Das Ziel dieser Arbeit ist die ganzheitliche Erfassung der Haftmechanismen zwischen Metallbeschichtungen (Kupfer, Aluminium) und Polymersubstraten (Polyetheretherketon) funktionalisiert durch Draht-Lichtbogenspritzen. Hierzu werden die Vorbehandlung sowie der Applikationsprozess erforscht. An den hergestellten Fügeverbindungen erfolgen unterschiedliche mechanische Versuche zur Ermittlung der Hafteigenschaften und der Auswirkungen des Beschichtungsvorgangs auf die Substrate. Zur Analyse des Interfaces kommen mikroskopische (REM, TEM, HR-TEM), spektroskopische (EDX) und diffraktometrische (SAED, XRD) Verfahren zum Einsatz. Anhand der Ergebnisse erfolgt die Durchdringung des Anbindungsprozesses. Die thermisch und mechanisch bedingten Einflüsse auf das Substrat sowie dessen Eigenschaftsprofil sind in ihrer geometrischen Ausdehnung (mikroskopisch) begrenzt. Die Bestätigung für die mechanische Verklammerung wird erbracht. Durch eine HR-TEM-Untersuchung des Interfaces erfolgt der Nachweis von Oxiden und Hydroxiden. Diese stellen die Voraussetzung für physikalisch und chemisch bedingte Haftmechanismen dar.:1 Einleitung und Problemstellung 19 2 Stand von Wissenschaft und Technik 21 2.1 Hochpolymere Werkstoffe 21 2.1.1 Bildungsreaktionen 21 2.1.2 Einteilung der Polymere 24 2.1.3 Mechanische und thermische Eigenschaften 28 2.2 Thermisches Spritzen nach DIN EN 657 28 2.2.1 Draht-Lichtbogenspritzen 30 2.2.2 Substratvorbehandlung nach DIN EN 13507 31 2.2.3 Analyse von thermisch applizierten Schichten 33 2.2.3.1 Haftzugfestigkeit (DIN EN 582) 33 2.2.3.2 Eigenspannungen 37 2.3 Polyetheretherketon als Konstruktions- und Substratwerkstoff 41 2.4 Haftmechanismen zwischen Polymer und Metall 47 2.4.1 Haftungstheorien 47 2.4.2 Resultierende Gesamthaftung 55 2.4.3 Metalloxid-Polymer-Komplexe 56 3 Zielstellung und methodische Vorgehensweise 59 4 Metallisierung von Polyetheretherketon 62 4.1 Analyse der Substratwerkstoffe 62 4.2 Auswahl der Spritzzusatzwerkstoffe 67 4.3 Substratvorbehandlung 68 4.4 Applikation metallischer Schichten durch Draht-Lichtbogenspritzen 77 5 Ergebnisse und Diskussion 85 5.1 Metallographische Analyse 85 5.2 Mechanische Charakterisierung des funktionalisierten Polyetheretherketon 90 5.2.1 Nano-Eindringprüfung 90 5.2.2 Haftzugversuch 95 5.2.3 Zugversuch und Grauwertanalyse 102 5.2.4 Scratch-Test 109 5.2.5 Biegeversuch 115 5.2.6 Schlagbiegeversuch (CHARPY) 119 5.2.7 Fazit der mechanischen Charakterisierung 122 5.3 Eigenspannungsanalyse (Krümmungsmethode) 124 5.4 Analyse des Interfaces 129 5.4.1 Rasterelektronenmikroskopie und Röntgenspektroskopie 129 5.4.2 Hochauflösende Transmissionselektronenmikroskopie (HR-TEM) 134 6 Fazit 142 7 Zusammenfassung 144 8 Ausblick 147 9 Literaturverzeichnis 148 10 Anhang 156 / The aim of this work is the holistic detection of the adhesion mechanisms between metal coatings (copper, aluminum) and polymer substrates (polyetheretherketone) functionalized by wire arc spraying. For this purpose, the pretreatment and the application process are researched. Different mechanical tests are carried out on the manufactured joints to determine the adhesive properties and the effects of the coating process on the substrates. For the analysis of the interface, microscopic (SEM, TEM, HR-TEM), spectroscopic (EDX) and diffractometric (SAED, XRD) methods are used. Based on the results, the investigation of the connection process is carried out. The ther-mally and mechanically conditioned influences on the substrate as well as its property profile are limited in their geometrical extent (microscopically). The confirmation for the mechanical clamping is provided. An HR-TEM examination of the