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Active Tuning of Thermal Conductivity in Single layer Graphene Phononic crystals using Engineered Pore Geometry and StrainRadhakrishna Korlam (11820830) 19 December 2021 (has links)
Understanding thermal transport across length scales lays the foundation to developing high-performance electronic devices. Although many experiments and models of the past few decades have explored the physics of heat transfer at nanoscale, there are still open questions regarding the impact of periodic nanostructuring and coherent phonon effects, as well as the interaction of strain and thermal transport. Thermomechanical effects, as well as strains applied in flexible electronic devices, impact the thermal transport. In the simplest kinetic theory models, thermal conductivity is proportional to the phonon group velocity, heat capacity, and scattering times. Periodic porous nanostructures impact the phonon dispersion relationship (group velocity) and the boundaries of the pores increase the scattering times. Strain, on the other hand, affects the crystal structure of the lattice and slightly increases the thermal conductivity of the material under compression. Intriguingly, applying strain combined with the periodic porous structures is expected to influence both the dispersion relation and scattering rates and yield the ability to tune thermal transport actively. But often these interrelated effects are simplified in models.<br><br>This work evaluates the combination of structure and strain on thermal conductivity by revisiting some of the essential methods used to predict thermal transport for a single layer of graphene with a periodic porous lattice structure with and without applied strain. First, we use the highest fidelity method of Non-Equilibrium Molecular Dynamics (NEMD) simulations to estimate the thermal conductivity which considers the impact of the lattice structure, strain state, and phononic band structure together. Next, the impact of the geometry of the slots within the lattice is interrogated with Boltzmann Transport Equation (BTE) models under a Relaxation Time Approximation. A Monte Carlo based Boltzmann Transport Equation (BTE) solver is also used to estimate the thermal conductivity of phononic crystals with varying pore geometry. Dispersion relations calculated from continuum mechanics are used as input here. This method which utilizes a simplified pore geometry only partially accounts for the effects of scattering on the pore boundaries. Finally, a continuum level model is also used to predict the thermal conductivity and its variations under applied strain. As acoustic phonon branches tend to carry the most heat within the lattice, these continuum models and other simple kinetic theories only consider their group velocities to estimate their impact on phonon thermal conductivity. As such, they do not take into account the details of phonon transport across all wavelengths.<br><br>By comparing the results from these different methods, each of which has different assumptions and simplifications, the current work aims to understand the effects of changes to the dispersion relationship based on strain and the periodic nanostructures on the thermal conductivity. We evaluate the accuracy of the kinetic theory, ray tracing, and BTE models in comparison to the MD results to offer a perspective of the reliability of each method of thermal conductivity estimation. In addition, the effect of strain on each phononic crystal with different pore geometry is also predicted in terms of change to their in-plane thermal anisotropy values. To summarize, this deeper understanding of the nanoscale thermal transport and the interrelated effects of geometry, strain, and phonon band structure on thermal conductivity can aid in developing lattices specifically designed to achieve the required dynamic thermal response for future nano-scale thermoelectric applications.
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Matematický model membránové destilace / Mathematical Model of Membrane DistillationHvožďa, Jiří January 2021 (has links)
Diplomová práce se zabývá membránovou destilací, především z matematické perspektivy. Jedná se o tepelně poháněný separační proces, ve kterém se pro rozdělení kapalné a plynné fáze používá porézní membrána. Kapalina se vypařuje a její plynná fáze prochází přes póry v membráně. Během tohoto procesu dochází k tepelné i látkové výměně, které jsou popsány systémem parciálních diferenciálnich rovnic. Další model je založen na analogii s elektrickými obvody, zákonu zachování energie, hmotnostní bilanci a empirických vztazích. Je ověřen s experimentálně naměřenými daty z nové alternativní destilační jednotky používající membránu a kondenzátor z polymerních dutých vláken. Výkon a účinnost jednotky jsou vyhodnoceny. Další možná vylepšení jsou navržena.
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Energetická náročnost vzduchotechnických jednotek pro bazénové haly / Energy performance of air handling units for swimming pool hallsBatelka, Václav January 2015 (has links)
The thesis is focused on determining the energy flows and the creation of an internal microclimate swimming pool halls. It describes the problems of design, the potential risks associated with the use of pools and thermodynamic processes heat and mass transfer. For this purpose was developed simulation program, which examines the behavior of heat and humidity in the room depending on external factors. The room can be simulated for any time period and geographic location. The outputs of the simulation are heat and mass balance, which will be covered air condition units. Three variants were designed and optimized solutions comparing claims on their operations. The experimental part is focused on the evaporation of the water. Measurement examines dependence of the speed of evaporation of water at different boundary conditions. Was investigated temperature dependence of water, temperature and relative humidity and air velocity above the water surface.
