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Zum Einfluss elektrochemischer Doppelschichten auf den Stofftransport in nanoskaligen Elektrolytsystemen:: Leitfähigkeit von Nanoporen und Voltammetrie an NanoelektrodenKubeil, Clemens 26 October 2016 (has links)
Es besteht enormes Interesse den Stofftransport in nanoskaligen Systemen zu verstehen und selektiv zu steuern, um analytische und synthetische Anwendungen zu entwickeln, aber auch um die physiologischen Prozesse lebender Zellen zu entschlüsseln. Im Rahmen dieser Arbeit wurde der Einfluss der elektrochemischen Doppelschicht an ausgewählten nanoskaligen Elektrolytsystemen untersucht.
Die Gleichrichtung von Ionenströmen (engl. Ionic Current Rectification ICR) in Nanoporen mit einer Oberflächenladung äußert sich in einer gekrümmten Strom-Spannungs-Kurve. Die Überlappung von innerem und äußerem Potential ist dabei hinsichtlich der Ionenverteilung und somit der Porenleitfähigkeit einander verstärkend oder gegenläufig. Auf Grundlage dieses Mechanismus wurde die Gleichrichtung bei einem sehr großen Verhältnis von Porenöffnung zu Debye-Länge erklärt. Ferner wurde mittels der eingeführten relativen Leitfähigkeit κ´ die verschiedenen Leitfähigkeitszustände in Abhängigkeit der Elektrolytkonzentration und Temperatur sichtbar gemacht und Implikationen für Sensoranwendungen wie z.B. dem resistiven Pulszähler zur Partikelanalyse abgeleitet.
Es wurde ein numerisches Modell basierend auf dem Poisson-Nernst-Planck-Gleichungssystem entwickelt, um die Translokation eines Nanopartikels durch eine konische Nanopore bei einer geringen Leitsalzkonzentration zu beschreiben. Neben dem klassischen Volumenausschluss-Effekt tritt zusätzlich ein Gleichrichtungseffekt (ICR-Effekt) in der Pore auf. Eine Analyse zur Entflechtung von Partikelgröße und Partikelladung aus der Pulshöhe und Pulsform wurde erfolgreich durchgeführt.
Wie der Stofftransport durch eine Oberflächenladung auf dem umgebenden Material einer Nanoelektrode beeinflusst wird, wurde anhand des voltammetrischen Verhaltens diskutiert. An sehr kleinen Elektroden (< 10 nm) ist demnach der Einfluss der elektrochemischen Doppelschicht auf die Strom-Spannungs-Kurve besonders groß und kann auch bei Vorliegen eines hohen Leitsalzüberschusses nicht vernachlässigt werden. In leitsalzfreien Elektrolyten sind die gefundenen Effekte so deutlich, dass sie auch an größeren Elektroden experimentell zweifelsfrei festgestellt worden sind. / There is an enormous interest in understanding and selectively controlling the material transport in nanoscale systems to develop analytical and synthetic applications, but also to decipher the physiological processes of living cells. Within this thesis, the influence of the electrochemical double layer on selected nanoscale electrolyte systems was studied.
Ionic Current Rectification (ICR) in nanopores carrying a surface charge manifests itself in a non-linear current-voltage-curve. The overlap of interior and exterior potential is cumulative or opposing with regard to the ion distribution and therefore the pore conductivity. Based on this mechanism, ICR for very large ratios of pore size and Debye length was explained. Furthermore, the different conducting states as a function of electrolyte concentration and temperature were visualized by introducing the relative conductivity κ´ and hence implications for sensor applications such as the resistive pulse sensor have been deduced.
A numerical model based on the Poisson-Nernst-Planck-equations was developed to describe the translocation of a nanoparticle through a conical nanopore at a low electrolyte concentration. An additional rectification effect (ICR effect) occurs in the pore beside the conventional volume exclusion effect. An analysis was successfully performed to deconstruct the particle size and particle charge from the pulse height and shape.
