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Thermal and fluid flow effects on bubble growth at a solidification frontWu, Ming-chang 30 August 2012 (has links)
The study applies the phase-field method to simulate the behavior between bubble and liquid-solid front in the solidification. During the process, the two-phase flow module is used to match up with temperature and phase-field function to determine the percentage of- solid, liquid, and gas- in the domain. The governing equations for mass, momentum and energy contain coefficients which are related to percentage of phases.The result show that the surface tension and the temperature difference will influence the shape of bubble and the velocity of solidification.
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Entrainment and mixing properties of multiphase plumes: Experimental studies on turbulence and scalar structure of a bubble plumeSeol, Dong Guan 15 May 2009 (has links)
This dissertation presents a series of laboratory experiments to study flow and mixing
properties of multiphase plumes. The particle image velocimetry (PIV) and laserinduced
fluorescence (LIF) techniques are developed to measure two-dimensional velocity
and concentration fields of multiphase plumes. The developed measurement
techniques are applied to bubble plumes in different ambient conditions.
The problems and errors in the two-phase PIV application to a bubble plume case
are addressed through a comparative study between the optical separation method
using fluorescent particles and a new phase separation method using vector postprocessing.
The study shows that the new algorithm predicts well the instantaneous
and time-averaged velocity profiles and has errors comparable to those for image
masking techniques.
The phase separation method developed in the previous section is applied to
study the mean flow characteristics of a bubble plume in quiescent and unstratified
condition. The entrainment coefficients representing the mixing properties of a bubble
plume are calculated to lie between 0.08 near the plume source and 0.05 in the upper
region, and to depend on the non-dimensional quantity us/(B/z)1/3, where us is the
bubble slip velocity, B is the initial buoyancy flux, and z is the height from the diffuser.
Further, the LIF technique is investigated to measure the scalar concentration
field around a bubble plume in quiescent, unstratified condition. This new application
to bubble plumes accounts for light scattering by bubbles using an attenuation coef-
ficient that is proportional to the local void fraction. Measured scalar concentration
fields show similar trend in concentration fluctuation to turbulent plume cases.
Finally, the velocity and concentration field measurements using the developed
two-phase PIV and LIF methods are applied for a bubble plume in a density-stratified
ambient. The turbulent flow characteristics induced by a bubble plume in a stratified
ambient water are studied. The plume fluctuation frequency is measured as about 0.1
Hz and compares well to plume wandering frequency measured in unstratified plume
cases.
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Prediction Of Separation Factor In Foam Separation Of ProteinsBhattacharjee, Samita 08 1900 (has links)
Polyhedral foams offer large gas-liquid interfacial area associated with a small amount of liquid. Therefore, if a solute adsorbs preferentially at the interface, the concentration of the solute in the foam will be greater than in the solution from which the foam has been generated. This effect provides a simple method of concentrating materials which have a tendency to adsorb on the gas-liquid interface. This is particularly relevant to biomaterials like whole cells, proteins, enzymes etc., which are surface active and are present in low concentrations in the broth. Foam separation has therefore attracted considerable attention, and several reports exist in literature on concentrating cells, proteins and enzymes using foams.
Foam separation is based on the difference in surface activity of the components to be separated. A surface active molecule consists of a lyophobic and a lyophilic group. (As water is commonly used as a solvent, the lyophilic and lyophobic groups are called hydrophilic and hydrophobic groups, respectively). When dissolved in a solvent, the presence of lyophobic groups in the interior of the solvent distorts the solvent liquid structure, thereby increasing the free energy of the system.
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Bubble Solid InteractionMukherjee, Manas 12 1900 (has links)
The interaction of a bubble with solid surfaces, hydrophobic and hydrophilic, was investigated. When a bubble approaches towards a solid surface, a thin liquid film forms between them. The liquid in the film drains until an instability forms and film ruptures resulting in a three phase contact (TPC). Following rupture, the TPC line spreads on the solid surface. In the present study, glycerol-water solutions with varying percentages of water were used to investigate the effect of viscosity. Experiments were carried out with varying bubble size. The rupture and TPC line movement were recorded by high-speed digital video camera. The dependence of the TPC line movement on different parameters was investigated. The experimental results were compared with the existing theories for the TPC line movement. An empirical equation was developed to predict the TPC line movement. Formation or rupturing of the intervening film in case of a hydrophilic surfaces, which were glass surface cleaned by six cleaning techniques, was investigated. It was shown that a stable film forms for acid or alkali cleaning.