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Numerical Simulation of a Continuous CasterMatthew T Moore (8115878) 12 December 2019 (has links)
Heat transfer and solidification models were developed for use in a numerical model of a continuous caster to provide a means of predicting how the developing shell would react under variable operating conditions. Measurement data of the operating conditions leading up to a breakout occurrence were provided by an industrial collaborator and were used to define the model boundary conditions. Steady-state and transient simulations were conducted, using boundary conditions defined from time-averaged measurement data. The predicted shell profiles demonstrated good agreement with thickness measurements of a breakout shell segment – recovered from the quarter-width location. Further examination of the results with measurement data suggests pseudo-steady assumption may be inadequate for modeling shell and flow field transition period following sudden changes in casting speed. An adaptive mesh refinement procedure was established to increase refinement in areas of predicted shell growth and to remove excess refinement from regions containing only liquid. A control algorithm was developed and employed to automate the refinement procedure in a proof-of-concept simulation. The use of adaptive mesh refinement was found to decrease the total simulation time by approximately 11% from the control simulation – using a static mesh.
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Modelling and Evaluation of Fixed-Bed Photocatalytic Membrane ReactorsPhan, Duy Dũng 20 December 2019 (has links)
This work aims at modelling and evaluating a new type of photocatalytic reactors, named fixed-bed photocatalytic membrane reactor (FPMR). Such reactors are based on the deposition of a thin layer of photocatalysts on a permeable substrate by filtration. This layer serves as a photocatalytic membrane, named fixed-bed photocatalytic mem-brane (FPM), which is perpendicularly passed by the reactant solution and illuminated by a suitable light source. One advantage of FPMs is their renewability. The model, which was developed for this reactor, relates the overall reaction rate in the FPM with the intrinsic reaction kinetic at the catalyst surface and accounts for light intensity, structural and optical layer properties as well as the mass transfer in the pores.
The concept of FPMR was realised by using a flat sheet membrane cell. It facilitated principal investigations into the reactor performance and the validity of the model. For this purpose, the photocatalytic degradation of organic compounds, such as meth-ylene blue and diclofenac sodium, was conducted at varying conditions. Pyrogenic ti-tania was used as a photocatalyst. The experimental data support the developed mod-el. They also indicate a significant impact of the flow conditions on the overall photo-catalytic activity, even though the Reynolds number in the FPM was very small; the to-tal mass transfer rate in the FPM amounted to more than 1.0 s−1. The experiments also showed a sufficient structural strength of the FPM and photocatalytic stability. In addi-tion, the renewal and regeneration of FPMs was successfully demonstrated.
Furthermore, another FPMR was designed by means of submerged ceramic mem-branes. This reactor was mainly used to assess the effectiveness and efficiency of FPMRs at the example of the photocatalytic degradation of oxalic acid. The correspond-ing reactor was run closed loop and in continuous mode. The effectiveness of the reac-tor was evaluated based on common descriptors, such as apparent quantum yield, photocatalytic space-time yield and light energy consumption. The results showed that the FPMR based on submerged ceramic membrane had a higher efficiency than other reported photocatalytic reactors. The comparison of the different modes of operation revealed that the closed loop FPMR is most efficient with regard to light energy con-sumption.
