A rapid, mask-less deposition technique for writing metal tracks has been developed. The technique was based on laser-induced chemical vapour deposition. The novelty in the technique was the usage of pulsed ultrafast lasers instead of continuous wave lasers in pyrolytic dissociation of the chemical precursor. The motivation of the study was that (1) ultrafast laser pulses have smaller heat affected zones thus the deposition resolution would be higher, (2) the ultrashort pulses are absorbed in most materials (including those transparent to the continuous wave light at the same wavelength) thus the deposition would be compatible with a large range of materials, and (3) the development of higher frequency repetition rate ultrafast lasers would enable higher deposition rates. A deposition system was set-up for the study to investigate the ultrafast laser deposition of tungsten from tungsten hexacarbonyl chemical vapour precursors. A 405 nm laser diode was used for continuous wave deposition experiments that were optimized to achieve the lowest track resistivity. These results were used for comparison with the ultrafast laser track deposition. The usage of the 405 nm laser diode was itself novel and beneficial due to the low capital and running cost, high wall plug efficiency, high device lifetime, and shallower optical penetration depth in silicon substrates compared to green argon ion lasers which were commonly used by other investigators. The lowest as-deposited track resistivity achieved in the continuous wave laser experiments on silicon dioxide coated silicon was 93±27 µΩ cm (16.6 times bulk tungsten resistivity). This deposition was done with a laser output power of 350 mW, scan speed of 10 µm/s, deposition pressure of 0.5 mBar, substrate temperature of 100 °C and laser spot size of approximately 7 µm. The laser power, scan speed, deposition pressure and substrate temperature were all optimized in this study. By annealing the deposited track with hydrogen at 650 °C for 30 mins, removal of the deposition outside the laser spot was achieved and the overall track resistivity dropped to 66±7 µΩ cm (11.7 times bulk tungsten resistivity). For ultrafast laser deposition of tungsten, spot dwell experiments showed that a thin film of tungsten was first deposited followed by quasi-periodic structures perpendicular to the linear polarization of the laser beam. The wavelength of the periodic structures was approximately half the laser wavelength (λ/2) and was thought to be formed due to interference between the incident laser and scattered surface waves similar to that in laser-induced surface periodic structures. Deposition of the quasi-periodic structures was possible on stainless steel, silicon dioxide coated silicon wafers, borosilicate glass and polyimide films. The thin-films were deposited when the laser was scanned at higher laser speeds such that the number of pulses per spot was lower (η≤11,000) and using a larger focal spot diameter of 33 µm. The lowest track resistivity for the thin-film tracks on silicon dioxide coated silicon wafers was 37±4 µΩ cm (6.7 times bulk tungsten resistivity). This value was achieved without post-deposition annealing and was lower than the annealed track deposited using the continuous wave laser. The ultrafast tungsten thin-film direct write technique was tested for writing metal contacts to single layer graphene on silicon dioxide coated silicon substrates. Without the precursor, the exposure of the graphene to the laser at the deposition parameters damaged the graphene without removing it. This was evidenced by the increase in the Raman D peak of the exposed graphene compared to pristine. The damage threshold was estimated to be 53±7 mJ/cm2 for a scanning speed of 500 µm/s. The deposition threshold of thin-film tungsten on graphene at that speed was lower at 38±8 mJ/cm2. However, no graphene was found when the deposited thin-film tungsten was dissolved in 30 wt% H2O2 that was tested to have no effect on the graphene for the dissolution time of one hour. The graphene likely reacted with the deposited tungsten to form tungsten carbide which was reported to dissolve in H2O2. Tungsten carbide was also found on the tungsten tracks deposited on reduced graphene oxide samples. The contact resistance between tungsten and graphene was measured by both transfer length and four-point probe method with an average value of 4.3±0.4 kΩ µm. This value was higher than reported values using noble metals such as palladium (2.8±0.4 kΩ µm), but lower than reported values using other metals that creates carbides such as nickel (9.3±1.0 kΩ µm). This study opened many potential paths for future work. The main issue to address in the tungsten ultrafast deposition was the deposition outside the laser spot. This prevented uniform deposition in successive tracks close to one another. The ultrafast deposition technique also needs verification using other precursors to understand the precursor requirements for this process. An interesting future study would be a combination with a sulphur source for the direct write of tungsten disulphide, a transition metal dichalcogenide that has a two-dimensional structure similar to graphene. This material has a bandgap and is sought after for applications in high-end electronics, spintronics, optoelectronics, energy harvesting, flexible electronics, DNA sequencing and personalized medicine. Initial tests using sulphur micro-flakes on silicon and stainless-steel substrates exposed to the tungsten precursor and ultrafast laser pulses produced multilayer tungsten disulphide as verified in Raman measurements.

