the maximum wave run-up observed at the shore. A semi-analytical model, based on inviscid and irrotational theory, is used to investigate the wave generation process of a moving submerged object in a constant depth channel. The simplified geometry allows a variety of phenomena, observed during the experimental tests, to be investigated further in a more controlled setting. The variations in the growth, magnitude, and decay of energy as a function of time is due the interaction of the pressure distribution surrounding the moving slider with the wave field, in particular, the leading crest and trough. The largest energy transfer between slider kinetic energy and wave potential energy occurs when there is prolonged interaction between the slider's low pressure region and the leading wave trough. The generation of onshore propagating waves by a decelerating landslide is confirmed, and the magnitude of the maximum wave run-up is found to be dependent on the magnitude of the slider deceleration. The model also shows that slides with Froude number close to unity convert substantial amounts of energy into offshore propagating waves. The onshore propagating wave potential energy is not as sensitive to Froude number. A further result from the model simulations is that the specific shape of the slider has only a minor influence on the wave response, provided the slider's length and area are known. A boundary element model, based on inviscid and irrotational theory, is used to simulate the laboratory experiments. Model predictions of the wave field are generally accurate, particularly the magnitude and range of wave amplitudes within the wave packet, the arrival time of the wave group, the amplitude of the run-up and run-down at the shore, the time the maximum run-down occurs, and the form and magnitude of the wave potential energy time history. The ratios of maximum wave potential energy to maximum slider kinetic energy are predicted to within ± 29%. The model predictions of the crest arrival times are within 3.6% of the measured times. The inability of the inviscid and irrotational model to simulate the flow separation and wake motions lead to a 45% under prediction of the maximum fluid kinetic energy. Both the semi-analytical and BEM models highlight the need for the correct specification of initial slider accelerations in numerical simulations in order to accurately predict the wave energy.

A new Laser Induced Fluorescence Capillary Zone Electrophoresis (LIF-CZE) bioassay to detect and study the catalytic activity of the sulfur assimilating enzyme commonly found in E. coli species; alkanesulfonate monooxygenase (EC 1.14.14.5) is described for the first time. This technique enables the possibility for direct injection onto a capillary for detection without the need for pre-concentration of sample and with minimal sample preparative steps prior to analysis. In this bioassay, a group of Fischer based cyanine dyes and two Oxazine (Nile red) derivatives were designed for further optimization as key Vis-NIR fluorescent substrate. In developing this technique, the test dyes were first assessed for their photophysical properties, based on four criteria; (1) photostable (2) solvatochromism (3) binding affinity towards both the monooxygenase active site and serum albumin and (4) chemical stability in strong electric field strength. Applying key dye characterization procedures including; molar absorptivity determination, quantum yield determination, photostability, solvatochromism and protein interaction studies it was determined that the Fischer indolium cyanine dyes were most suitable for the method development. The data revealed that under the test conditions, reduced flavin, the oxidative monooxygenase catalytically specifically converts the alkylsulfonate substituted cyanine dyes to the corresponding aldehyde. This new bioassay has proven to be quick, portable, sensitive, reliable and the exhibit the possibility of ‘on-the-spot’ detection; advantages not readily realized with other commonly applied techniques such as PCR, SPR, ELISA and GC used to study bacterial sulfur assimilation processes. In addition, recent literature results proposed by other research groups developing similar techniques showed strong reliance on GC analyses. Those assays involve the use of low molecular weight straight chain non-emissive alkanesulfonate substrates. Once enzyme catalysis occurs the aldehyde is formed becomes rather volatile and requires complex and tedious headspace sampling for GC analyses. This feature limits the in vitro applicability and eliminated the possibility in vivo development. Our goal is to further develop, optimize and present this CZE based bioassay as a suitable alternative to the current trends in the field while creating a more robust and sensitive in vitro monooxygenase detection method with the possibilities of in vivo application.