The material transport is affected by a surface charge on the shrouding material of nanoelectrodes as it was discussed by means of the voltammetric behaviour. The influence of the electrochemical double layer on the current-voltage-curve is particularly large at very small electrodes (< 10 nm) and cannot be neglected even at a high excess of supporting electrolyte. The observed effects were pronounced in unsupported electrolytes, so that they could be clearly detected experimentally at even larger electrodes.
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Molecular Dynamics Investigation of Surface Potential andElectrokinetic Phenomena at the Amorphous Silica/WaterInterfaceChen, Si-Han January 2018 (has links)
No description available.
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A Travelling Wave Slot Array based on a Double-Layer Lens for 77 GHz Automotive RadarUgle, Ashray January 2023 (has links)
Automotive radars have gained considerable interest in recent years for applications of road safety for vulnerable road users. The use of multipleinput and multiple-output (MIMO) technology in automotive radar has helped in realising a virtual aperture greater than the physical aperture of the antenna which has reduced the size of the overall radar module. But increasing the number of MIMO channels for greater angular resolution can introduce increased computational complexity, processing time and latency. A new type of radar using the multiple input multiple steered output (MIMSO) radar can alleviate these concerns by replacing the angle-FFT with beamforming by means of a lens. A double-layer lens with a beamforming layer and a radiating layer with a radiating aperture on the 2-D footprint of the lens is proposed as an antenna system for this new radar technique. This work focuses on the radiating aperture which has been realised as a travelling wave planar slotted array in gap waveguide technology due to its benefit of low losses and ease of manufacturing. A ridged gap waveguide is chosen for the reduction of the waveguide size and to avoid the appearance of grating lobes in the visible range for large scan angles. The planar slotted array is synthesised in the travelling wave configuration and reflection cancelling notches are used in the ridge to cancel the reflections from the slots. The aperture is chosen to be of a circular shape for a compact design and to maximise aperture efficiency. The planar array is verified with a full-wave simulation with a bandwidth of 76 to 81 GHz and a realised gain of 27.7 dBi at the centre frequency. The array can be scanned up to ±50◦ with a scan loss of 2.4 dBi. / Fordonsradarer har fått stort intresse under de senaste åren för tillämpningar av trafiksäkerhet för utsatta trafikanter. Användningen av MIMO-teknik (multipleinput och multiple-output) i bilradar har hjälpt till att realisera en virtuell bländaröppning som är större än antennens fysiska bländaröppning, vilket har minskat storleken på den totala radarmodulen. Men att öka antalet MIMOkanaler för större vinkelupplösning kan introducera ökad beräkningskomplexitet, bearbetningstid och latens. En ny typ av radar som använder MIMSO-radarn (multiple input multiple steered output) kan lindra dessa problem genom att ersätta vinkel-FFT med strålformning med hjälp av en lins. En dubbelskiktslins med ett strålformande skikt och ett strålande skikt med en strålande bländare på linsens 2D-fotavtryck föreslås som ett antennsystem för denna nya radarteknik. Detta arbete fokuserar på strålningsöppningen som har realiserats som en plan slitsad array i gap-vågledarteknologi på grund av dess fördel med låga förluster och enkel tillverkning. En vågledare med räfflade gap väljs för att minska vågledarstorleken och för att undvika uppkomsten av gitterlober i det synliga området för stora avsökningsvinklar. Den plana uppsättningen syntetiseras i den vandringsvågkonfigurationen och reflektionsupphävande skåror används i åsen för att eliminera reflektionerna från slitsarna. Bländaren är vald för att ha en cirkulär form för en kompakt design och för att maximera bländareffektiviteten. Planar arrayen verifieras med en helvågssimulering med en bandbredd på 76 till 81 GHz och en realiserad vinst på 27, 7 dBi vid mittfrekvensen. Arrayen kan skannas upp till ±50◦ med en skanningsförlust på 2, 4 dBi.