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Behavioral Finance : The Student InvestorSairafi, Kamran, Selleby, Karl, Ståhl, Thom January 2008 (has links)
<p>Bachelor thesis within Business Administration</p><p>Title: Behavioral Finance – The Student Perspective</p><p>Authors: Kamran Sairafi, Karl Selleby, Thom Ståhl</p><p>Tutor: Urban Österlund</p><p>Date: 2008-05-30</p><p>Background: History is full of examples on how humans can create investment</p><p>bubbles through speculation; from the Dutch tulip mania to the</p><p>Dot Com bubble humans have proven to be capable of creating</p><p>economical chaos. Classical economical theories hold the assumption</p><p>that individuals act rationally regarding decisions of an</p><p>economical nature. Since the information on the stock market is</p><p>available to everyone who seeks it, the appearance of investment</p><p>bubbles should not be possible. Behavioral finance is an academic</p><p>branch which seeks to explore these phenomenons through the</p><p>psychological factors affecting humans in investment decisions.</p><p>Purpose: The purpose of the report is twofold. Firstly it is to examine the</p><p>characteristics of investment interested business students enrolled</p><p>at Jönköping International Business School. Secondly it looks into</p><p>the decision-making process and choices of the population</p><p>from the perspective of behavioral finance.</p><p>Method: This research holds an abductive approach and is based on qualitative</p><p>data. Data collection was done through an Internet-based</p><p>questionnaire containing several different questions on the areas</p><p>related to the inquiries. In some cases statistical analysis was conducted</p><p>to test for significant correlation between key characteristics.</p><p>Results: A statistically proven correlation could be discerned between</p><p>trading experience and frequency; for each additional year an individual</p><p>engaged in trading the frequency increased. Herd behavior</p><p>was detected in a majority of the sample. When faced with a</p><p>scenario in which their immediate surrounding opposed their own</p><p>analysis of a stock, the greater part of the sample would reconsider</p><p>their position. Two main sub-groups were detected. The first</p><p>was characterized by its high tolerance of risk; the second subgroup</p><p>was characterized by its inconsistency in behavior.</p><p>Conclusions: This paper found that the behavior of respondents in the chosen</p><p>population was best described as “student behavior”; a somehow</p><p>irrational behavior explained by the learning process in which</p><p>business students exist.</p>
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Untersuchung der Dynamik fluider Partikel auf Basis der Volume of Fluid MethodeSchmidtke, Martin 31 March 2010 (has links) (PDF)
Die in dieser Arbeit vorgestellten Simulationen aufsteigender fluider Partikel wurden mit dem CFD-Programm FS3D durchgeführt, welches auf der Volume-of-Fluid (VoF) Methode basiert. Die Validierung des Codes erfolgt durch Vergleich der numerischen Lösungen für schleichende Strömungen mit analytischen Lösungen, wobei eine gute Übereinstimmung festgestellt wird. Im ersten Teil der Dissertation werden Simulationen für den freien Aufstieg von Öltropfen in Wasser mit experimentellen Beobachtungen hinsichtlich der Aufstiegsgeschwindigkeit, der Tropfenform und der Bewegungsbahn verglichen. Die Aufstiegsgeschwindigkeiten und Widerstandsbeiwerte sind vergleichbar, die simulierten Tropfen sind jedoch deutlich flacher. Dieser Unterschied kann durch Verunreinigungen der Grenzfläche im Experiment verursacht sein. Der Übergang von einem gradlinigen Aufstieg zu zickzack-förmigen Aufstiegsbahnen kann mit Hilfe der Simulationen auf Instabilitäten im Nachlauf der Blasen zurückgeführt werden, die zu einer periodischen Wirbelablösung führen. Im zweiten Teil der Dissertation wird der Aufstieg von Blasen in linearen Scherströmungen untersucht. Steigen die Blasen in einer vertikalen Scherströmung auf, so beobachtet man eine seitliche Migration. Diese seitliche Migration der Blasen wird durch die sogenannte Liftkraft verursacht, deren Vorzeichen und Betrag von der Blasengröße und den Stoffeigenschaften der Flüssigkeit abhängt. Die Simulationen