An isolated wing-tip vortex from a square-tipped NACA 0012 wing at an angle of attack of 5 degrees was studied in a water tunnel at a chord based Reynolds number of approximately 24000. Measurements were taken using stereo particle image velocimetry at three measurement planes downstream of the wing under each of three freestream turbulence conditions. The amplitude of wandering of the vortex axis increased with increasing distance downstream of the wing and with increasing freestream turbulence intensity. The magnitude of the peak azimuthal velocity decreased with increasing distance from the wing as well as with increases in the freestream turbulence intensity. The streamwise velocity in the vortex core was less than the freestream velocity in all cases. Time resolved histories of the instantaneous waveform shape and location of the vortex axis were determined from sequences of images of fluorescent dye released from the wing.

In the frame of this thesis, a new experimental setup for the measurement of the energy loss of carbon ions at maximum stopping power in a hot laser-generated plasma has been developed and successfully tested. In this parameter range where the projectile velocity is of the same order of magnitude as the thermal velocity of the plasma free electrons, large uncertainties of up to 50% are present in the stopping-power description. To date, no experimental data are available to perform a theory benchmarking. Testing the different stopping theories is yet essential for inertial confinement fusion and in particular for the understanding of the alpha-particle heating of the thermonuclear fuel. Here, for the first time, precise measurements were carried out in a reproducible and entirely characterized beam-plasma configuration. It involved a nearly fully-stripped ion beam probing a homogeneous fully-ionized plasma. This plasma was generated by irradiating a thin carbon foil with two high-energy laser beams and features a maximum electron temperature of 200 eV. The plasma conditions were simulated with a two-dimensional radiative hydrodynamic code, while the ion-beam charge-state distribution was predicted by means of a Monte-Carlo code describing the charge-exchange processes of projectile ions in plasma. To probe at maximum stopping power, high-frequency pulsed ion bunches were decelerated to an energy of 0.5 MeV per nucleon. The ion energy loss was determined by a time-of-flight measurement using a specifically developed chemical-vapor-deposition diamond detector that was screened against any plasma radiation. A first experimental campaign was carried out using this newly developed platform, in which a precision better than 200 keV on the energy loss was reached. This allowed, via the knowledge of the plasma and of the beam parameters, to reliably test several stopping theories, either based on perturbation theory or on a nonlinear T-Matrix formalism. A preliminary analysis suggests that the energy deposition at maximum stopping power is significantly smaller than predicted, particularly, by perturbation approaches.

Cette thèse porte sur l’amélioration de la résistance au flux laser de la surface descomposants optiques en silice en régime nanoseconde. Ce matériau est utilisé sur lesinstallations de laser de puissance telles que le Laser Mégajoule. Pour augmenter la durée de viedes composants optiques et garantir le fonctionnement nominal de cette installation,l’endommagement laser doit être maîtrisé. Il s’agit d’une dégradation irréversible de la surfacedes composants causée par l’interaction entre le faisceau laser et des défauts précurseurs. Cesderniers sont une conséquence de la synthèse de la silice puis du polissage des composants etleur présence peut être limitée par une action de traitement chimique réalisée à l’issue dupolissage qui consiste à éroder la surface de silice à l’aide d’une solution chimique. Cette érosionne doit cependant pas dégrader la qualité de la surface polie et ses propriétés optiques. Cettethèse se concentre sur la réalisation de cette étape de traitement chimique et se décompose entrois études. La première porte sur la caractérisation de la pollution induite en surface par lepolissage et sa suppression par le traitement chimique. La seconde et la troisième analysentl’impact des traitements chimiques respectivement sur les propriétés optiques de la surface etsur les rayures de polissage. Ces études nous permettent d’évaluer l’influence des différentsparamètres du traitement chimique, tels que la solution, le système de mise en oeuvre etl’épaisseur érodée, sur les performances apportées aux composants optiques. Finalement,l’ensemble de ces connaissances nous conduit à proposer un traitement chimique optimisé quiaméliore la tenue au flux des composants optiques sans dégrader leurs propriétés optiques. / In this thesis, laser-induced damage resistance improvement of fused silica opticsis investigated in the nanosecond regime. This material is used on high power laser facilitiessuch as the Laser Mégajoule. In order to improve the optics life time and to ensure the nominaloperation of this facility, laser induced damage has to be controlled. This phenomenon is anirreversible modification of the components surface because of the interaction between the laserbeam and precursors defects. These defects are a consequence of the synthesis of silica and thepolishing of the optics and their presence can be reduced by a wet etching. This process consistsin an erosion of the surface using a chemical solution however optical properties must remainunchanged. In this thesis, we focus on the wet etching process and we conduct three studies. Thefirst one is about the characterization of the polishing induced contamination and the capabilityof a wet etching to remove it from the surface. The second and the third analyzes are about theimpact of the wet etching respectively on the surface and on the scratches. These studies allowus to evaluate the influence of the wet etching parameters as the chemical solution, the systemused and the deep etched. Finally, the highlights obtained thanks to these studies enable tooptimize the wet etching process and improve the laser induced damage resistance ofcomponents without compromising their optical properties.

