Este trabalho teve como objetivo avaliar o uso do método das médias móveis na atomização de cádmio, crômio e chumbo utilizando filamento de tungstênio de 150 W (OSRAM) como atomizador eletrotérmico. Realizou-se um estudo sistemático da influência da altura de observação, da temperatura e taxa de aquecimento na atomização dos analitos e a viabilidade do uso do método das médias móveis no tratamento dos sinais transientes gerados na atomização. O estudo da influência da altura de observação foi realizado posicionado-se o filamento no centro (0 mm), 1 e 2 mm abaixo do feixe de radiação. A influência da temperatura e da taxa de aquecimento foi estudada utilizando temperaturas na etapa de atomização entre 1890 e 2780 °C. O método das médias móveis foi aplicado aos sinais transientes gerados na atomização, com o filamento posicionado no centro (0 mm), 1 e 2 mm e com temperatura de atomização entre 2060 e 2780 °C, utilizando fatores 0, 3, 5, 7 e 9. No estudo da temperatura e da taxa de aquecimento foram aplicadas ddps no software de controle na etapa de atomização entre 4 e 12 V. As soluções usadas no desenvolvimento deste trabalho foram preparadas em meio 0,1 % v/v HNO3. Utilizou-se como gás de proteção a mistura de 90% Ar+10 % H2. Para o cádmio, recomenda-se a utilização da altura de observação de 1 mm, para o chumbo recomenda-se 0 mm e para o crômio a altura recomendada é a de 2 mm. Os estudos comprovaram a dependência dos sinais de absorção atômica em altura de pico com a temperatura e a taxa de aquecimento. O cádmio foi o analito em que a taxa de aquecimento foi a menos crítica para a atomização, enquanto que o crômio foi o mais afetado pela variação da taxa de aquecimento. Não foi observada diferença significativa entre os sinais de cádmio com alturas de observação de 0 e 1 mm. Para o chumbo, a diferença entre os sinais com altura de observação de 0 e 1 mm foi constante em todas as taxas de aquecimento estudadas. A 2 mm a diferença entre os sinais aumentou com o aumento da taxa de aquecimento. Para o crômio, não ocorreu uma diferença significativa entre os sinais nas alturas de 1 e 2 mm com atomização até 2180 °C. Nos três analitos a sensibilidade aumentou com o aumento da taxa de aquecimento. O método das médias móveis permitiu a diminuição da variação dos sinais transientes do branco e do ruído. Para o cádmio, não ocorreu uma melhora no limite de detecção do método com a aplicação das médias móveis em nenhuma condição. Para o chumbo e crômio, ocorreu uma melhora no limite de detecção do método nas alturas de observação de 0 e 1 mm. O limite de detecção instrumental apresentou uma melhora significativa para os três elementos em todas as condições estudadas. / The aim of this paper was to evaluate the use of moving averages of cadmium, chromium and lead transient atomic absorption signals generated by 150 W (OSRAM) tungsten coil electrothermal atomizer. A systematic study dealing with the influence of observation height, temperature and heating rate on atomization was carried through in order to demonstrate the viability of moving averages in the treatment of the transient signals during the atomization step. The influence of observation height was carried out with the tungsten coil in the center (0 mm), at 1 and 2 mm below the radiation beam. The influence of atomization temperature and heating rate were evaluated between 1890 °C (3.3 K.ms-1) and 2780 °C (9,3 K.ms-1). The transient moving averages were obtained by using factors 0, 3, 5, 7 and 9, with the tungsten coil in the center (0 mm), 1 and 2 mm and with atomization between 2060 and 2780 °C. For obtaining different temperatures and heating rates, an appropriate power supply was used by applying 4 to 12 V (40 to 120 W) to the atomizer during atomization and a mixture 90% Ar+10% H2 was used as purge/atomization gas. Blanks and reference solutions were prepared in 0,1% v/v HNO3. Best results for cadmium were obtained at 1 mm. For lead it is recommended 0 mm and for chromium 2 mm. The studies had proven the dependence of peak height absorbance signals with temperature and heating rate. Cadmium was the analyte where the heating rate was to less critical for the atomization, whereas chromium was affected by the variation of the heating rate. Significant differences were not observed between cadmium signals with observation heights of 0 and 1 mm. For lead, the difference between the absorbance signals with observation heights of 0 and 1 mm were constant in all tested heating rates. At 2 mm the difference between signals increased by increasing the heating rates. For chromium, a significant difference was not noticed between peak height absorbance signals at 1 and 2 mm with up to 2180 °C. As expected, sensitivity increased for all three analytes by increasing the heating rate. The moving average is a powerful mathematical treatment for minimizing unpredictable fluctuations of the base line during the chosen time interval for measuring the transient absorbance signals. With the exception of Cd, where no improvements on the method detection limit were noticed, the application of the moving average for the lead and chromium showed 3 to 4 fold improvement in the LDmet at 0 and 1 mm observation heights, respectively. The LDinstr presented a significant improvement (3 to 6 fold) for the three analytes in all studied conditions.