[pt] Entender o processo de produção de fuligem é crucial para o projeto de novos queimadores, como os de fornos industriais. Estes queimadores, que utilizam processos de combustão turbulenta, dependem de transferência de calor via radiação das partículas de fuligem para as paredes do forno para seu bom funcionamento. A fuligem formada na região de radiação deve ser oxidada para evitar problemas de saúde e meio ambiente. Mesmo tendo havido significativo progresso no decorrer das duas últimas décadas em relação às chamas laminares, a interação entre a turbulência e a produção de fuligem ainda é um problema em aberto. Este trabalho apresenta resultados experimentais recentes da distribuição instantânea e média da distribuição de fuligem em chamas turbulentas de etileno/ar não prémisturadas estabilizadas em um queimador do tipo bluff-body. A intensidade de turbulência na região de esteira deste queimador é muito alta, levando a uma presença de fuligem intermitente e a estruturas de fuligem altamente distorcidas. A distribuição de fuligem é medida usando incandescência induzida por laser (LII), com uma excitação em 266 nm a 10 Hz e fluência de 0,8 J/cm2 e medição em 400 nm por uma câmera intensificada. Os resultados da técnica LII são comparados à técnica clássica de extinção da luz. Resultados da distribuição de hidrocarbonetos aromáticos policíclicos também são apresentados. Os resultados obtidos permitem caracterizar a distribuição da função de densidade de probabilidade de fuligem. Nas situações de escoamento onde a turbulência da esteira é controlada pelo escoamento de ar, demonstra-se que a PDF da fração volumétrica de fuligem corresponde a uma distribuição lognormal. / [en] Understanding the soot production process is crucial to the design of new burners, such as those in industrial furnaces. Indeed, these burners, which use turbulent combustion processes, rely on radiative heat transfer from the soot particles to the furnace walls to operate properly. The soot formed within the radiation region must the be oxidized in order to avoid health and environment issues. Although there has been significant progress over the past two decades in relation to laminar flames, the interaction between turbulence and soot production is still an open problem. This works presents recent experimental results of the instantaneous and mean soot distribution on non-premixed turbulent ethylene/air flames stabilized at a bluff-body burner. The turbulence intensity in the wake region of this burner is very high, leading to a soot intermittent presence and to highly distorted soot structures. The soot distribution is measured using laserinduced incandescence (LII), with 266 nm excitation at 10 Hz, 0.8 J/cm2 fluence and collected at 400 nm by an intensified camera. The results of the LII technique are compared to those of a classical of light extinction technique. Polyciclic aromatic hydrocarbon distribution results are also presented. The results obtained allow to characterize the soot probability density function distribution. In flow situations where the wake turbulence is controlled by the air flow, the soot volume fraction PDF is shown to correspond to a lognormal distribution.

The laser beam interaction with matter and the plasma generation have been studied for many years. In some applications what is really important is to understand the composition and the temporal evolution of the species in the interested medium. In this thesis, time resolved optical spectroscopy was employed to understand the evolution of the plasma which is produced by interaction of Infrared (1.064 &micro / m) laser beam with air. In this thesis, a new technique is suggested to analyze the time evolution of laser induced breakdown spectroscopy. The suggested method and the instrumentation of the setup are tested with a single gas (He). After the tests, we analyzed time sequence spectra of Laser Induced Air Breakdown. The suggested method is based on triggering the laser and the spectrometer at different time and applying the spectrometer trigger time by adding the time delay (&amp / #916 / t) between them by using the pulse generator. The results show that the decay rates are slowing down microseconds after the excitation of the plasma. The results of the time-resolved measurements of the line spectra show that different component of the air has different decay rate, and lifetime. The lifetime of helium is 20 &micro / s, and the decay start 5 &micro / s after the initiation of plasma. Air has 12 &micro / s lifetime, and the decay start 3 &micro / s after the initiation of the plasma. Also, the decay rate and the lifetime depend on the state. We also calculate Doppler velocity for different component and different emission states. Doppler velocities show that the component which has great mass has small velocity, the component which has small mass has high velocity.