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Transmission problems for Dirac's and Maxwell's equations with Lipschitz interfacesAxelsson, Andreas, kax74@yahoo.se January 2002 (has links)
The aim of this thesis is to give a mathematical framework for scattering of electromagnetic waves by rough surfaces. We prove that the Maxwell transmission problem with a weakly Lipschitz interface,in finite energy norms, is well posed in Fredholm sense for real frequencies. Furthermore, we give precise conditions on the material constants ε, μ and σ and the frequency ω when this transmission problem is well posed. To solve the Maxwell transmission problem, we embed Maxwells equations in an elliptic Dirac equation. We develop a new boundary integral method to solve the Dirac transmission problem. This method uses a boundary integral operator, the rotation operator, which factorises the double layer potential operator. We prove spectral estimates for this rotation operator in finite energy norms using Hodge decompositions on weakly Lipschitz domains. To ensure that solutions to the Dirac transmission problem indeed solve Maxwells equations, we introduce an exterior/interior derivative operator acting in the trace space. By showing that this operator commutes with the two basic reflection operators, we are able to prove that the Maxwell transmission problem is well posed. We also prove well-posedness for a class of oblique Dirac transmission problems with a strongly Lipschitz interface, in the L_2 space on the interface. This is shown by employing the Rellich technique, which gives angular spectral estimates on the rotation operator.
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Atomic Layer Deposition onto Fibers / Atomlagenabscheidung auf FasernRoy, Amit Kumar 19 March 2012 (has links) (PDF)
The main goal of this dissertation was to show that the principle of atomic layer deposition (ALD) can be applied to “endless” fibers. A reactor of atomic layer deposition has been designed, especially for coating depositions onto meter long bundles of fibers. Aluminum oxide (alumina), titanium oxide (titania), double layers of alumina and titania, as well as aluminium phosphate have been deposited onto bundles of carbon fibers using the home-built reactor. Scanning electron microscopic (SEM) and transmission electron microscopic (TEM) images indicate that the coatings were uniform and conformal onto fiber surface. There was a good adhesion of the coatings to the fibers.
Alumina has been deposited using two separate aluminum sources (aluminum trichloride and trimethylaluminum), and water as a source of oxygen. In case of alumina deposition using aluminum trichloride and water, initial deposition temperature was 500 °C. In these conditions, a part of the fiber bundle has been damaged. Thus, the deposition temperature was decreased to 300 °C and the fibers were unaffected. In addition, during this process hydrochloric acid is formed as a byproduct which is a corrosive substance and affects the reactor and there was a chloride impurity in the coatings. Thus, aluminum trichloride precursor was replaced by trimethylalumium.
Alumina deposition onto carbon fibers using trimethylaluminum and water was carried out at a temperature of 77 °C. SEM images revealed that the fibers were unaffected and the coatings were uniform and conformal. Oxidation resistance of the carbon fibers was improved slightly after alumina deposition. Oxidation onset temperature of the uncoated fibers was about 630 °C. The resistance was linearly increased with the coating thickness (up to 660 °C) and getting saturated over a thickness of 120 nm. Titania coatings have been deposited using titanium tetrachloride and water. The physical appearances of the titania coatings were similar to the alumina coatings. The oxidation onset temperature of the titania coated carbon fibers was similar to the uncoated fibers but the rate of oxidation was decreased than the uncoated fibers. Two double layer coatings were deposited, alumina followed by titania (alumina/titania), and titania followed by alumina (titania/alumina). If the fibers were coated with the double layer of alumina/titania, they had almost same oxidation onset as alumina coated fibers but the rate of oxidation was decreased significantly compared to alumina coated fibers. This feature is independent of the thickness of the titania layers, at least in the regime investigated (50 nm alumina followed by 13 nm and 40 nm titania). On the other hand, the oxidation onset temperature of fibers coated with titania/alumina (20 nm titania /30 nm alumina) was approximately 750 °C. The fibers were burned completely when temperature was further increased to 900 °C and held another 60 minutes at 900 °C. This is significantly better than any other coating used in this dissertation.