Natural turbulent convection studies encompass a wide range of flows occurring in nature, for example, atmospheric and oceanic flows, con-vection in the Earth’s mantle, convection in the stars and also in many engineering applications. Rayleigh-Benard convection (RBC), i.e. con-vection in a horizontal fluid layer confined between two plates with a temperature differential maintained across them, has been a proto-type problem in the studies of turbulent natural convection. Many small scale and global features of the flow in the turbulent regime of RBC are known, yet the flow dynamics is not fully understood, es-pecially at high Rayleigh numbers (Ra). Present work comprises of experimental investigations of a different type of flow, high Rayleigh number turbulent convection in a long vertical tube (abbreviated as tube convection or TC). The tube of aspect ratio (length to diameter) of about 10, open at both the ends interconnects two large tanks. The flow driven by an unstable density difference created between the two tanks, has some unique features, different from RBC. The net flow at any tube cross-section is zero and the time averages of the velocities, the Reynolds shear stress and the mean shear are also zero. Turbu-lent energy production is therefore solely due to buoyancy. The flow is axially homogeneous and axisymmetric. In the homogeneous region, the mean density gradient is linear. Rayleigh number in TC is conve-niently defined based on the mean (linear) density gradient (denoted by Rag). Two sets of experiments are carried out. In one set of experiments, the density difference is created using brine and fresh water and in another set, it is created using heat. The ranges of Rag achieved are 3 × 108 < Rag < 8 × 109 in the experiments using salt (Schmidt number, Sc ≈ 600) and 5 × 104 < Rag < 5 × 106 in the experiments using heat (Prandtl number, P r ≈ 6). From the measured salt and heat fluxes in both the sets of experiments, the non dimensional flux 1 1 scaling above a certain value of Rag is obtained as N ug ∼ Rag2 P r 2 and from the velocity measurements in the experiments using salt, the 1 Reynolds number scaling is obtained as Re ∼ Rag2 P r− 12 . Both these are as per the predicted scalings by the mixing length model proposed by Arakeri et al. (2000) for high Rag convection in the vertical tube. The flux scaling N u ∼ (RaP r)2 , also known as the ‘ultimate regime’ of convection, expected at very high Ra but not yet observed in the experiments in classical RBC, is easily achieved in TC at relatively lower values of Ra. The fluxes and Reynolds numbers in TC are orders of magnitude higher as compared to those obtained in RBC for similar values of Ra and P r. In the lower range of Rag values for P r ≈ 6, a transition to a new flux scaling, N u ∼ (RaP r)0.29 is found. Similar transitions are also found to be present in the results of Tovar (2002) for Sc ≈ 600 and in the DNS results of Schmidt et al. (2012) for P r = 1, at different values of Rag. Collecting all these data, it is shown that the transition occurs at a fixed Grashof number of 1.6 × 105, independent of P r. Velocity measurements are carried out using particle image velocime-try (PIV) in the salt experiments. Kinetic energy spectra computed from the velocity fields are presented for the locations from the tube axis to the wall, for the lowest and the highest values of Rag achieved in the experiments. The spatial energy spectrum of lateral velocity at the tube axis follows Kolmogorov-Obukhov (KO) scaling (−5/3 scaling exponent) while the spatial spectrum of longitudinal velocity shows a scaling slightly higher than −5/3 but lower than −11/5 (the Bolgiano-Obukhov (BO) scaling). The scalar spectra is computed from the concentration fields obtained from planar laser induced fluorescence (PLIF) in the experiments using salt, and also from the temperature measurements from the experiments using heat. Both the concentra-tion and temperature fluctuations spectra show some evidence of dual scaling - BO scaling (−7/5 scaling exponent) in the inertial subrange followed by Obukhov-Corrsin (OC) scaling (−5/3 scaling exponent) over a narrow range of scales. Light propagation through the buoyancy driven turbulent flow in TC has also been experimentally investigated. Light propagation