This PhD work was devoted to the understanding of the laser-induced plasma on organic materials and theapplication of laser-induced breakdown spectroscopy (LIBS) to quantitative analysis of these materials. Itcontributes to deepen our knowledge on the physical mechanisms involved in laser-matter interaction, plasmageneration, evolution and expansion of the plasma into the ambient gas, with emphasis on plasmas induced onorganic targets. It also intends to improve the performance of LIBS for the analysis of organic materials. Thespecificity for organic targets fits the current focus of the international community working on LIBS, toimprove the control of the plasma induced on this kind of material which has a distinguished optical prosperitywith respect to that of metals, better known for laser ablation. It addresses also the growing need to apply theLIBS technique to organic materials for different applications in the environmental, food, or biomedicaldomains. The works in this thesis were therefore presented in this thesis document according to the followingorganization.After the General Introduction which introduces the scientific and technological contexts, Chapter Irecalls the basic theoretical elements necessary to understand the phenomenon of plasma generation by laserablation, and its evolution in the background gas. Ablation of organic material is emphasized. Procedures andtechniques of diagnostics of laser-induced plasma were then presented with a focus on the transient andinhomogeneous nature of the expanding plasma. Chapter II focuses on the generation and the evolution of theplasma induced on the skin of a potato, a typical sample of agricultural product. The characteristics of plasmainduced on a soft and wet organic target, such as a fresh potato, was something unknown when the thesis workstarted. These characteristics provide the necessary basis for the quantitative analysis of the trace andultra-trace metallic elements in these samples. Following this characterization, semi-quantitative analyticalresults were extracted from LIBS spectra corresponding to potato skin. Chapter III is presented in thecontinuity of Chapter II for the application of LIBS to the quantitative analysis of organic materials. Acomparative study on the analytical results with LIBS and ICP-AES for milk powders allows an assessment ofthe performances of quantitative analysis by LIBS for organic materials, and a validation of the CF-LIBSprocedure that we have developed. Different from Chapters II and III where attention was paid to trace metalelements, Chapter IV studies the behavior of the major elements that make up the matrix of organic material,which are 4 known organic elements: H, C, O, N. During the decomposition of organic material by laserablation, these elements can be found in the form of molecular fragments, or recombined into molecularspecies. We then study in this Chapter the evolution of these species as a function of the laser ablationparameters, the laser wavelength in particular. The thesis document ends with a general conclusion andoutlooks.

Combustion-generated carbon black nano particles, or soot, have both positive and negative effects depending on the application. From a positive point of view, it is used as a reinforcing agent in tires, black pigment in inks, and surface coatings. From a negative point of view, it affects performance and durability of many combustion systems, it is a major contributor of global warming, and it is linked to respiratory illness and cancer. Laser-Induced Incandescence (LII) was used in this study to measure soot volume fractions in four steady and twenty-eight pulsed ethylene diffusion flames burning at atmospheric pressure. A laminar coflow diffusion burner combined with a very-high-speed solenoid valve and control circuit provided unsteady flows by forcing the fuel flow with frequencies between 10 Hz and 200 Hz. Periodic flame oscillations were captured by two-dimensional phase-locked LII images and broadband luminosity images for eight phases (0°- 360°) covering each period. A comparison between the steady and pulsed flames and the effect of the pulsation frequency on soot volume fraction in the flame region and the post flame region are presented. The most significant effect of pulsing frequency was observed at 10 Hz. At this frequency, the flame with the lowest mean flow rate had 1.77 times enhancement in peak soot volume fraction and 1.2 times enhancement in total soot volume fraction; whereas the flame with the highest mean flow rate had no significant change in the peak soot volume fraction and 1.4 times reduction in the total soot volume fraction. A correlation (ƒv Reˉ1 = a+b· Str) for the total soot volume fraction in the flame region for the unsteady laminar ethylene flames was obtained for the pulsation frequency between 10 Hz and 200 Hz, and the Reynolds number between 37 and 55. The soot primary particle size in steady and unsteady flames was measured using the Time-Resolved Laser-Induced Incandescence (TIRE-LII) and the double-exponential fit method. At maximum frequency (200 Hz), the soot particles were smaller in size by 15% compared to the steady case in the flame with the highest mean flow rate.

No description available.

No description available.