Finally, this work discusses the up-scaling of FPMRs for industrial applications and proposes a solution, which can e.g. be employed for wastewater treatment or CO2 conversion.:Abstract iii
Kurzfassung v
Acknowledgment vii
Contents ix
Nomenclature xiii
1 Introduction 1
1.1 Motivation 1
1.2 Aim and objectives of the work 3
1.3 Thesis outline 3
2 Heterogeneous photocatalytic reactors 5
2.1 Introduction to photocatalysis 5
2.2 Processes in heterogeneous photocatalysis 6
2.2.1 Optical phenomena 7
2.2.2 Mass transfer 8
2.2.3 Adsorption and desorption 9
2.2.4 Photocatalytic reactions 10
2.2.5 Factors affecting heterogeneous photocatalysis 12
2.3 Photocatalytic reactor systems towards water treatment 16
2.3.1 Introduction to photocatalytic reactors 16
2.3.2 Development of photocatalytic reactor designs 17
2.3.3 Quantitative criteria for evaluating photocatalytic reactor designs 21
2.4 Cake layer formation in membrane microfiltration 22
2.4.1 Suspension preparation 22
2.4.2 Cake layer formation 23
2.5 Fluid flow through a fixed bed of particles 25
2.5.1 Pressure drop through a fixed-bed 25
2.5.2 Liquid-solid mass transfer correlation in fixed-bed 25
3 Concept and mathematical modelling of FPMRs 29
3.1 Concept of fixed-bed photocatalytic membrane reactors 29
3.2 Modelling of fixed-bed photocatalytic membrane reactors 31
3.3 Model sensitivity analysis 37
3.4 Chapter summary 39
4 FPMR realised with flat sheet polymeric membrane 41
4.1 Introduction 41
4.2 Materials and set-up 41
4.2.1 Materials 41
4.2.2 Experimental set-up 43
4.3 Experiments and methods 48
4.3.1 Formation of fixed-bed photocatalytic membrane 48
4.3.2 Reactor performance 50
4.3.3 Parameters study and model verification 53
4.3.4 Catalyst layer characterisation 56
4.3.5 Measurement and evaluation of photocatalytic activity of FPM 59
4.4 Results and model verification 60
4.4.1 Reactor performance 60
4.4.2 Influence parameters 71
4.4.3 Model verification 79
5 FPMR realised with submerged ceramic membrane 92
5.1 Introduction 92
5.2 Materials and reactor set-up 93
5.2.1 Reactor set-up 93
5.2.2 Chemicals 97
5.3 Experiments and methods 97
5.3.1 Formation of fixed-bed photocatalytic membranes 97
5.3.2 Photocatalytic performance 97
5.3.3 Parameter study 98
5.3.4 Reactor model for calculating reaction rate constant of FPM 99
5.3.5 Comparison of different reactor schemes 102
5.4 Results and discussions 105
5.4.1 Reactor performance 105
5.4.2 Consistency of CPMR and LPMR data 107
5.4.3 Influence of catalyst loading 108
5.4.4 Influence of permeate flux and light intensity 109
5.4.5 Reactor efficiency 111
5.4.6 Comparison of different reactor schemes 113
5.5 Proposed up-scaled FPMR systems 113
5.6 Concluding remarks 116
6 Conclusion and outlook 118
6.1 Summary of thesis contributions 118
6.2 Discussion and outlook 120
References 122
List of Figures 134
List of Tables 138
Appendix A Calibration 139
A.1 Distribution of light intensity on the surface of catalyst layer 139
A.2 Concentration and absorbance of diclofenac 141
A.3 TOC concentration and electrical conductivity of oxalic acid 141
A.4 Concentration and absorbance of methylene blue 142
Appendix B Mathematical modelling 143
B.1 Influence of axial dispersion on the reaction rate 143
B.2 Special case 146
Appendix C Comparison the photocatalytic activity of TiO2 and ZnO 147
Appendix D Mathematical validation of model for LPMR and CPMR 148
D.1 Model for LPMR (cf. Eq. (5 12)):148
D.2 Model for CPMR (cf. Eq. (5 17)) 149
Appendix E Particle size distribution 151
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Voltage loss analysis of PEM fuel cellsJayasankar, B., Pohlmann, C., Harvey, D.B. 25 November 2019 (has links)
The assessment of performance for PEM Fuel Cells (PEMFC) at the stack, Single Repeating Unit (SRU), and Membrane Electrode Assembly (MEA) level is dominated by the evaluation of polarization curves. However, polarization curves do not provide adequate detail as to the origin of the inefficiencies of the fuel cell performance and information on these sources of origin are critical to understand and address topics such as material selection, optimal operating conditions, and overall robust and reliable cell and stack design characteristics. To the purpose of understanding the origin of the inefficiencies underlying the fuel cell polarization curve a series of additional experimental and analysis techniques must be applied and from the resultant data the origin of the inefficiencies can then be assigned to kinetic, ohmic, and mass transport loss categorizations. Further, through a combination of the diagnostic methods further resolution can be implied down to the contribution of the individual components to the relative voltage loss categories. In this topic, a methodology will be presented and discussed that achieves and demonstrates this process.