through convective turbulence is encountered in many situations. In some cases e.g. in observational astronomy it is undesirable, while in some other cases it is useful, e.g. in remote sensing of meteorological parameters. In the present study, light intensity and angle of arrival fluctuations in a parallel beam of light are measured. Laser shadowgraphy is used in the intensity measurements while the angle of arrival is obtained by measuring deflections of narrow laser beams, created by passing collimated laser light through a mask having equispaced grid of holes. Background oriented schlieren (BOS) measurements have also been carried out to obtain the displacements, which are proportional to the angle of arrivals. The equations for frequency spectrum of intensity and angle of arrival from the literature, developed for isotropic, ho-mogeneous turbulent media, are modified for the flow in the present case and the asymptotic scalings for high and low frequency ranges are obtained. The scalings in the frequency spectra computed from the measurements of intensity and angle of arrival fluctuations are com-pared with the obtained asymptotic scalings. The results from the present work are also compared with results from studies in the atmo-sphere and lab experiments.

Nos últimos 20 anos, a espectroscopia de emissão ótica com plasma induzido a laser (LIBS) tem se tornado uma das mais promissoras ferramentas em química analítica, cujas aplicações são destinadas às análises multi-elementares em amostras nos estados sólido, líquido e gasoso. Suas aplicações são as mais diversas, pois sua instrumentação é relativamente simples e pode ser portátil. Em especial, a LIBS apresenta grande potencial de uso na agricultura, com diversas publicações que exploram, principalmente, a concentração de carbono em solos. Entretanto, a construção de modelos gerais de calibração é uma das maiores dificuldades da técnica, pois ela está suscetível aos efeitos de matriz que adicionam comportamentos não-lineares às intensidades das emissões. Com intuito de compreender quais são as principais causas dessa dependência, este trabalho avaliou relações entre propriedades físicas do plasma LIBS e as inclinações das curvas de calibração para cinco emissões de carbono em amostras sintéticas de diferentes potenciais de ionização, sendo elas KCl e H3BO3 com 1% de CuSO4 e concentrações entre 0 e 10 % de carbono. Constatou-se que temperatura e densidade de elétrons dependem inversamente da concentração de carbono nas amostras, o que provavelmente está associado às taxas de ablação de material da amostra e recombinação no interior do plasma. Ademais, esses parâmetros em plasmas originados das amostras de KCl + CuSO4 são maiores do que para a matriz de H3BO3 + CuSO4, além de que apenas plasmas originados da primeira matriz satisfizeram o critério de McWhirter para C I, Cu I e Cu II em todas as concentrações de carbono, indicando que eles devem apresentar condições de equilíbrio termodiâmico local. O mesmo não foi obtido para o caso da matriz de H3BO3 + CuSO4, o que pode explicar suas elevadas incertezas nos valores da temperatura e densidade de elétrons. Verificou-se ainda que as inclinações das curvas de calibração para o carbono foram maiores para o caso da matriz com elementos majoritários de menor potencial de ionização e que isso está diretamente relacionado às propriedades intrínsecas dos plasmas originados, o que corrobora a hipótese deste trabalho. Além disso, cálculos de correlação entre a área do pico de carbono em 247,89 nm e cada ponto dos espectros LIBS mostraram que a emissão de Cu II em 224,72 nm linearizou as curvas de calibração, minimizando os efeitos de matriz. Por fim, este trabalho contribuiu tanto com avanços no conhecimento até então existente a respeito dos efeitos de matriz quanto com um eficiente conjunto de técnicas analíticas para espectros, cujo potencial de aplicação é enorme. / In the last 20 years, laser-induced breakdown spectroscopy (LIBS) has been one of the main tools in analytical chemistry, whose applications are destinated to multi-elementar analysis in solid, liquid or gaseous samples. Its use is diverse, since its instrumentation is relatively simple and can be portable. In particular, LIBS has a great potential for use in agriculture, with