Tsunami are a very dangerous natural hazard, as highlighted in recent years by the Indian Ocean Tsunami of 2004 and the Japan Tsunami of 2011. In the last decade, tsunami have claimed hundreds of thousands of lives, and caused billions of dollars in damage around the world. The hazard posed to coastal communities by tsunami is expected to increase in the future, due to population growth, intensification of coastal development and sea level rise due to climate change. Tsunami may be generated by a number of different source mechanisms. One such source mechanism is a submarine landslide, which can occur in a number of marine environments containing significant sediment accumulation on a sloping seafloor. The high amplitudes and rapid celerities of landslide-generated tsunami make them very dangerous to communities in the vicinity of the landslide, although these waves do not possess the potential for transoceanic devastation. The objectives of this research project are to carry out a series of two-dimensional physical experiments investigating the waves generated by a rigid block landslide moving along a horizontal boundary. The use of a horizontal boundary has the advantage that waves propagating in the offshore and onshore directions may be measured (unlike previous studies using sloping boundaries). The landslide motion is provided by a mechanical system, allowing testing of a broad range of motion, and isolation of the wavemaking properties of different phases of landslide motion. Experiments are carried out in a 14.66 m long flume, with width 0.25 m and working depth 0.50 m. A false floor installed in the flume provides the sliding surface for the landslide motion, and houses the mechanical system. A series of preliminary particle tracking velocimetry experiments confirm the ability of the mechanical system to achieve its velocity targets to within 5% or better, depending on the parameters of the landslide motion. Full spatial and temporal resolution of the wave field is achieved using a laser-induced fluorescence technique to identify the air-water interface to sub-pixel accuracy. The measurements obtained using laser-induced fluorescence are validated against measurements from a resistance wave gauge, with sub-millimetre agreement. In an additional experiment, the particle tracking velocimetry technique provides measurements of the subsurface velocity field. The landslide motion during all experiments consists of an initial period of constant acceleration, followed by a period of constant velocity, followed by a deceleration to rest (at the same rate as the initial acceleration). The landslide acceleration generates two dispersive packets of waves, travelling in the offshore and onshore directions. The offshore-propagating wave packet contains a leading crest and the onshore-propagating wave packet contains a leading trough, with both waves approaching the shallow water limit. A free surface depression forms above the landslide during its constant-velocity motion, and its amplitude may be predicted to within approximately 20% using standard hydraulic theory (considering a frame of reference moving with the landslide). The offshore-propagating waves passing over the landslide cause the amplitude of this depression to fluctuate over time. The deceleration of the landslide generates two additional packets of waves with the opposite polarity to the waves generated by the landslide acceleration. The full spatial and temporal resolution of the generated wave field allows the calculation of the potential energy within the wave field. Additionally, the energy (and mass) within the onshore- and offshore-propagating wave packets may be estimated by calculating these quantities within the onshore and offshore regions of the experimental domain. The wave packets generated by the initial landslide acceleration transport positive mass in the offshore direction, and negative mass in the onshore direction. This mass transport is balanced by the waves generated during the deceleration of the landslide. The nondimensional landslide acceleration, landslide Froude number and submergence depth are varied during the physical experiments. The landslide Froude number has the greatest effect on the behaviour of the generated wave field. At low Froude numbers, the wave field is dominated by the waves generated by the acceleration and deceleration of the landslide. As the Froude number increases, the onshore-propagating waves become negligible in amplitude compared to the offshore-propagating waves. Additionally, the free surface depression increases in amplitude and a group of short-wavelength waves become trapped behind the landslide. These waves exhibit highly nonlinear behaviour at landslide Froude numbers greater than 0.5. The simple experimental geometry allows comparison between the measured wave fields with the predictions of three mathematical models. Two inviscid-irrotational models, differing in their treatment of the bottom boundary condition, provide comparisons over the entire parameter space. These models under-predict the amplitudes of the generated waves, and fail to correctly predict the ongoing interaction between the landslide and the offshore-propagating waves. The inclusion of bottom boundary nonlinearity improves the predictions of the amplitude of the leading waves, and the potential energy within the wave field. However, both of the inviscid models do not predict the extent of wave trapping behaviour behind the landslide observed in the experiments. A viscous model, formulated in the DNS solver Gerris, improves the predictions of wave trapping (and amplitude in general) in one experiment. Although the model still under-predicts the amplitudes of the generated waves, it correctly predicts the amplification of the waves behind the landslide during its constant-velocity motion. The failure of the inviscid models to predict the amplitudes of these waves can be mostly attributed to the linearised free surface condition used by both models. The presence of the turbulent wake may also have a secondary effect on these predictions. An extension of the linear inviscid-irrotational model to three dimensions allows the effect of the landslide width on the amplitudes of the generated waves to be determined. As the width increases, the behaviour of the waves approaches the two-dimensional limiting case.