zeigen, daß das Vorzeichen der Liftkraft für eher sphärische Blasen durch den Bernoulli-Effekt erklärt werden kann. An stark deformierten Blasen hingegen wirkt die Liftkraft in umgekehrter Richtung. Dieses Phänomen tritt auch in den Simulationen auf. Verschiedene Hypothesen für die Ursache dieses Phänomens werden überprüft. Die bekannteste experimentelle Korrelation für die Liftkraft von Tomiyama u.a. (2002) wird durch Simulation von realen Flüssigkeiten mit bekannten Stoffeigenschaften wie auch von Modellfluiden mit willkürlichen Stoffeigenschaften validiert und weitgehend bestätigt. Die Lift-Korrelation hat demnach hinsichtlich der Stoffeigenschaften der Flüssigkeit einen größeren Geltungsbereich, als bisher experimentell überprüft wurde. The simulations presented in this thesis were performed with the CFD code FS3D which is based on the Volume of Fluid method. The code is validated using analytical solutions for creeping flows and a good agreement is observed between simulation and analytical solution. In the first part of the thesis, the free rise of oil drops in water is simulated and compared with experimental observations. The results show that the rising velocities and the drag coefficients are similar in both cases, but the simulated drops are flatter (more oblate). This difference may be caused by impurities of the particle surface (surfactants) in the experiments. The simulations show that the transition from rectilinear to periodic trajectories is caused by instabilities in the wake, which lead to a periodic vortex shedding. In the second part of the thesis, the rise of bubbles in linear shear flows is investigated. If bubbles rise in a vertical shear flow, a lateral migration can be observed. This migration is caused by the so called lift force. Sign and magnitude of the lift force depend on the size of the bubble and the material properties of the liquid. The simulation results show that the sign of the lift force on spherical bubbles can be explained by the Bernoulli effect. However, the lift force on more distorted bubbles acts in the opposite direction. This phenomenon can also be observed in the simulation. In this work several hypotheses for the reason of this phenomenon are checked. Furthermore, most common correlation for the lift force (developed by Tomiyama et al. in 2002) is validated for fluids of known material and model fluids with arbitrary material data. The correlation is valid in a wider range of fluid material properties than proved experimentally up to now.
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Turbulent dispersion of bubbles in poly-dispersed gas-liquid flows in a vertical pipeShi, Jun-Mei, Prasser, Horst-Michael, Rohde, Ulrich 31 March 2010 (has links) (PDF)
Turbulence dispersion is a phenomenon of practical importance in many multiphase flow systems. It has a strong effect on the distribution of the dispersed phase. Physically, this phenomenon is a result of interactions between individual particles of the dispersed phase and the continuous phase turbulence eddies. In a Lagrangian simulation, a particle-eddy interaction sub-model can be introduced and the effect of turbulence dispersion is automatically accounted for during particle tracking. Nevertheless, tracking of particleturbulence interaction is extremely expensive for the small time steps required. For this reason, the Lagrangian method is restricted to small-scale dilute flow problems. In contrast, the Eulerian approach based on the continuum modeling of the dispersed phase is more efficient for densely laden flows. In the Eulerian frame, the effect of turbulence dispersion appears as a turbulent diffusion term in the scalar transport equations and the so-called turbulent dispersion force in the momentum equations. The former vanishes if the Favre (mass-weighted) averaged velocity is adopted for the transport equation system. The latter is actually the total account of the turbulence effect on the interfacial forces. In many cases, only the fluctuating effect of the drag force is important. Therefore, many models available in the literature only consider the drag contribution. A new, more general derivation of the FAD (Favre Averaged Drag) model in the multi-fluid modeling framework is presented and validated in this report.