many publications that explore mainly the carbon concentration in soils. However, the construction of general calibration models is one of the greatest difficulties of the technique, since it is susceptible to matrix effects that add non-linear behaviors to the emission intensities. In order to understand the main causes of this dependence, this study evaluated the relationships between physical properties of the LIBS plasma and the slope of the calibration curves for carbon emissions in synthetic samples with different ionization potentials. Those samples were made of KCl and H3BO3 with 1% of CuSO4 and carbon concentrations ranging from 0 to 10%. It was found that the plasma temperature and electron density are inversely proportional to the carbon concentration in the samples, which is probably associated with rates of sample ablation and recombination within the plasma. In addition, these parameters in plasmas originating from the samples of KCl + CuSO4 are larger than those originating from the matrix of H3BO3 + CuSO4 at all carbon concentrations, indicating that the first matrix must be in local thermodynamics equilibrium. However, similar results were not found for the other matrix which may explain its high uncertainties in the values of temperature and electron density. It was verified that the slope of the carbon calibration curves were higher for the matrix with elements of low ionization potential than for the other matrix and that this is directly related to the intrinsic properties the plasmas originated, which corroborates the hypothesis of this study. Furthermore, the analysis of correlation between the carbon peak area at 247.89 nm and each point of the LIBS spectra have shown that the Cu II emission at 224.72 nm linearized the calibration curves, minimizing the matrix effects. Finally, this study contributed with advances in the knowledge about matrix effects and with an efficient set of analytical tools for spectra whose application potential is huge.

A cultura da cana-de-açúcar no Brasil é uma das atividades mais relevantes na agroindústria nacional devido ao alto potencial de produção e elevada importância econômica de seus subprodutos como e.g. açúcar e etanol. Embora o Si não seja considerado um elemento essencial, a adubação silicatada tem proporcionado aumentos apreciáveis na produtividade da cana-de-açúcar e na resistência a algumas pragas e doenças. Ainda não existem métodos bem estabelecidos para a determinação de Si em material vegetal visando à diagnose foliar. O objetivo deste trabalho foi desenvolver um método para determinação de Si em pastilhas de folhas de cana-de-açúcar por espectrometria de emissão óptica com plasma induzido por laser (LIBS). O arranjo experimental foi composto por um laser pulsado de Nd:YAG a 1064 nm (pulsos de 5 ns, 360 mJ, 10 Hz) e os sinais de emissão foram coletados por um telescópio acoplado por fibra óptica ao espectrômetro Echelle com detector ICCD. Amostras laboratoriais consistiram de pastilhas preparadas com folhas de cana-de-açúcar moídas criogenicamente por 40 min. Melhores resultados foram obtidos quando a linha de emissão Si I 212,412 nm foi selecionada e os parâmetros instrumentais foram ajustados em 25 pulsos acumulados, 50 J cm-2, diâmetro de focalização de 750 \'mü\'m, 2,0 \'mü\'s de atraso e 4,5 \'mü\'s de integração. Os resultados obtidos por LIBS na análise de pastilhas de 20 amostras laboratoriais foram comparados com os obtidos por espectrometria de emissão óptica com plasma acoplado indutivamente (ICP OES) após decomposição alcalina e por espectrometria de micro-fluorescência de raio-X por energia dispersiva (\'mü\'ED-XRF) após análise direta das pastilhas. Aplicando-se o teste t de Student pareado, não foram verificadas diferenças significativas ao nível de 95% de confiança nas determinações de Si por LIBS, ICP OES e \'mü\'ED-XRF. Os resultados obtidos nesta tese indicam a viabilidade de LIBS para determinação direta de Si em pastilhas de folhas de cana-de-açúcar e abrem uma expectativa para futuras explorações de LIBS em análises em campo / The high production of sugarcane and its subproducts (e.g. sugar and ethanol fuel) make this crop one of the most important for the Brazilian agro-industrial economy. Although Si is not considered an essential