The field of lipidomics encompasses the study of pathways, networks, and functionality of cellular lipids in biological systems. The lipid subclass, primary fatty acid amides, are crucial to nervous system signaling, receptor function, and numerous other physiological roles. Chapter 1 details these bioactive properties of several well-studied primary fatty acid amides as well as their biosynthesis, degradation, and most common analysis techniques. As these bioactive lipids are endogenously present in trace and ultra-trace abundancies, the field of microfluidics presents an attractive alternative analysis system to incorporate minimization of sample and reagent usage, analysis cost reduction, highly sensitive detection pairing, and decreased analysis time, all while limiting sample handling. Chapter 2 provides a microfluidics-based review of common device fabrication techniques, droplet microfluidics, and detection systems. Current primary fatty acid amide analysis techniques have detection limits on the periphery of endogenous concentrations, presenting the need for a more sensitive detection system, such as fluorescence. Chapter 3 serves as the foundation in developing methodology to analyze these amides and their conjugate fluorescently-tagged primary amines. Chapter 4 focuses on the development of a microfluidic platform capable of efficient on-chip fluorescent tagging reactions and the coupling of a highly sensitive laser induced fluorescence detection system capable of detection limits several orders of magnitude lower than currently employed mass spectrometry techniques. In addition, the appendix details the method development for the quantitative analysis of the anti-inflammatory and anti-cancer drug, celecoxib, uptake into novel drug delivery vehicles. / Bayer School of Natural and Environmental Sciences; / Chemistry and Biochemistry / PhD / Dissertation;

Doctor of Philosophy / Department of Chemistry / Christopher T. Culbertson / Recent approaches in analytical separations are being advanced towards the “lab-on-a-chip” concept in which multiple lab functions are integrated into micro/nano fluidic platforms. Among the variety of separation techniques that can be implemented on microfluidic devices, capillary electrophoresis is the most popular as it provides high efficiency, simple, fast and low cost separations. In addition, integrating miniaturized fluid manipulation tools into microfluidic devices with separations is essential for a variety of biological applications. Chapter 1 discusses the fundamentals of capillary electrophoresis and miniaturized fluid manipulation tools and provides an over view of single cell analysis in microfluidics. In chapter 2, the integration of miniaturized peristaltic pumps into multilayer microfluidic platforms is discussed. In addition, device characterization, precise fluid control and high throughput single cell analysis are discussed. As a proof of principle, T-lymphocytes were loaded with two fluorescent probes Carboxyfluorescein diacetate (CFDA) and Oregon green (OG). Thousands of single cells were automatically transported, lysed on these devices and analytes from the lysate were electrophoretically separated. 1120 cells were analyzed over the course of 80 min (14 cells/min) and separation characteristics of analytes released from individual cells were investigated. In the third chapter, the development of microfluidic platforms for the electrochemical detection of nitric oxide (NO) and other reactive nitrogen species (RNS) at the single cell level is discussed. A microfluidic system was developed to perform rapid cell lysis followed by electrochemical detection. Miniaturized microband electrodes were designed and integrated with a microfluidic separation channel. Three alignment techniques (in-channel, end-channel and off-channel configurations) were used to detect the electrochemical response of the analyte of interest. Furthermore, a model analyte (CFDA) was used to demonstrate the potential of performing the simultaneous dual detection with electrochemical and laser induced fluorescence detection. In addition, the same microfluidic platform was adapted to detect intracellular superoxide using laser induced fluorescence. In the fourth chapter, the off-chip integration of optical fiber bridges with multilayer microfluidic chips is discussed. A multimode optical fiber (~10cm long) was integrated between the single cell lysing spot and a spot downstream of the separation channel in order to detect both intact cells and the analyte in the lysate. This technique was used to create two detection spots on the microfluidic platform with the use of a single excitation source and single detector. Fluorescently labeled T-lymphocytes were automatically transported and lysed in a manner similar to that described in chapter 2. Hundreds of single cells were analyzed and the absolute migration time was determined for the analytes in the lysate. In addition, the separation characteristics of fluorescently labeled protein kinase B peptide substrates were investigated. Furthermore, this technique was used to measure cell size and the velocity of intact cells (discussed in 5th chapter) by making use of a light tunneling concept available in multimode optical fibers. All the experiments presented in this dissertation exploit the use of multilayer microfluidic platforms to investigate intracellular components in single cells in a high throughput manner that has several advantages over current conventional techniques.