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Mathematical modelling and experimental simulation of chlorate and chlor-alkali cells.Byrne, Philip January 2001 (has links)
<p>The production of chlorate, chlorine and sodium hydroxiderelies heavily on electrical energy, so that savings in thisarea are always a pertinent issue. This can be brought aboutthrough increased mass transfer of reacting species to therespective electrodes, and through increased catalytic activityand uniformity of current density distribution at theseelectrodes. This thesis will present studies involvingmathematical modelling and experimental investigations of theseprocesses. They will show the effect that hydrodynamicbehaviour has on the total current density and cell voltages,along with the effects on current density distributions andindividual overpotentials atthe respective electrodes.</p><p>Primary, secondary and psuedo-tertiary current densitydistribution models of a chlor-alkali anode are presented anddiscussed. It is shown that the secondary model presentsresults rather similar to the pseudo-tertiary model, when thecurrent density distribution is investigated, although thepotential distribution differs rather markedly. Furthermore, itis seen that an adequate description of the hydrodynamicsaround the anode is required if the potential distribution, andthereby the prevalence of side-reactions, is to be reasonablepredicted.</p><p>A rigorous tertiary current density distribution model ofthe chlorate cell is also presented, which takes into accountthe developing hydrodynamic behaviour along the height of thecell. This shows that an increased flowrate gives more uniformcurrent density distributions. This is due to the fact that theincreased vertical flowrate of electrolyte replenishes ioncontent at the electrode surfaces, thus reducing concentrationoverpotentials. Furthermore, results from the model lead to theconclusion that it is the hypochlorite ion that partakes in themajor oxygen producing side-reaction.</p><p>A real-scale cross-section of a segmented anode-cathode pairfrom a chlorate cell was designed and built in order to studythe current density distribution in industrial conditions.These experiments showed that increased flowrate brought aboutmore even current density distributions, reduced cell voltageand increased the total current density. An investigation ofthe hydrodynamic effects on the respective electrodeoverpotentials shows the anode reactions being more favoured byincreased flowrate. This leads to the conclusion that theuniform current density distribution, caused by increasedflowrate, occurs primarily through decreasing the concentrationoverpotential at the anode rather than by decreasing thebubble-induced ohmic drop at the cathode.</p><p>Finally, results from experiments investigating thebubble-induced free convection from a small electrochemicalcell are presented. These experiments show that Laser DopplerVelocimetry is the most effective instrument for investigatingthe velocity profiles in bubble-containing electrochemicalsystems. The results also show that the flow can transform fromlaminar to turbulent behaviour on both the vertical andhorizontal planes, in electrochemical systems where bubbles areevolved.</p>
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Designing Microfluidic Control ComponentsWijngaart, Wouter van der January 2002 (has links)
No description available.
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The thermal evolution and dynamics of pyroclasts and pyroclastic density currentsBenage, Mary Catherine 21 September 2015 (has links)
The thermal evolution of pyroclastic density currents (PDCs) is the result of entrainment of ambient air, particle concentration, and initial eruptive temperature, which all impact PDC dynamics and their hazards, such as runout distance. The associated hazards and opaqueness of PDCs make it impossible for in-situ entrainment efficiencies or concentration measurements that would provide critical information on the thermal evolution and physical processes of PDCs. The thermal evolution of explosive eruptive events such as volcanic plumes and pyroclastic density currents (PDCs) is reflected in the textures of the material they deposit. A multiscale model is developed to evaluate how the rinds of breadcrust bombs can be used as a unique thermometer to examine the thermal evolution of PDCs. The multiscale, integrated model examines how bubble growth, pyroclast cooling, and dynamics of PDC and projectile pyroclasts form unique pyroclast morphology. Rind development is examined as a function of transport regime (PDC and projectile), transport properties (initial current temperature and current density), and pyroclast properties (initial water content and radius). The model reveals that: 1) rinds of projectile pyroclasts are in general thicker and less vesicular than those of PDC pyroclasts; 2) as the initial current temperature decreases due to initial air entrainment, the rinds on PDC pyroclasts progressively increase in thickness; and 3) rind thickness increases with decreasing water concentration and decreasing clast radius. Therefore, the modeled pyroclast’s morphology is dependent not only on initial water concentration but also on the cooling rate, which is determined by the transport regime.
The developed secondary thermal proxy is then applied to the 2006 PDCs from the Tungurahua eruption to constrain the entrainment efficiency and thermal evolution of PDCs. A three-dimensional multiphase Eulerian-Eulerian-Lagrangian (EEL) model is coupled to topography and field data such as paleomagnetic data and rind thicknesses of collected pyroclasts to study the entrainment efficiency and thus the thermal history of PDCs at Tungurahua volcano, Ecuador. The modeled results that are constrained with observations and thermal proxies demonstrate that 1) efficient entrainment of air to the upper portion of the current allows for rapid cooling, 2) the channelized pyroclastic density currents may have developed a stable bed load region that was inefficient at cooling and 3) the PDCs had temperatures of 600-800K in the bed load region but the upper portion of the currents cooled down to ambient temperatures. The results have shown that PDCs can be heterogeneous in particle concentration, temperature, and dynamics and match observations of PDCs down a volcano and the thermal proxies. Lastly, the entrainment efficiencies of PDCs increases with increasing PDC temperature and entrainment varies spatially and temporally. Therefore, the assumption of a well-mixed current with a single entrainment coefficient cannot fully solve the thermal evolution and dynamics of the PDC.
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