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The aim of this project is to investigate the quality of the anodic oxide coating of twotypes of aluminium alloy samples, EN AW-6014 and EN AC-43100, and to identifyappropriate test methods to assess their corrosion resistance properties. The corrosionbehaviors of the anodic oxide coating of the selected aluminium alloys with the surfacestage as-is, anodized, and anodized & scratched are evaluated through standardizedclimate chamber tests, standardized and non-standardized immersion tests, non-standardized climatic cycle tests, and electrochemical tests. The form and extent ofcorrosion that occurs on the alloy samples after the tests are evaluated by visualappearance,surfacemorphology,andthroughcomparisonofcross-sectionalmicroscopic images of samples taken before the test. This study found that impedancetests were easy and quick test methods to check the quality of the anodic oxide layer.The study also concluded that the cyclic testing in artificial seawater and immersiontest in natural seawater at 28 ºC are the most appropriate test methods to assess thecorrosion behavior of the anodic oxide coating of aluminium alloys due to theircapability of identifying the significant differences between surface stages compared tothe pre-test samples.

Cyclopropane derivatives are frequently utilized as "probes" for radical cation intermediates in a number of important chemical and biochemical oxidation. The implicit assumption in such studies is that if a radical cation is produced, it will undergo ring opening. Through a detailed examination of follow-up chemistry of electrochemically and chemically generated cyclopropylarene radical cations, we have shown that the assumption made in the use of these substrates as SET probes is not necessarily valid. While cyclopropylbenzene radical cation undergoes rapid methanol-induced ring opening (e.g., k = 8.9⁷ s⁻¹M⁻¹), the radical cations generated from 9-cyclopropylanthracenes do not undergo cyclopropane ring opening at all. The radical cations generated from cyclopropylnaphthalenes disproportionate or dimerize before undergoing ring opening. Utilizing cyclic, derivative cyclic, and linear sweep voltammetry, it was discovered that decay of radical cations generated from cyclopropylnaphthalenes in CH₃CN/CH₃OH is second order in radical cation and zero order in methanol. Anodic and Ce(IV) oxidation of all these naphthyl substrates in CH₃CN/CH₃OH led to cyclopropane ring-opened products. However, the rate constant for methanol-induced ring opening (Ar-c-C₃H₅⁺. + CH₃OH -> ArCH(·)CH₂CH₂O(H⁺)CH₃) is extremely small (<20 s⁻¹M⁻¹ for 1-cyclopropylnaphthalenes) despite the fact that ring opening is exothermic by nearly 30 kcal/mol. These results are explained on the basis of a product-like transition state for ring opening wherein the positive charge is localized on the cyclopropyl group, and thus unable to benefit from potential stabilization offered by the aromatic ring. Reactions of radical cations generated from 9-cyclopropylanthracenes in CH₃CN/CH₃CN have also been investigated electrochemically. The major products arising from oxidation of these anthryl substrates are attributable to CH₃OH attack at the aromatic ring rather than CH₃OH-induced cyclopropane ring opening. Ce(IV) oxidation of 9-cyclopropyl-10-methylanthracene and 9,10-dimethylanthracene further showed that radical cations generated from these anthryl substrates undergo neither cyclopropane ring opening nor deprotonation but nucleophilic addition. Side-chain oxidation products from Ce(IV) oxidation of methylated anthracenes arose from further reaction of nuclear oxidation products under acidic and higher temperature conditions. An analogous (more product-like) transition state picture can be applied for cyclopropane ring opening and deprotonation of these anthryl radical cations. Because of much higher intrinsic barrier to either nucleophile-induced cyclopropane ring opening or deprotonation of these anthryl radical cations, nucleophilic addition predominates. Stereoelectronic effects may be another additional factor contributing to this intrinsic barrier because the cyclopropyl group in these anthryl systems adopts a perpendicular conformation which may not meet the stereoelectronic requirements for cyclopropyl ring opening at either the radical cation or dication stage. / Ph. D.