element, the Si-based fertilizers have provided considerable improvement in productivity of sugarcane and resistance to some pests and diseases. At moment, there are no well-established methods for the determination of Si in plant materials aiming at nutritional diagnosis. The aim of this work was to develop a method for Si determination in pellets of sugarcane leaves by laser-induced breakdown spectroscopy (LIBS). The experimental setup was designed by using a Q-switched Nd:YAG laser (5 ns, 360 mJ, 10 Hz, \'lâmbda\' = 1064 nm) and the emission signals were collected by lenses into an optical fiber coupled to an Echelle spectrometer equipped with an ICCD. Pellets prepared from cryogenically ground sugarcane leaves were used as laboratory samples. Best results were obtained when the Si I 212.412 nm emission line was selected and the instrumental parameters were adjusted at 25 laser shots, 50 J cm-2, 750 \'mü\'m laser spot size, 2.0 \'mü\'s delay time and 4.5 \'mü\'s integration time gate. The results obtained by LIBS in the analysis of pellets of 20 laboratory samples were compared with those from inductively coupled plasma optical emission spectrometry (ICP OES) after alkaline digestion and by microenergy dispersive X-ray fluorescence (\'mü\'ED-XRF) after direct analysis of pellets. By applying a paired t-test at 95 % confidence level, there was no significant difference in the Si determination by LIBS, ICP OES and \'mü\'ED-XRF. The findings of this thesis indicate the feasibility of LIBS for the direct determination of Si in pellets of sugarcane leaves and open expectations for future investigations of LIBS for field analysis

A espectrometria de emissão óptica com plasma induzido por laser (LIBS) constitui um método alternativo para a determinação simultânea de macro e micronutrientes em pastilhas de materiais vegetais. No entanto, pouca informação com relação às condições de fluência e de focalização do laser mais apropriadas para a análise de pastilhas de materiais vegetais são disponíveis na literatura. O objetivo deste trabalho foi avaliar os efeitos da fluência, do diâmetro de focalização do laser e do tamanho das partículas das amostras nas análises de pastilhas de tecidos vegetais por LIBS. O arranjo experimental foi composto por um laser pulsado de Nd:YAG a 1064 nm (pulsos de 5 n\'delta\', 360 mJ, 10 Hz) e os sinais de emissão foram coletados por um telescópio acoplado por fibra óptica ao espectrômetro Echelle com detector ICCD. Os parâmetros instrumentais foram ajustados em 20 pulsos acumulados, 2,0 \'mü\'s de atraso e 5,0 \'mü\'s de integração. Amostras laboratoriais consistiram de pastilhas preparadas com folhas moídas criogenicamente (90 % das partículas < 50 \'mü\'m). Maiores intensidades das linhas Ca I 442,554, Mg I 277,983, P I 213,618, Al I 309,271, B I 249,773, Cu I 324,755, Fe II 261,187, Mn II 257,610 e Zn II 206,200 nm foram obtidas com fluências entre 35 e 60 J cm-2 e diâmetros de focalização entre 600 e 1050 \'mü\'m. O uso de fluências e diâmetros de focalização maiores concorreu para melhorar os coeficientes de variação (CV) das medidas. Fixando-se o diâmetro de focalização em 750 \'mü\'m, observou-se que, para a maioria dos analíticos, o CV das medidas foi reduzido 2 vezes quando a fluência foi alterada de 20 para 50 J cm-2. Nestas condições, estes resultados foram atribuídos à maior massa removida e, conseqüentemente, à amostragem mais representativa. Os coeficientes angulares das curvas de calibração também aumentaram quando a fluência foi acrescida. No entanto, não foram verificadas diferenças significativas nos coeficientes de correlação das curvas de calibração e nos limites de detecção empregando-se 25 e 50 J cm-2. Embora as intensidades dos sinais de emissão aumentem com a fluência, a emissão de fundo também aumenta. Por outro lado, o tamanho das partículas das amostras afeta as eficiências de atomização e excitação no plasma induzido por laser. Quando partículas maiores são parcialmente vaporizadas, os sinais de emissão resultantes dos processos de atomização e excitação das espécies constituintes são menores do que os provenientes de partículas menores. Nesta dissertação, melhorias significativas da intensidade dos sinais de emissão e dos CVs das medidas foram observados quando pastilhas preparadas com