ALD of titania and alumina in principle was known beforehand, this dissertation here applies this knowledge for the first time to endless fibers. Furthermore, this dissertation shows for the first time that one can deposit aluminum phosphate via ALD (planar surface as well as fibers). Aluminum phosphate might be special interest in the fiber coating because it is a rather soft material and thus might be used to obtain a weak coupling between fiber and matrix in composites. Aluminum phosphate was deposited using trimethylaluminum and triethylphosphate as precursors. Energy dispersive X-ray spectroscopy and solid state nuclear magnetic resonance spectra confirmed that the coating comprises aluminum phosphate (orthophosphate as well as other stoichiometries). Scanning electron microscopic images revealed that coatings are uniform and conformal. In cases of alumina and titania, it was observed that the coatings were delaminated from the ends of cut fibers and thus formed of clear steps. On the other hand, for aluminum phosphate coating it was observed that the border between coating and underlying fiber often being smeared out and thus formed an irregular line. It seems in case aluminum phosphate cohesion is weaker than adhesion, thus it might be act a weak interface between fiber and matrix. Alumina, titania, and double layer microtubes have been obtained after selective removal of the underlying carbon fibers. The carbon fibers were selectively removed via thermal oxidation in air at temperatures exceeding 550 °C. SEM and TEM images indicate that the inner side of the tube wall has the same morphology like the fibers. In addition, it was observed that the individual microtubes were separated from their neighbors and they had almost uniform wall thicknesses. The longest tubes had a length of 30 cm. / Das Hauptziel dieser Dissertation bestand darin nachzuweisen, dass die Atomlagenabscheidung (engl. atomic layer deposition (ALD)) auf „endlose“ Fasern angewendet werden kann. Es wurde ein Reaktor zur Atomlagenabscheidung gestaltet, der speziell für die Beschichtung meterlanger Faserbündel geeignet ist. Aluminiumoxid, Titanoxid, Doppelschichten aus Aluminiumoxid und Titanoxid sowie Aluminiumphosphat wurden mit Hilfe des selbstgebauten Reaktors auf Kohlefaserbündel abgeschieden. Rasterelektronenmikroskopische (REM) und transmissionselektronenmikroskopische (TEM) Aufnahmen zeigten, dass die Beschichtung auf den Fasern einheitlich und oberflächentreu war. Des Weiteren wurde eine gute Adhäsion zwischen Beschichtung und Fasern beobachtet. Das Prinzip der Beschichtung mit Titanoxid und Aluminiumoxid mit Hilfe der ALD war bereits vorher bekannt und im Rahmen dieser Dissertation jedoch erstmals auf "endlose" Fasern angewendet. Des Weiteren wird in dieser Dissertation erstmals gezeigt, dass es möglich ist, Aluminiumphosphat mittels ALD abzuscheiden (sowohl auf planaren Oberflächen als auch auf Fasern). Aluminiumphosphat könnte von besonderem Interesse in der Faserbeschichtung sein, da es ein relativ weiches Material ist und könnte daher als eine Art „schwacher“ Verbindung zwischen Faser und Matrix in Kompositen dienen. Die Oxidationsbeständigkeit von beschichten Kohlefasern wurde im Vergleich zu unbeschichteten Fasern bis zu einem gewissen Grad erhöht. Monoschichten von Aluminiumoxid und Titanoxid waren dafür wenig effektiv. Aluminiumphosphatbeschichtete Fasern waren deutlich besser geeignet als die beiden anderen. Eine Doppelschicht aus Titanoxid gefolgt von Aluminiumoxid verbesserte die Oxidationsbeständigkeit nochmals deutlich gegenüber allen anderen Beschichtungen, die in dieser Dissertation verwendet wurden. Mikroröhren aus Aluminiumoxid, Titanoxid und Doppelschichten wurden durch die selektive Entfernung der zugrunde liegenden Kohlefasern erhalten. Einzelne Mikroröhren waren von benachbarten Röhren getrennt und sie weisen eine nahezu einheitliche Wanddicke auf.
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Analýza a návrh vinutí střídavých strojů / Analysis and design of the AC machines winding.Vorel, Luboš January 2014 (has links)
This diploma thesis is focused on an analysis and design of an AC machines windings. In the theoretical part of the thesis, differences between single-layer and double-layer windings are explained. Next, the properties of a stator winding of synchronous machines are described. Finally, the winding factor is determined by means of a standard calculation method and by means of a new progressive calculation method, too. In the experimental part of this thesis, the stator winding of a high-speed synchronous generator excited by permanent magnets on the rotor is designed. This generator is driven by a steam turbine.