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Strömungsinstabilitäten bei Stoffübergang und chemischer Reaktion an der ebenen Grenzfläche zwischen zwei nicht mischbaren FlüssigkeitenGrahn, Alexander January 2005 (has links)
In verfahrenstechnischen Anlagen der Flüssig-Flüssig-Stoffübertragung kommt es an der Phasengrenze zwischen den nicht mischbaren Flüssigphasen häufig zur Ausbildung hydrodynamischer Instabilitäten. Sie sind mit komplexen Geschwindigkeitsfeldern in den Flüssigphasen, insbesondere in den grenzschichtnahen Regionen verbunden und führen zu einem starken Anstieg der pro Zeiteinheit übertragenen Stoffmenge. Die Lösung der Diffusionsgleichung reicht in diesem Fall zur Vorausberechnung des für Auslegungszwecke bedeutsamen Stoffdurchgangskoeffizienten nicht mehr aus. Chemische Reaktionen stellen Quellen oder Senken von Wärme und Stoff dar, die das Auftreten von Instabilitäten begünstigen und die mathematische Beschreibung zusätzlich erschweren. Im Rahmen der vorliegenden Arbeit wurden experimentelle und numerische Untersuchungen zum Flüssig-Flüssig-Stoffübergang in einem vertikalen Kapillarspalt durchgeführt. Reaktionsfreie Stoffübergänge und solche mit einer exothermen chemischen Reaktion an der Phasengrenze zeigten eine große Vielfalt von Konvektionsstrukturen, wie Rollzellen, Thermiken und das doppeldiffusive Fingerregime. Die Visualisierung der Transportvorgänge erfolgte durch das Schattenschlierenverfahren. Die Beobachtungen wurden hinsichtlich geometrischer Eigenschaften von Konvektionsstrukturen sowie deren zeitlicher Änderung ausgewertet. Dazu zählten insbesondere das Längenwachstum von Thermiken und horizontale Wellenlängen von Fingerstrukturen. Zur mathematischen Beschreibung der Phänomene im Kapillarspalt wurde ein Modell entwickelt, welches auf den gekoppelten, zweidimensionalen Transportgleichungen von Impuls, Wärme und Stoff beruht. Es berücksichtigt dichte- und grenzflächenspannungsgetriebene Instabilitätsmechanismen sowie die besonderen Durchströmungseigenschaften des Kapillarspalts. Die Phasengrenze wurde als eben angenommen. Die Lösung der Modellgleichungen erfolgt auf numerischem Wege durch ein Computerprogramm. Das Modell ist in der Lage, die beobachteten Instabilitätsphänomene qualitativ richtig wiederzugeben. Mit Hilfe von Simulationsrechnungen konnte der Mechanismus aufgeklärt werden, der zum schnelleren Rückgang des Stoffdurchgangskoeffizienten im Rollzellenregime der rein grenzflächenspannungsgetrieben Instabilität im Vergleich zum Vorgang mit überlagerter Dichtekonvektion führt. Des Weiteren gelang der Nachweis des doppeldiffusiven Fingerregimes beim Stoffübergang mit exothermer Grenzflächenreaktion. Die berechnete Erhöhung des Stoffdurchgangskoeffizienten stimmt mit Angaben in experimentellen Arbeiten anderer Autoren überein.
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Ein Beitrag zur Modellierung von Dampfreformern für erdgasbetriebene BrennstoffzellenheizgeräteNitzsche, Jörg 29 October 2010 (has links)
Eine kompakte und effiziente Wasserstofferzeugung aus verfügbaren Energieträgern ist für die Marktfähigkeit von Brennstoffzellenheizgeräten essentiell. Der Auslegung von Reformern für PEM-Brennstoffzellen kommt eine große Bedeutung zu, da bei diesem Brennstoffzellentyp keine interne Reformierung möglich ist. In dieser Arbeit werden die mathematische Modellierung der Dampfreformierung von Erdgas, die Rolle der eingesetzten Katalysatoren und die Problematik von Wärme- und Stofftransportprozessen untersucht. Für fünf kommerzielle Nickel- und einen Rhodiumkatalysator werden die Kinetik, die effektive Wärmeleitfähigkeit und der Diffusionskoeffizient ermittelt. Unter Verwendung dieser Werte wird in einem Einzelpartikelmodell die Existenz und Signifikanz von intra- und extrapartikulären Stoff- und Temperaturgradienten evaluiert. Daraus werden für ein quasihomogenes Reaktormodell Modellparameter abgeleitet, die eine exakte Simulation unter Berücksichtigung der relevanten Phänomene zulassen. Schließlich wird ein Reaktormodell erstellt, welches mit Messwerten aus einem Versuchsreaktor validiert und für eine Sensitivitätsanalyse verwendet wird.