Este trabalho teve como objetivo avaliar o filamento de tungstênio de 150 W (OSRAM) como atomizador eletrotérmico para determinação de alumínio em amostras de águas, incluindo um estudo sistemático sobre o seu comportamento eletrotérmico na presença de até 1000 mg l-1 de sódio, potássio, cálcio, magnésio e/ou da mistura destes elementos. Alguns parâmetros, como comprimento de onda, corrente da lâmpada de catodo oco, altura de observação e temperatura de atomização do alumínio foram avaliados visando à melhoria da qualidade dos resultados e do limite de detecção. Após uma primeira avaliação, fixaram-se o comprimento de onda em 309,3 nm e a corrente da lâmpada de catodo oco em 10 mA, elegendo-se altura de observação de 1,5 mm e temperatura de atomização de 2860 oC (13,0 V). No programa de aquecimento usado no desenvolvimento deste trabalho adotou-se rampa invertida de voltagem variando entre 0,65 a 0,30 V durante 50 s para secagem de 10 µl, 2,8 V durante 10 s para pirólise e 13,0 V durante 1 s para atomização. As soluções usadas no desenvolvimento deste trabalho formam preparadas, em sua maioria, em meio 0,1 % v/v HNO3. A avaliação dos potenciais interferentes Na, K, Ca, Mg e a mistura desses elementos foi realizada nas alturas de observação de 0,0 a 2,0 mm e nas composições do gás de proteção de 90% Ar/10% H2, 80% Ar/20% H2, 65% Ar/35% H2. Pode-se inferir que o aumento do hidrogênio na composição do gás de proteção não acarretou melhora significativa na ação dos interferentes na atomização do alumínio. Não foram observadas interferências significativas em até 1000 mg l-1 Na e K na atomização de 100 µg l-1 Al na altura de observação de 0,0 mm. Na mesma condição de altura de observação, a mistura dos interferentes não afetou significativamente a atomização do alumínio. Observaram-se interferências em torno de 40 % na atomização de 100 µg l-1 Al em 0,1 % v/v HNO3 na altura de observação de 0,0 mm na presença de até 100 mg l-1 de Ca e Mg. Nessa mesma condição, mas com a mistura 65 % Ar/35 % H2, a supressão do sinal de absorbância de alumínio foi da ordem 90%. Os resultados obtidos na determinação de alumínio em amostras de água foram obtidos nas condições anteriormente citadas, utilizando gás de proteção 90% Ar/ 10% H2. Nestas condições, o limite de detecção foi de 2,3 µg l-1 Al e a massa característica de 69 pg Al. Os resultados encontrados foram satisfatórios e concordantes com aqueles encontrados quando se utilizou o forno de grafite como método de comparação. Aproximadamente 500 queimas foram feitas com um único filamento de tungstênio. / The aim of this paper was to evaluate the 150 W (OSRAM) tungsten coil as electrothermal atomizer in order to determine aluminum in water samples as well as a systematic study of its electrothermal behavior in the presence of up to 1000 mg l-1 of sodium, potassium, calcium, magnesium and/or of mixture of these elements. Some parameters, such as wavelength, hollow cathode lamp current, observation height and atomization temperature were evaluated in order to improve the quality of results and the detection limit. After a first evaluation, measurements were always carried out at 309,3 nm as well as the hollow cathode lamp current at 10 mA, and it was adopted an observation height of 1,5 mm and atomization temperature at 2860 oC (13,0 V). In the heating program defined experimentally, the inverted voltage ramp was adopted for drying 10 μl of sample solution by varying the applied voltage from 0,65 to 0,30 V during 50 s, with further application of 2,8 V for 10 s in the pyrolysis step and 13,0 V for 1 s in the atomization step. Most solutions were prepared in 0,1% v/v HNO3. The evaluation of the potential interfering elements such as Na, K, Ca, Mg an the mixture of these elements, was carried out in observations heights from 0,0 to 2,0 mm at different gas