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Atomic Layer Deposition onto FibersRoy, Amit Kumar 14 March 2012 (has links)
The main goal of this dissertation was to show that the principle of atomic layer deposition (ALD) can be applied to “endless” fibers. A reactor of atomic layer deposition has been designed, especially for coating depositions onto meter long bundles of fibers. Aluminum oxide (alumina), titanium oxide (titania), double layers of alumina and titania, as well as aluminium phosphate have been deposited onto bundles of carbon fibers using the home-built reactor. Scanning electron microscopic (SEM) and transmission electron microscopic (TEM) images indicate that the coatings were uniform and conformal onto fiber surface. There was a good adhesion of the coatings to the fibers.
Alumina has been deposited using two separate aluminum sources (aluminum trichloride and trimethylaluminum), and water as a source of oxygen. In case of alumina deposition using aluminum trichloride and water, initial deposition temperature was 500 °C. In these conditions, a part of the fiber bundle has been damaged. Thus, the deposition temperature was decreased to 300 °C and the fibers were unaffected. In addition, during this process hydrochloric acid is formed as a byproduct which is a corrosive substance and affects the reactor and there was a chloride impurity in the coatings. Thus, aluminum trichloride precursor was replaced by trimethylalumium.
Alumina deposition onto carbon fibers using trimethylaluminum and water was carried out at a temperature of 77 °C. SEM images revealed that the fibers were unaffected and the coatings were uniform and conformal. Oxidation resistance of the carbon fibers was improved slightly after alumina deposition. Oxidation onset temperature of the uncoated fibers was about 630 °C. The resistance was linearly increased with the coating thickness (up to 660 °C) and getting saturated over a thickness of 120 nm. Titania coatings have been deposited using titanium tetrachloride and water. The physical appearances of the titania coatings were similar to the alumina coatings. The oxidation onset temperature of the titania coated carbon fibers was similar to the uncoated fibers but the rate of oxidation was decreased than the uncoated fibers. Two double layer coatings were deposited, alumina followed by titania (alumina/titania), and titania followed by alumina (titania/alumina). If the fibers were coated with the double layer of alumina/titania, they had almost same oxidation onset as alumina coated fibers but the rate of oxidation was decreased significantly compared to alumina coated fibers. This feature is independent of the thickness of the titania layers, at least in the regime investigated (50 nm alumina followed by 13 nm and 40 nm titania). On the other hand, the oxidation onset temperature of fibers coated with titania/alumina (20 nm titania /30 nm alumina) was approximately 750 °C. The fibers were burned completely when temperature was further increased to 900 °C and held another 60 minutes at 900 °C. This is significantly better than any other coating used in this dissertation.