Das Ziel dieser Dissertation besteht darin, einen Beitrag zur technologischen, ökonomischen und ökologischen Weiterentwicklung der anodischen Verfahren zur Oberflächenkeramisierung von Aluminium zu leisten. Die Arbeit ist in zwei thematische Schwerpunkte untergliedert. Im ersten Teil wird für die Hartanodisation eine hinsichtlich eines geringeren Energieeinsatzes optimierte Elektrolytzusammensetzung identifiziert und mit einem optimierten galvanostatischen Pulsmuster simultan appliziert. Im Ergebnis kann die Gesamtleistungsaufnahme um ca. 6 % reduziert werden, ohne die mechanischen Eigenschaften der Oxidschichten zu mindern. Im zweiten Schwerpunkt werden das Lichtbogen- und das Flammspritzen mit der plasmaelektrolytischen anodischen Oxidation kombiniert, um verschleißbeständige Aluminiumoxidschichten auf Stahl-, Titan- und Magnesiumsubstraten zu applizieren. Neben einer umfangreichen Mikrostrukturanalyse (REM, EDX, XRD, EBSD) werden die mechanischen Eigenschaften der Schichten untersucht und mit atmosphärisch plasmagespritzten Al2O3-Schichten verglichen. Insbesondere Oxidschichten auf lichtbogengespritztem AlCu4Mg1 zeigen dabei eine hohe Härte sowie eine sehr gute Verschleißbeständigkeit. / The aim of the present work is to contribute to the technological, economic and ecological improvement of the anodic processes for the surface ceramization of aluminum. The work is subdivided into two thematic priorities. In the first part, for the hard anodizing process an optimized electrolyte composition for a lower energy input is identified and applied simultaneously with an optimized galvanostatic pulse regime. As a result, the total power consumption can be reduced by approximately 6% without reducing the mechanical properties of the oxide coatings. In the second focus, arc and flame spraying are combined with plasma electrolytic anodic oxidation to apply wear resistant aluminum oxide coatings on steel, titanium and magnesium substrates. In addition to a comprehensive microstructural analysis (SEM, EDX, XRD, EBSD), the mechanical properties of the layers are investigated and compared with atmospheric plasma sprayed Al2O3 coatings. In particular, oxide layers formed on arc sprayed AlCu4Mg1 coatings show a high hardness as well as very good wear resistance.

Die vorliegende Arbeit enthält neuartige Ergebnisse festkörperanalytischer Untersuchungen zu Synthese, Struktur und Eigenschaften von anodischen Konversionsschichten auf Vanadium und Zirkonium. Schwerpunkte sind die Darstellung anodischer Oxidschichten auf den Metallen Vanadium und Zirkonium sowie ihre Charakterisierung mit ausgewählten Methoden der Festkörperanalytik. Am Beispiel des Vanadiums wird die anodische Schichtbildung in Essigsäurebasiselektrolyten untersucht. Unter anderem wird anhand von Strom-Spannungs-Kennlinien das unterschiedliche anodische Verhalten der physikalisch ähnlichen Metalle Vanadium und Zirkonium diskutiert. Neben den Methoden der Röntgenbeugung, Infrarotspektroskopie, Photoelektronenspektroskopie und Elektronenmikroskopie wird die Ramanspektroskopie als ein geeignetes Mittel zur Unterscheidung der Oxidphasen verwendet. Die amorphen VOx-Schichten und kristallinen ZrO2- bzw. modifizierten Schichten wurden sowohl unter anodischen als auch unter elektrochemischen Plasmabedingungen erzeugt. Die Korrelation zwischen Schichtstruktur und Syntheseverfahren wird herausgearbeitet.

La conversion thermoélectrique a suscité un regain d'intérêt en raison des possibilités d'augmenter l'efficacité tout en exploitant les effets de taille. Par exemple, les nanofils montrent théoriquement une augmentation des facteurs de puissance ainsi qu'une réduction du transport des phonons en raison d'effets de confinement et/ou de taille. Dans ce contexte, le diamètre des nanofils devient un paramètre crucial à prendre en compte pour obtenir des rendements thermoélectriques élevés. Une approche habituelle consiste à réduire la conductivité thermique phononique dans les nanofils en améliorant la diffusion sur les surfaces tout en réduisant les diamètres.Dans ce travail, la caractérisation thermique d'une forêt dense de nanofils de silicium, germanium, silicium-germanium et alliage Bi2Te3 est réalisée par une méthode 3-omega très sensible. Ces forêts de nanofils pour le silicium, le germanium et les alliages silicium-germanium ont été fabriqués selon une technique "bottom-up" suivant le mécanisme Vapeur-Liquide-Solide en dépôt chimique en phase vapeur. La croissance assistée par matrice et la croissance par catalyseurs en or des nanofils à diamètres contrôlés ont été réalisés à l'aide d'alumine nanoporeuse comme matrice. Les nanofils sont fabriqués selon la géométrie interne des nanopores, dans ce cas le profil de surface des nanofils peut être modifié en fonction de la géométrie des nanopores. Profitant de ce fait, la croissance à haute densité de nanofils modulés en diamètre a également été démontrée, où l'amplitude et la période de modulation peuvent être facilement contrôlées pendant la fabrication des matrices. Même en modulant