compositions: 90% Ar/ 10% H2 , 80 % Ar/ 20% H2 and 65 % Ar/ 35% H2. It can be inferred that the hydrogen increase in the protection gas did not change the interference behavior of the studied concomitants on aluminum atomization. Significant interferences were not observed up to 1000 mg l-1 of Na and K in the atomization of 100 μg l-1 Al when the optical beam was intercepting the atomizer (0,0 mm observation height). In the same condition, the mixture of the interfering species did not significantly affect the aluminum atomization. In addition, 100 mg l-1 of Ca and Mg depressed the absorbance of 100 μg l-1 Al in 0,1 % v/v HNO3 by approximately 40 %. When the atomization was made in the presence of 65 % Ar/ 35 % H2, the suppression of the aluminum absorbance signal was about 90 %. The results obtained in the determination of aluminum in water samples were achieved in the conditions previously mentioned, using protection gas of 90 % / 10 % H. In these conditions, the detection limit was 2,3 μg l-1 Al and the characteristic mass was 69 pg Al. The results were reasonable and in agreement with those found by atomic absorption with graphite furnace as a comparative method. Approximately 500 firings were made with a single tungsten coil.

<p>Microfluidics has established itself as a key technology in a wide range of fields including pharmaceuticals, point-of-care diagnostics, thermal management, and space technology. Most of these applications involve manipulation of small quantities (micro – nanoliters) of fluids and various particles or biological cells suspended in them. These platforms employ mechanical, thermal, acoustic, magnetic, optical, electric and many other means for creating particle and fluid motion. Many biological applications require handling cells that are vulnerable to getting damaged if proper physiological conditions are not maintained or if excessive force is applied on them. The non-invasive nature of optical and electrical micro-manipulation techniques such as rapid electrokinetic patterning (REP) has proven to be of great importance in such applications. These techniques enable handling, transportation, sorting and arrangement of fragile synthetic micro/nanoparticles and biological cells without compromising their structure and surface properties.</p> <p>REP is a recently developed micro-manipulation tool that employs optically induced electrothermal vortices to create custom flow patterns. Particle suspensions are entrained in these vortices and are trapped on an electrode surface through AC electrokinetic mechanisms. This work focuses on characterizing a REP trap and discusses its potential applications in handling biological cells. Polystyrene microparticles are confined in a REP trap and a MATLAB program is used to track their motion inside the trap. The tracked particle trajectory reveals that the potential energy of the trapped particle is parabolic and hence the trap is Hookean in nature. The trap is modelled as a spring-mass system and the stiffness coefficient of that system is found to be of the order of 10^-15 N/μm. The origin of the restoring force in the spring-mass model is found to be the drag force created by the electrothermal vortex. The ability to exert ultra-small forces in a stable trap enables REP to be used in various non-invasive particle manipulation applications.</p> <p>The transient nature of REP is studied using numerical modeling and particle image velocimetry (PIV) analysis of a vortex created by a moving laser spot. A numerical model suggests that custom-shaped steady state REP vortices can be created via superposition of multiple axisymmetric circular shaped vortices. However, the method of superposition cannot be extended to transient traps and a more involved 3D model is required to simulate them. The laser spot is scanned back-and-forth in a line with different speeds to create transient REP vortices. The PIV analysis, in agreement with the numerical model, shows that the location of the moving vortex is undiscernible at high speeds. Moreover, the circular shaped vortex is stretched out into a line when the laser scanning frequencies are more than 15 Hz.