ALD of titania and alumina in principle was known beforehand, this dissertation here applies this knowledge for the first time to endless fibers. Furthermore, this dissertation shows for the first time that one can deposit aluminum phosphate via ALD (planar surface as well as fibers). Aluminum phosphate might be special interest in the fiber coating because it is a rather soft material and thus might be used to obtain a weak coupling between fiber and matrix in composites. Aluminum phosphate was deposited using trimethylaluminum and triethylphosphate as precursors. Energy dispersive X-ray spectroscopy and solid state nuclear magnetic resonance spectra confirmed that the coating comprises aluminum phosphate (orthophosphate as well as other stoichiometries). Scanning electron microscopic images revealed that coatings are uniform and conformal. In cases of alumina and titania, it was observed that the coatings were delaminated from the ends of cut fibers and thus formed of clear steps. On the other hand, for aluminum phosphate coating it was observed that the border between coating and underlying fiber often being smeared out and thus formed an irregular line. It seems in case aluminum phosphate cohesion is weaker than adhesion, thus it might be act a weak interface between fiber and matrix. Alumina, titania, and double layer microtubes have been obtained after selective removal of the underlying carbon fibers. The carbon fibers were selectively removed via thermal oxidation in air at temperatures exceeding 550 °C. SEM and TEM images indicate that the inner side of the tube wall has the same morphology like the fibers. In addition, it was observed that the individual microtubes were separated from their neighbors and they had almost uniform wall thicknesses. The longest tubes had a length of 30 cm.:Bibliographische Beschreibung und Referat 2
Abstract 4
List of abbreviations 10
1. General introduction and outline of this dissertation 12
1.1 References 20
2. Atomic layer deposition: Process and reactor 25
2.1 Introduction 25
2.2 Principle of atomic layer deposition 26
2.3 Materials and methods 29
2.3.1 Precursors 29
2.3.2 Precursors transportation 31
2.3.3 Carrier and purge gas 32
2.3.4 ALD reactors 32
2.4 Flow-Type ALD reactor for fiber coating 33
2.5 Conclusion 35
2.6 References 35
3. Single layer oxide coatings 38
3.1 State of the art 38
3.2 Alumina coating using non-flammable precursors 39
3.2.1 Introduction 39
3.2.Result and discussion 39
3.3 Alumina coating using organometallic precursor 46
3.2.1 Introduction 46
3.2.2 Results and discussion 46
3.4 Titania coating using titanium tetrachloride and water 59
3.4.1 Introduction 59
3.4.2 Results and discussion 59
3.5 Experimental Part 67
3.5.1 General experiments 67
3.5.2 Alumina coating using aluminum chloride and water 69
3.5.3 Alumina coating using trimethylalumium and water 69
3.5.4 Titania coating 72
3.6 Conclusions 72
3.7 References 74
4. Coating thickness and morphology 78
4.1 Introduction 78
4.2 Results and discussion 80
4.2.1 Purge time 15 s 81
4.2.2 Purge time 30 s 85
4.2.3 Purge time 45 s to 100 s 85
4.3 Experimental part 88
4.4 Conclusions 89
4.5 References 89
5. Alumina and titania double layer coatings 91
5.1 Introduction 91
5.2 Results and discussion 92
5.3 Experimental part 102
5.4 Conclusions 103
5.5 References 103
6. Atomic layer deposition of aluminum phosphate 105
6.1 Introduction 105
6.2 Results and discussion 106
6.3 Experimental part 113
6.4 Conclusions 114
6.5 References 115
7. Alumina microtubes 117
7.1 Introduction 117
7.2 Results and discussion 118
7.2.1 Fibers before coating deposition 118
7.2.2 Coatings on the carbon fibers 118
7.2.3 Microtubes 121
7.3 Experimental part 127
7.4 Conclusions 128
7.5 References 128
8. Conclusions 131
Acknowledgements 136
Curriculum Vitae 138
Selbständigkeitserklärung 142 / Das Hauptziel dieser Dissertation bestand darin nachzuweisen, dass die Atomlagenabscheidung (engl. atomic layer deposition (ALD)) auf „endlose“ Fasern angewendet werden kann. Es wurde ein Reaktor zur Atomlagenabscheidung gestaltet, der speziell für die Beschichtung meterlanger Faserbündel geeignet ist. Aluminiumoxid, Titanoxid, Doppelschichten aus Aluminiumoxid und Titanoxid sowie Aluminiumphosphat wurden mit Hilfe des selbstgebauten Reaktors auf Kohlefaserbündel abgeschieden. Rasterelektronenmikroskopische (REM) und transmissionselektronenmikroskopische (TEM) Aufnahmen zeigten, dass die Beschichtung auf den Fasern einheitlich und oberflächentreu war. Des Weiteren wurde eine gute Adhäsion zwischen Beschichtung und Fasern beobachtet. Das Prinzip der Beschichtung mit Titanoxid und Aluminiumoxid mit Hilfe der ALD war bereits vorher bekannt und im Rahmen