les diamètres pendant la croissance, les nanofils ont été structurellement caractérisés comme étant monocristallins par microscopie électronique à transmission et analyse par diffraction des rayons X.La caractérisation thermique de ces nanofils a révélé une forte diminution de la conductivité thermique en fonction du diamètre, dont la réduction était principalement liée à une forte diffusion par les surfaces. La contribution du libre parcours moyen à la conductivité thermique observée dans ces matériaux "bulk" varie beaucoup, Bi2Te3 ayant une distribution en libre parcours moyen (0,1 nm à 15 nm) très faible par rapport aux autres matériaux. Même alors, des conductivités thermiques réduites (~40%) ont été observées dans ces alliages attribuées à la diffusion par les surfaces et par les impuretés. D'autre part, le silicium et le germanium ont une conductivité thermique plus élevée avec une plus grande distribution de libre parcours moyen. Dans ces nanofils, une réduction significative (facteur 10 à 15 ) a été observée avec une forte dépendance avec la taille des nanofils.Alors que les effets de taille réduisent la conductivité thermique par une meilleure diffusion sur les surfaces, le dopage de ces nanofils peut ajouter un mécanisme de diffusion par différence de masse à des échelles de longueur atomique. La dépendance en température de la conductivité thermique a été déterminée pour les nanofils dopés de silicium afin d'observer une réduction de la conductivité thermique à une valeur de 4,6 W.m-1K-1 dans des nanofils de silicium fortement dopés avec un diamètre de 38 nm. En tenant compte de la conductivité électrique et du coefficient Seebeck calculé, on a observé un ZT de 0,5. Avec l'augmentation significative de l'efficacité du silicium en tant que matériau thermoélectrique, une application pratique réelle sur les appareils n'est pas loin de la réalité. / Thermoelectric conversion has gained renewed interest based on the possibilities of increasing the efficiencies while exploiting the size effects. For instance, nanowires theoretically show increased power factors along with reduced phonon transport owing to confinement and/or size effects. In this context, the diameter of the nanowires becomes a crucial parameter to address in order to obtain high thermoelectric efficiencies. A usual approach is directed towards reducing the phononic thermal conductivity in nanowires by achieving enhanced boundary scattering while reducing diameters.In this work, thermal characterisation of a dense forest of silicon, germanium, silicon-germanium and Bi2Te3 alloy nanowires is done through a sensitive 3ω method. These forest of nanowires for silicon, germanium and silicon-germanium alloy were grown through bottom-up technique following the Vapour-Liquid-Solid mechanism in Chemical vapour deposition. The template-assisted and gold catalyst growth of nanowires with controlled diameters was achieved with the aid of tuneable nanoporous alumina as templates. The nanowires are grown following the internal geometry of the nanopores, in such a case the surface profile of the nanowires can be modified according to the fabricated geometry of nanopores. Benefiting from this fact, high-density growth of diameter-modulated nanowires was also demonstrated, where the amplitude and the period of modulation can be easily tuned during the fabrication of the templates. Even while modulating the diameters during growth, the nanowires were structurally characterised to be monocrystalline through transmission electron microscopy and X-ray diffraction analysis.The thermal characterisation of these nanowires revealed a strong diameter dependent decrease in the thermal conductivity, where the reduction was predominantly linked to strong boundary scattering. The mean free path contribution to the thermal conductivity observed in the bulk of fabricated nanowire materials vary a lot, where Bi2Te3 has strikingly low mean free path distribution (0.1 nm to 15 nm) as compared to the other materials. Even then, reduced thermal conductivities (~40%) were observed in these alloys attributed to boundary and impurity scattering. On the other hand, silicon and germanium have higher thermal conductivity with a larger mean free path distribution. In these nanowires, a significant reduction (10-15 times) was observed with a strong dependence on the size of the nanowires.While size effects reduce the thermal conductivity by enhanced boundary scattering, doping these nanowires can incorporate mass-difference scattering at atomic length scales. The temperature dependence of thermal conductivity was determined for doped nanowires of silicon to observe a reduction in thermal conductivity to a value of 4.6 W.m-1K-1 in highly n-doped silicon nanowires with 38 nm diameter. Taking into account the electrical conductivity and calculated Seebeck coefficient, a ZT of 0.5 was observed. With these significant increase in the efficiency of silicon as a thermoelectric material, a real practical application to devices is not far from reality.