</p> <p>The particle-electrode attraction force, which entraps the particles at the electrode surface, is characterized using particle diffusometry (PD) and defocusing particle tracking. PD is used to measure the diffusion coefficient of polystyrene particles under different electric field parameters near an electrode surface. It is found that the particle diffusivity decreases with a decrease in the electric field frequency from 150 – 30 kHz and with an increase in the applied voltage from 4 – 8 V_pp. A MATLAB program is used to track the number of in-focus particles and their distance from the electrode surface. A histogram of the particles’ distance from the electrode surface shows an increase in the particle concentration near the electrode at low frequencies (30 – 60 kHz). These observations suggest that the average height of an entrapped particle decreases with a decrease in applied field frequency and an increase in applied voltage. This suggests that the attractive trapping force is significant at 30 kHz but diminishes at around 150 kHz.</p> <p>Salt and sugar-based isotonic media used for cell suspensions pose several challenges for electrokinetic mechanisms such as REP. Various solutions to overcome these challenges for bio-manipulation applications are discussed in this work. The presence of DC offset in the AC electric field is found to enhance particle entrapment in sugar-based media. The effect of DC offset on trapping performance in bio-relevant media is assessed by measuring the stability of the REP trap. This work also shows entrapment and manipulation of Mice pancreatic cancer cells (KPC2) suspended in the sugar-based isotonic media using REP. The biological applications of the REP technology are highly promising, but they have not yet been well-explored. This work lays the foundation of understanding how REP can be operated in high osmolarity media for bio-manipulation applications.</p>

Future magnetic fusion reactors such as tokamaks will need innovative, fast, deep-fueling systems to inject frozen deuterium-tritium pellets at high speeds and high repetition rates into the hot plasma core. There have been several studies and concepts for pellet injectors generated, and different devices have been proposed. In addition to fueling, recent studies show that it may be possible to disrupt edge localized mode (ELM) formation by injecting pellets or gas into the fusion plasma. The system studied is capable of doing either at a variety of plasma and pellet velocities, volumes, and repetition rates that can be controlled through the formation conditions of the plasma. In magnetic or inertial fusion reactors, hydrogen, its isotopes, and lithium are used as fusion fueling materials. Lithium is considered a fusion fuel and not an impurity in fusion reactors as it can be used to produce fusion energy and breed fusion products. Lithium hydride and lithium deuteride may serve as good ablating sleeves for plasma formation in an ablation-dominated electrothermal plasma source to propel fusion pellets. Previous studies have shown that pellet exit velocities, greater 3 km/s, are possible using low-z propellant materials. In this work, a comprehensive study of solid lithium hydride and deuteride as a pellet propellant is conducted using the ETFLOW code, and relationships between propellants, source and barrel geometry, pellet volume and aspect ratio, and pellet velocity are determined for pellets ranging in volume from 1 to 100 mm3. / Master of Science

No description available.