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High-Speed Flow Visualization and IR Imaging of Pool Boiling on Surfaces Having Differing Dynamic WettabilitiesNicholas Toan-Nang Vu (9760715) 14 December 2020 (has links)
Boiling is used in a wide variety of industries, including electronics cooling, distillation, and power generation. Fundamental studies on the boiling process are needed for effective implementation. Key performance characteristics of boiling are the heat transfer coefficient, which determines the amount of heat flux that can be dissipated for a given superheat, and critical heat flux(CHF), the failure point that occurs when vapor blankets the surface. The wettability of a surface is one of the key parameters that affects boiling behavior. Wetting surfaces(e.g., hydrophilic surfaces), typically characterized by a static contact angle below 90°,have better critical heat flux due to effective rewetting, but compromised heat transfer coefficients due to increased waiting times between nucleation of each bubble. Meanwhile, nonwetting surfaces (e.g., hydrophobic surfaces), characterized by static contact angles greater than 90°, have better heat transfer coefficients due to improved nucleation characteristic, but reach critical heat flux early due to surface dry out. However, recent studies have shown that the static contact angle alone offers and incomplete, and sometimes inaccurate, description of this behavior, which is instead governed entirely by the dynamic wettability. Specifically, the receding contact angle impacts the size and contact area of bubbles forming on a surface during boiling, while the advancing contact angle determines how the bubble departs. With this more complete set of wettability descriptors, three characteristic wetting regimes define the boiling behavior: hygrophilic surfaces having advancing and receding contact angles both under 90°; hygrophobic surfaces having both these dynamic contact angles over 90°;and ambiphilic surfaces having a receding contact angle less than 90°, but an advancing contact angle greater than 90°.The goal of this thesis is to experimentally characterize and compare the behavior of boiling surfaces in each of these regimes, observe the contact line behavior, and explain the mechanisms for their differences in performance.
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APPLICATIONS OF MICROHEATER/RESISTANCE TEMPERATURE DETECTOR AND ELECTRICAL/OPTICAL CHARACTERIZATION OF METALLIC NANOWIRES WITH GRAPHENE HYBRID NETWORKSDoosan Back (6872132) 16 December 2020 (has links)
<div>A microheater and resistance temperature detector (RTD) are designed and fabricated for various applications. First, a hierarchical manifold microchannel heatsink with an integrated microheater and RTDs is demonstrated. Microfluidic cooling within the embedded heat sink improves heat dissipation, with two-phase operation offering the potential for dissipation of very high heat fluxes while maintaining moderate chip temperatures. To enable multi-chip stacking and other heterogeneous packaging approaches, it is important to densely integrate all fluid flow paths into the device. Therefore, the details of heatsink layouts and fabrication processes are introduced. Characterization of two-phase cooling as well as reliability of the microheater/RTDs are discussed. In addition, another application of microheater for mining particle detection using interdigitated capacitive sensor. While current personal monitoring devices are optimized for monitoring microscale particles, a higher resolution technique is required to detect sub-micron and nanoscale particulate matters (PM) due to smaller volume and mass of the particles. The detection capability of the capacitive sensor for sub-micron and nanoparticles are presented, and an incorporated microheater improved stable capacitive sensor reading under air flow and various humidity. </div><div>This paper also introduces the characterization of nanomaterials such as metallic nanowires (NWs) and single layer graphene. First, the copper nanowire (CuNW)/graphene hybrid networks for transparent conductors (TC) is investigated. Though indium tin oxide (ITO) has been widely used, demands for the next generation of TC is increasing due to a limited supply of indium. Thus, the optical and electrical properties of CuNW/graphene hybrid network are compared with other transparent conductive materials including ITO. Secondly, silver nanowire (AgNW) growth technique using electrodeposition is introduced. A vertically aligned branched AgNW arrays is made using a porous anodic alumina template and the optical properties of the structure are discussed.</div><div><br></div>
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