Doctor of Philosophy / Department of Chemistry / Takashi Ito / Self-organized nanoporous materials have drawn a lot of attention because the uniform, highly dense, and ordered cylindrical nanopores in these materials provide a unique platform for chemical separations and chemical sensing applications. Here, we explore self-organized nanopores of PS-b-PMMA diblock copolymer thin films and anodic gallium oxide for chemical separations and sensing applications. In the first study, cyclic voltammograms of cytochrome c on recessed nanodisk-array electrodes (RNEs) based on nanoporous films (11, 14 or 24 nm in average pore diameter; 30 nm thick) derived from polystyrene-poly(methylmethacrylate) diblock copolymers were measured. The faradic current of cytochrome c was observed on RNEs, indicating the penetration of cytochrome c (hydrodynamic diameter ≈ 4 nm) through the nanopores to the underlying electrodes. Compared to the 24-nm pores, the diffusion of cytochrome c molecules through the 11- and 14-nm pores suffered significantly larger hindrance. The results reported in this study will provide guidance in designing RNEs for size-based chemical sensing and also for controlled immobilization of biomolecules within nanoporous media for biosensors and bioreactors. In another study, conditions for the formation of self-organized nanopores of a metal oxide film were investigated. Self-organized nanopores aligned perpendicular to the film surface were obtained upon anodization of gallium films in ice-cooled 4 and 6 M aqueous H2SO4 at 10 V and 15 V. The average pore diameter was in the range of 18 ~ 40 nm, and the anodic gallium oxide was ca. 2 µm thick. In addition, anodic formation of self-organized nanopores was demonstrated for a solid gallium monolith incorporated at the end of a glass capillary. Nanoporous anodic oxide monoliths formed from a fusible metal will lead to future development of unique devices for chemical sensing and catalysis. In the final study, surface chemical property of self-organized nanoporous anodic gallium oxide is explored through potentiometric measurements. The nanoporous anodic and barrier layer gallium oxide structures showed slow potentiometric response only at acidic pH (≤ 4), in contrast to metallic gallium substrates that exhibited a positive potentiometric response to H⁺ over the pH range examined (3-10). The potentiometric response at acidic pH probably reflects some chemical processes between gallium oxide and HCl.

In this work the gallium and bismuth film plating in situ and ex situ processes were investigated. The metal film plating conditions for determination of heavy metals in water samples were optimized. When depositing Bi films on glassy carbon electrode it was found, that the addition of Br-1 changes the BiFE morphology making it more uniform and forming crystalline aggregates. The reoxidation peak of Bi was shifted to more negative potentials showing the electrocatalytic effect of bromide for the bismuth film. The addition of the other metal ions to the deposition solutions caused changes in the morphology of the Bi film It has been shown, that Cd was slowing the Bi film deposition and Pb was catalyzing this deposition. Zn(II), Cd(II), Cu(II) and Pb(II) ions were determined in the water samples using bismuth film electrode. The linear calibration curve of each metal was obtained. Good linear responses of the peak area vs. concentration were obtained for Zn(II), Cd(II), Pb(II) and Cu (II) with correlation coefficients of 0.997, 0.997, 0.999 and 0.998 respectively. The possibilities of gallium film plating were studied. The glassy carbon substrate was chosen for optimization. The optimized deposition conditions were: supporting electrolyte 0.1 M acetate buffer, deposition potential -1.7 V, deposition time 120 s, deposition temperature 40oC. The gallium influence on Pb(II) and Cd(II) deposition at the glassy carbon electrode was studied. It has been shown that Pb(II) and Cd(II)... [to full text] / Šiame darbe tiriama galio ir bismuto plėvelinių elektrodų formavimo in situ ir ex situ metodais ypatumai skirtingose sistemose. Optimizuotos bismuto ir galio plėvelinių elektrodų panaudojimo sąlygos sunkiųjų metalų koncentracijos nustatymui. Atliekant bismuto plėvelės nusodinimą ant stikliškosios anglies elektrodo nustatyta, kad papildomas Br- pridėjimas į tiriamąjį tirpalą keičia bismuto plėvelės morfologines savybes ir formuojasi tolygesnė bismuto plėvelė sudarydama kristalines struktūras. Reoksidacinė bismuto smailė pasislenka į neigiamesnių potencialo verčių pusę, kas rodo elektrokatalizinį Br- efektą bismuto plėvelės formavimuisi. Nustatyta, kad Cd(II) pridėjimas į tiriamąjį tirpalą lemia lėtesnį bismuto plėvelės nusodinimą, o Pb(II) pridėjimas katalizuoja bismuto plėvelės nusodinimą. Taip pat nustatyta, kad Pb(II) katalizuoja ir kitų metalų jonų nusodinimą. Bismuto plėvelinis elektrodas sėkmingai pritaikytas sunkiųjų metalų Cu(II), Zn(II), Pb(II), Cd(II) koncentracijos nustatymui pramoniniuose vandens mėginiuose. Gautos Zn(II), Cd(II), Cu(II) ir Pb(II) kalibravimo kreivės, kurių korealiacijos koeficientai atitinkamai yra 0,997, 0,997, 0,999 ir 0,998. Optimizuotos galio plėvelės nusodinimo sąlygos ant stikliškosios anglies elektrodo. Geriausi rezultatai gauti atliekant galio plėvelės nusodinimą 0,1 M acetatiniame buferyje (pH = 4,5) 40o C temperatūroje. Optimizuotas nusodinimo laikas ir potencialas atitinkamai yra 120 s ir -1,7 V. Tiriant galio jonų įtaką Pb(II) ir... [toliau žr. visą tekstą]