Recent concepts for controlled magneto-inertial fusion (MIF), such as magnetized liner inertial fusion (MagLIF), have suffered from magnetohydrodynamic (MHD) instabilities that lead to degradations in fusion yield. High levels of azimuthally-correlated MHD instability structures have been observed on cylindrical liner experiments without a pre-imposed axial magnetic field (Bz=0) elsewhere in the literature and are believed to be seeded from surface machining roughness. This dissertation uses highly resolved (0.5 μm and less resolution) 1D and 2D resistive magnetohydrodynamics (MHD) arbitrary-Lagrangian-Eulerian (ALE) simulations of electrical wire explosions (EWEs) and liner implosions to show that micrometer-scale surface roughness seeds the electrothermal instability (ETI), which induces early melting in pockets across the conductor and leads to millimeter-scale instability growth. The relationship between the ETI and the MRTI in liner implosions is also described in this dissertation, which shows that the traditional growth rates associated with these modes are coupled together and are not linearly independent. This dissertation also describes the preliminary implementation of a Koopman neural network architecture for learning the nonlinear dynamics of a high energy density (HED) exploding or imploding electrical conductor. / Doctor of Philosophy / Researchers have been working on controlling nuclear fusion and harnessing it as a power source since the discovery that nuclear fusion powers stars. In many of these controlled nuclear fusion concepts the aim is to heat the fuel until it forms a high-temperature plasma state of matter and then compress it to the point that the atoms are close enough and at high enough speeds that they collide fuse together. In the magnetized liner inertial fusion (MagLIF) concept these temperatures, densities, and pressures are achieved by surrounding the fusion fuel with a cylindrical piece of metal called a liner and using magnetic fields to implode the liner inward. Experiments have shown, however, that these liner implosions do not occur smoothly and that the system becomes unstable and can mix liner material into the fuel, which disrupts the fusion process. This dissertation investigates the stability of liner implosions and electrical wire explosions. In particular, this dissertation shows that surface roughness imparted on the surface of a solid fusion target by a machining process can grow into a millimeter-scale perturbation. It also describes the relationship between two common types of instabilities found in current-driven nuclear fusion: the magneto-Rayleigh-Taylor instability and the electrothermal instability. Finally, it looks at using neural networks to better understand the dynamics of electrical wire explosions.

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / This work presents an LED electrothermal design methodology applied to a street lighting system. The methodology aims to provide indicatives of the optimal LED operating point for lighting systems design, considering electrical, thermal and photometric system features. Different projects are developed according to the methodology, the theoretical results are compared with fluid dynamics simulation and demonstrated by experimental results. A research including luminous flux, luminous efficacy and flicker is performed considering the LED current ripple, defining acceptable levels of ripple based on the optimal operational point. The methodology is applied by developing a lighting system composed of an LED driver and a thermal dissipation system, comprising a luminaire, a heatsink and fans. The lighting system includes electrothermal feedback control. The results provide high power factor with low current harmonic distortion to the power grid. The LED operational temperature ensures the luminous flux maintenance over the system lifetime. / Este trabalho apresenta uma metodologia de projeto eletrotérmico de LEDs aplicada a um sistema de iluminação pública. A metodologia tem o objetivo de proporcionar indicativos do melhor ponto de operação do LED para o projeto de sistemas de iluminação, considerando os aspectos elétricos, térmicos e fotométricos envolvidos no sistema. Diferentes projetos são desenvolvidos utilizando a metodologia, os resultados teóricos obtidos são comparados com simulações computacionais de dinâmica dos fluidos e comprovados através de resultados experimentais. Um estudo do fluxo, eficácia e cintilação luminosa é também realizado considerando a ondulação de corrente aplicada aos LEDs, definindo os níveis aceitáveis de ondulação com base no ponto ótimo de operação. Para aplicação da metodologia é desenvolvido um sistema de iluminação pública composto por um circuito de acionamento dos LEDs e um sistema de dissipação térmica, formado por uma luminária, um dissipador de calor e ventiladores. O sistema de iluminação possui controle com realimentação eletrotérmica. Os resultados obtidos proporcionam alto fator de potência com baixa distorção harmônica ao sistema elétrico e temperatura de operação que garante a manutenção do fluxo luminoso dos LEDs durante toda a vida útil do sistema.