dieser Dissertation jedoch erstmals auf "endlose" Fasern angewendet. Des Weiteren wird in dieser Dissertation erstmals gezeigt, dass es möglich ist, Aluminiumphosphat mittels ALD abzuscheiden (sowohl auf planaren Oberflächen als auch auf Fasern). Aluminiumphosphat könnte von besonderem Interesse in der Faserbeschichtung sein, da es ein relativ weiches Material ist und könnte daher als eine Art „schwacher“ Verbindung zwischen Faser und Matrix in Kompositen dienen. Die Oxidationsbeständigkeit von beschichten Kohlefasern wurde im Vergleich zu unbeschichteten Fasern bis zu einem gewissen Grad erhöht. Monoschichten von Aluminiumoxid und Titanoxid waren dafür wenig effektiv. Aluminiumphosphatbeschichtete Fasern waren deutlich besser geeignet als die beiden anderen. Eine Doppelschicht aus Titanoxid gefolgt von Aluminiumoxid verbesserte die Oxidationsbeständigkeit nochmals deutlich gegenüber allen anderen Beschichtungen, die in dieser Dissertation verwendet wurden. Mikroröhren aus Aluminiumoxid, Titanoxid und Doppelschichten wurden durch die selektive Entfernung der zugrunde liegenden Kohlefasern erhalten. Einzelne Mikroröhren waren von benachbarten Röhren getrennt und sie weisen eine nahezu einheitliche Wanddicke auf.:Bibliographische Beschreibung und Referat 2
Abstract 4
List of abbreviations 10
1. General introduction and outline of this dissertation 12
1.1 References 20
2. Atomic layer deposition: Process and reactor 25
2.1 Introduction 25
2.2 Principle of atomic layer deposition 26
2.3 Materials and methods 29
2.3.1 Precursors 29
2.3.2 Precursors transportation 31
2.3.3 Carrier and purge gas 32
2.3.4 ALD reactors 32
2.4 Flow-Type ALD reactor for fiber coating 33
2.5 Conclusion 35
2.6 References 35
3. Single layer oxide coatings 38
3.1 State of the art 38
3.2 Alumina coating using non-flammable precursors 39
3.2.1 Introduction 39
3.2.Result and discussion 39
3.3 Alumina coating using organometallic precursor 46
3.2.1 Introduction 46
3.2.2 Results and discussion 46
3.4 Titania coating using titanium tetrachloride and water 59
3.4.1 Introduction 59
3.4.2 Results and discussion 59
3.5 Experimental Part 67
3.5.1 General experiments 67
3.5.2 Alumina coating using aluminum chloride and water 69
3.5.3 Alumina coating using trimethylalumium and water 69
3.5.4 Titania coating 72
3.6 Conclusions 72
3.7 References 74
4. Coating thickness and morphology 78
4.1 Introduction 78
4.2 Results and discussion 80
4.2.1 Purge time 15 s 81
4.2.2 Purge time 30 s 85
4.2.3 Purge time 45 s to 100 s 85
4.3 Experimental part 88
4.4 Conclusions 89
4.5 References 89
5. Alumina and titania double layer coatings 91
5.1 Introduction 91
5.2 Results and discussion 92
5.3 Experimental part 102
5.4 Conclusions 103
5.5 References 103
6. Atomic layer deposition of aluminum phosphate 105
6.1 Introduction 105
6.2 Results and discussion 106
6.3 Experimental part 113
6.4 Conclusions 114
6.5 References 115
7. Alumina microtubes 117
7.1 Introduction 117
7.2 Results and discussion 118
7.2.1 Fibers before coating deposition 118
7.2.2 Coatings on the carbon fibers 118
7.2.3 Microtubes 121
7.3 Experimental part 127
7.4 Conclusions 128
7.5 References 128
8. Conclusions 131
Acknowledgements 136
Curriculum Vitae 138
Selbständigkeitserklärung 142
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Entwicklung von Werkzeugen zur automatisierten Traktionsspeicherdimensionierung auf dieselelektrisch angetriebenen SchienenfahrzeugenMelzer, Michael 28 March 2014 (has links)
Diese Arbeit befasst sich mit der Implementierung eines Energiespeichersystems in ein dieselelektrisches Schienenfahrzeug. Ziel der Arbeit ist es mit einem automatisierten Ansatz die besten Parameter für das Energiespeichersystem zu finden. Um die geeignetsten Parameter zu bestimmen, wurde eine Optimierung basierend auf genetischen Algorithmen verwendet. Neben der Charakteristik des Energiespeichersystems wird auch dessen Betriebsstrategie untersucht und optimiert. Der Fahrstil genau wie die Leistung des Dieselmotors werden ebenfalls variiert, um die Ergebnisse der Optimierung mit und ohne Energiespeichersystem zu vergleichen. / This work deals with an implementation of an energy storage system in a diesel electric driven rail vehicle. The aim of this work is an automatic approach to find the best parameters for an energy storage system. To find the best fitting parameters an optimization based on genetic algorithms is used. Beside the characteristics of the energy storage system as well the strategy to operate it is investigated and optimized. The driving style as well as the power of the internal combustion engine are varied in order to compare the solution of the optimization with and without energy storage systems.