partículas < 75 \'mü\'m foram analisadas. Não foram observadas diferenças significativas nas intensidades dos sinais de emissão e no CV das medidas nas análises de pastilhas preparadas com partículas entre 20 e 75 \'mü\'m. Pastilhas preparadas com partículas > 75 \'mü\'m apresentaram problemas de coesão e, após ablação, apresentaram crateras não uniformes. A análise destas pastilhas resultou em CV das medidas geralmente > 15 %. Os resultados obtidos neste trabalho confirmaram que é recomendável utilizar amostras de calibração e amostras-teste com distribuição do tamanho das partículas semelhante para evitar efeitos físicos de matriz, que alteram as interações laser-amostra / Most recently, it was demonstrated that laser induced breakdown spectrometry (LIBS) constitutes an alternative for the simultaneous determination of macro- and micronutrients in pellets of plant materials. However, there is no information regarding the most appropriate fluence and laser focusing for analysis of pellets of plant materials. The aim of this work was to evaluate the effect of laser focusing and fluence on LIBS analysis of plants. The effect of particle size on LIBS analysis of pellets of plant materials as well as sample preparation approaches were also discussed. The experimental setup was designed by using a Q-switch Nd:YAG laser (5 n\'delta\', 360 mJ, 10 Hz, _ \'lâmbda\' = 1064 nm) and the emission signals were collected by lenses into an optical fiber coupled to an echelle spectrometer equipped with a high-resolution ICCD. Instrumental parameters consisted of 20 accumulated laser pulses, 2.0 \'mü\'s delay time and 5.0 \'mü\'s integration time gate. Pellets prepared from cryogenically ground plant leaves (90 % particles < 50 \'mü\'m; median = 10 \'mü\'m) were used as laboratory samples and 6 laser spot diameters (from 180 to 1050 \'mü\'m) at different laser fluences were evaluated. Results indicate that elements emission intensities increased with both laser fluence and spot diameter. Higher intensities for Ca I 442.554, Mg I 277.983, P I 213.618, Al I 309.271, B I 249.773, Cu I 324.755, Fe II 261.187, Mn II 257.610, and Zn II 206.200 nm emission lines were observed with fluences in the 35 - 60 J cm-2 range and spot diameters between 600 and 1050 \'mü\'m. Higher spot diameters improved mass removal and minimized repeatability drawbacks. It was observed that the coefficients of variation (CV) of site-to-site measurements decreased by using higher laser focusing diameters. By fixing the laser spot diameter at 750 \'mü\'m, the CV of measurements improved at least 2-fold for all analytes when 50 J cm-2 was applied in comparison to 20 J cm-2. These results can be attributed to a larger mass removal obtained at higher laser fluences and better laser sampling representativeness. Sensitivity did also increase with laser fluence but no significant differences were observed in the detection limits using 25 and 50 J cm-2. Although emission intensities increased with laser fluence the background emission and noise increased as well. On the other hand, particle size distribution of powdered samples affects the atomization and excitation efficiencies by laser induced plasmas. When larger particles are incompletely vaporized the resulting emission signals were lower than those obtained from smaller particles. In this work, significant improvements on emission intensities and CV of measurements were observed when pellets made with particles < 75 \'mü\'m were analyzed. No significant differences were observed (emission intensities and CV of measurements) in the analysis of pellets prepared with particles in the 20-75 \'mü\'m range. Pellets prepared with particles > 75 \'mü\'m presented cohesion drawbacks and resulted non uniform craters after laser ablation. The CV of measurements for most analytes in these materials was > 15 %. Therefore, similar particle size distribution between calibration and test samples is recommended to avoid physical matrix effects on laser-sample interaction