In this diploma thesis, rubidium in plant material samples was determined by atomic absoption spectrometry. Determination of plant material rubidium was performed on two different atomic absorption spectrometers (GBC 933 AA and ContrAA 700) for comparison. The selection of a proper method of atomization was essential, therefore optimizations for the flame atomizer and electrothermal atomizer were performed. On the GBC 933 AA, flame atomization was tested. The flow rate of the acetylene-air, vertical and horizontal flame profile, spectral interval width was optimized for the instrument. On the ContrAA 700, the conditions for flame atomization were optimized as well as for electrothermal atomization. The optimized parameters included the acetylene-air flow rate and the vertical flame profile again. For the electrothermal atomization, the temperature dependence of pyrolysis and the temperature dependence of atomization were optimized. Under experimentally determined optimal conditions, the determination of rubidium in fruit and vegetable juice samples was performed by the method of calibration curve. Rubidium usually accompanies toher alkali metals. In the absence of essential biogenic elements iportant for plant growth, rubidium is able to help out and take on the role of potassium.

In the development of a nonlinear transistor model, several measurements are used to extract equivalent circuit parameters. The current-voltage (IV) characteristic of a transistor is one of the measurement data sets that allows the nonlinear model parameters to be extracted. The accuracy of the IV measurement greatly influences the accuracy of the large-signal model. Numerous works have reported the inadequacy of traditional static DC IV measurements to accurately predict radio-frequency (RF) behavior for many devices. This inaccuracy results from slow processes in the device that do not have time to completely respond to the quick changes in terminal conditions when the device is operating at high frequencies; however, these slow processes respond fully to reach a new steady-state condition in the DC sweep measurement. The two dominant processes are self-heating of the device and changes in trap occupancy. One method of allowing the thermal and trap conditions to remain in a state comparable to that of RF operation is to perform pulsed IV measurements to obtain the IV curves. In addition, thermal correction can be used to adjust the IV curves to compensate for self-heating in the case that the predominant effect in the device is thermal. To gain a better understanding of pulsed IV measurement techniques, measurement waveforms of a commercially available pulsed IV analyzer are examined in the time domain. In addition, the use of bias tees with pulsed IV measurement is explored; such a setup may be desired to maintain stability or to enable simultaneous pulsed S-parameter and pulsed IV measurement. In measurements with bias tees, the pulse length setting must be long enough to allow the voltage across the inductor to change before the measurement is made. In many circumstances, it is beneficial to compare different sets of IV curves for a device. The comparison of pulsed and static IV measurements, measured and modeled IV measurements, as well as two measurements with identical settings on the same instrument (to ascertain instrument repeatability) can be performed using the proposed normalized difference unit (NDU). This unit provides a comparison that equally weights the two sets of data to be compared. Due to the normalization factor used, the value of the NDU is independent of the size of the device for which the IV curves are compared. The variety of comparisons for which this unit can be used and its ability to present differences quantitatively allow it to be used as a robust metric for comparing IV curves. Examples of the use of the NDU shown include determination of measurement repeatability, comparison of pulsed and static IV data, and a comparison of model fits. The NDU can also be used to isolate thermal and trapping processes and to give the maximum pulse length that can be used for pulsed IV measurement without contamination by each of these processes. Plotting the NDU comparing static and pulsed IV data versus pulse length shows this maximum pulse length that can be used for each effect, while a plot of the NDU comparing pulsed IV data for two quiescent bias points of equal power dissipation reveals only differences due to trapping effects. In this way, trapping effects can be distinguished from thermal effects. Electrothermal modeling has arisen as a method of correcting for self-heating processes in a device with predominantly thermal effects. A parallel RC circuit is used to model channel temperature as a function of ambient temperature and power dissipated in the channel or junction. A technique is proposed for thermal resistance measurement and compared with a technique found in the literature. It is demonstrated that the thermal time constant can be measured from a plot of the NDU versus pulse length, and the thermal capacitance is then obtained using the thermal resistance and time constant. Finally, the results obtained through the thermal resistance measurement procedures are used to thermally correct static IV curves. Because trapping effects are negligible, it is shown that IV curves corresponding to different quiescent bias points for a Si LDMOSFET can be synthesized from three sets of static IV data taken at different ambient temperatures. The results obtained from this correction process for two quiescent bias points are compared to the pulsed IV results for these quiescent bias points and found to be quite accurate. Use of the methods presented in this work for obtaining more accurate transistor IV data data should assist in allowing more accurate nonlinear models to be obtained.

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