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Numerical simulation of an inertial spheroidal particle in Stokes flow / Numerisk simulering av en trög sfäroidisk partikel i StokesflödeBagge, Joar January 2015 (has links)
Particle suspensions occur in many situations in nature and industry. In this master’s thesis, the motion of a single rigid spheroidal particle immersed in Stokes flow is studied numerically using a boundary integral method and a new specialized quadrature method known as quadrature by expansion (QBX). This method allows the spheroid to be massless or inertial, and placed in any kind of underlying Stokesian flow. A parameter study of the QBX method is presented, together with validation cases for spheroids in linear shear flow and quadratic flow. The QBX method is able to compute the force and torque on the spheroid as well as the resulting rigid body motion with small errors in a short time, typically less than one second per time step on a regular desktop computer. Novel results are presented for the motion of an inertial spheroid in quadratic flow, where in contrast to linear shear flow the shear rate is not constant. It is found that particle inertia induces a translational drift towards regions in the fluid with higher shear rate. / Partikelsuspensioner förekommer i många sammanhang i naturen och industrin. I denna masteruppsats studeras rörelsen hos en enstaka stel sfäroidisk partikel i Stokesflöde numeriskt med hjälp av en randintegralmetod och en ny specialiserad kvadraturmetod som kallas quadrature by expansion (QBX). Metoden fungerar för masslösa eller tröga sfäroider, som kan placeras i ett godtyckligt underliggande Stokesflöde. En parameterstudie av QBX-metoden presenteras, tillsammans med valideringsfall för sfäroider i linjärt skjuvflöde och kvadratiskt flöde. QBX-metoden kan beräkna kraften och momentet på sfäroiden samt den resulterande stelkroppsrörelsen med små fel på kort tid, typiskt mindre än en sekund per tidssteg på en vanlig persondator. Nya resultat presenteras för rörelsen hos en trög sfäroid i kvadratiskt flöde, där skjuvningen till skillnad från linjärt skjuvflöde inte är konstant. Det visar sig att partikeltröghet medför en drift i sidled mot områden i fluiden med högre skjuvning.
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Kompaktní město - aneb co nového se může ještě dít v Brně mezi nádražími / Compact City - or what new is able to yet be done in Brno among railway stationsHill, Petr January 2010 (has links)
Diploma project seeks for new visions in urban solutions of area south of Brno main railway station. This place could become an interesting space for new spacial creativity in connection with the project of new railway station. The work looks for alternatives to officially presented projects with orderly and straight street layouts to create pleasing and livable public space, which would become not only the tour from station to the city, but the city itself. Six meters of height difference is used to separate road and pedestrian traffic and offers an undisturbed walking movement through the elevated pedestrian streets, which are not so deep as they would be when on the ground level, so their width could be downsized to a pleasant minumum, whereas all necesary functions (like parking and supplies areas) také place below it. Geometrical concept of two shifted hexagonal grids delivers a practical large blocks on the ground level for parking and divides the area into separate projects. The walking streets` grid fractionates big portions into more subtle building block layout so comfortable for pedestrian movement. Project also deals with development phases of area to protect it from nonreversible tenous development at the beginning. The structure works as a lively city in the very beginning of the development.
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