La technique laser-induced breakdown spectroscopy (LIBS), qui consiste à exploiter le spectre du plasma induit par laser sur la surface de l'échantillon pour déterminer sa composition élémentaire, a été inventée il y a plus de 50 ans. Récemment, elle connaît un développement rapide, poussée par des besoins d'application dans différents domaines, citons par exemple, exploration océanique, détection de pollution environnementale, ou contrôle de procédés industriels. Cette technique utilise le plasma généré par ablation laser comme la source spectroscopique. La particularité de LIBS est que le plasma induit par laser présente un comportement transitoire et une distribution spatiale qui ne soit pas uniforme en général. Bien que la détection résolue en temps puisse améliorer considérablement la performance de LIBS, surtout pour le procédé de LIBS autocalibration avec une meilleure détermination de température, l'évolution temporelle du plasma est souvent corrélée avec sa morphologie et son inhomogénéité spatiale. L'étude de la morphologie ainsi que la structure interne du plasma avec l'évolution pendant l'expansion de celui-ci dans un gaz ambiant, représente donc un point crucial pour l'optimisation du plasma entant qu'une source spectroscopique. Suite à la thèse de Qianli Ma réalisée dans notre équipe et soutenue en décembre 2012, qui a été notamment consacrée à l'étude de l'effet de la longueur d'onde du laser d'ablation sur les propriétés et l'évolution du plasma dans un gaz ambiant d'argon, la présente thèse s'intéresse aux effets des autres paramètres, la fluence du laser d'ablation, la durée de l'impulsion, et les différents gaz ambiants (argon ou air), sur la morphologie et la structure du plasma. Par ailleurs, les mécanismes microscopiques conduisant à l'onde de détonation soutenue par laser dans argon ou dans l'air sont aussi étudiés. Lors du refroidissant du plasma dans l'air, des oxydes métalliques peuvent se former. L'étude de la formation de molécules, au-delà de l'intérêt pratique pour la LIBS, fournit également un aperçu de la cinétique chimique dans le plasma, ce qui est intéressant pour l'étude de la transformation du plasma en phase gazeuse à une phase recondensée de nanoparticules / Laser-induced breakdown spectroscopy (LIBS) has been invented for more than 50 years, which analyzes the spectrum of the laser-induced plasma to determine the elemental composition of the ablated sample. Recently, LIBS technique has been well developed and applied in different domains, for example oceanic exploration, pollution monitoring in the environment. LIBS uses the ablation plasma as a light source that contains the elemental composition information of the sample. However, the laser-induced plasma exhibits a transient behavior. Although time-resolved and gated detection can greatly improve the performance of the LIBS technique especially that of calibration-free LIBS (CF-LIBS) with a better determination of plasma temperature, the temporal evolution of the plasma is correlated to its morphology and its spatial inhomogeneity. The determination of the morphology as well as the internal structure of the plasma together with their evolution during plasma expansion into the ambient gas is therefore crucial for the optimization of the use of ablation plasma as a spectroscopic emission source. Evolutions of the morphology and the internal structure of the ablation plasma are considered as the consequence of its hydrodynamic expansion into the ambient gas. Following the thesis of Qianli Ma which has studied the effect of laser wavelength on the behavior of the plasma induced in an ambient gas of argon, the present thesis has used the same diagnostic techniques (time- and space-resolved emission spectroscopy and fast spectroscopic images) together with 1064 nm ns laser pulse ablation of a target of aluminum to investigate the effects of other parameters, such as the fluence and the duration of laser pulse, the effect of different ambient gases (argon and air), on the morphology and internal structure of the plasma. Furthermore, in order to understand the effects of these parameters on the properties of the plasma, the microscopic mechanisms during post ablation and the propagation of the plasma are also studied. While the plasma cools down in air, molecules are formed, AlO for instance. So the thesis also studied the condition for the formation of the molecules in the plasma. Beyond the practical interest of this study for LIBS, it provides also insights to the kinetics of the AlO molecule formation in laserinduced plasma