interface reveals the presence of oxides and hydroxides. These are the requirements for physically and chemically induced adhesive mechanisms.:1 Einleitung und Problemstellung 19 2 Stand von Wissenschaft und Technik 21 2.1 Hochpolymere Werkstoffe 21 2.1.1 Bildungsreaktionen 21 2.1.2 Einteilung der Polymere 24 2.1.3 Mechanische und thermische Eigenschaften 28 2.2 Thermisches Spritzen nach DIN EN 657 28 2.2.1 Draht-Lichtbogenspritzen 30 2.2.2 Substratvorbehandlung nach DIN EN 13507 31 2.2.3 Analyse von thermisch applizierten Schichten 33 2.2.3.1 Haftzugfestigkeit (DIN EN 582) 33 2.2.3.2 Eigenspannungen 37 2.3 Polyetheretherketon als Konstruktions- und Substratwerkstoff 41 2.4 Haftmechanismen zwischen Polymer und Metall 47 2.4.1 Haftungstheorien 47 2.4.2 Resultierende Gesamthaftung 55 2.4.3 Metalloxid-Polymer-Komplexe 56 3 Zielstellung und methodische Vorgehensweise 59 4 Metallisierung von Polyetheretherketon 62 4.1 Analyse der Substratwerkstoffe 62 4.2 Auswahl der Spritzzusatzwerkstoffe 67 4.3 Substratvorbehandlung 68 4.4 Applikation metallischer Schichten durch Draht-Lichtbogenspritzen 77 5 Ergebnisse und Diskussion 85 5.1 Metallographische Analyse 85 5.2 Mechanische Charakterisierung des funktionalisierten Polyetheretherketon 90 5.2.1 Nano-Eindringprüfung 90 5.2.2 Haftzugversuch 95 5.2.3 Zugversuch und Grauwertanalyse 102 5.2.4 Scratch-Test 109 5.2.5 Biegeversuch 115 5.2.6 Schlagbiegeversuch (CHARPY) 119 5.2.7 Fazit der mechanischen Charakterisierung 122 5.3 Eigenspannungsanalyse (Krümmungsmethode) 124 5.4 Analyse des Interfaces 129 5.4.1 Rasterelektronenmikroskopie und Röntgenspektroskopie 129 5.4.2 Hochauflösende Transmissionselektronenmikroskopie (HR-TEM) 134 6 Fazit 142 7 Zusammenfassung 144 8 Ausblick 147 9 Literaturverzeichnis 148 10 Anhang 156

The adsorption and coadsorption of sulfur and oxygen on the Ir(110) surface was investigated by scanning tunneling microscopy (STM), low-energy electron diffraction (LEED), and Auger electron spectroscopy (AES). The clean Ir(110) surface forms alternating (331) and (33-1) minifacets, resulting in a mesoscopically rippled surface. Upon chemisorption of sulfur or oxygen and subsequent annealing, the surface structure is changed. In the following, the results concerning sulfur and oxygen adsorption will be summarized before addressing the coadsorption system. Sulfur adsorption: At sulfur coverages of 0.1-0.2 ML, the Ir(110) surface adopts a (1x2) missing-row configuration similar to clean Au(110) and Pt(110). The sulfur-stabilized Ir(110)-(1x2) does not show any evidence for the preference of (111) faceted steps, and consequently does not form a mesoscopic fish-scale pattern. The latter was observed on the (110) surfaces of Au and Pt, and was found to be driven by the preference for (111) step facets. On Ir(110), no such preference seems to exist, since (331) step facets are frequently observed. With respect to the adsorbed sulfur, no extended islands are observed, indicating repulsive adsorbate-adsorbate interactions. At sulfur coverages near 0.5 ML, a p(2x2) structure with p2mg (glide-plane) symmetry is observed. The adsorption site and structural model derived by STM are compatible with an earlier LEED analysis of that structure: S adsorbs in threefold coordinated fcc hollow sites above the (111) facets formed by the non-missing substrate rows. At coverages higher than 0.5 ML, a c(2x4) LEED pattern with additional faint streaks in the [-110] azimuth is observed. STM reveals that the streaks are due to pairs of sulfur atoms (dimers, for brevity) in a second adsorbate layer, that can be desorbed by heating to 1100 K. A structural model is derived on the basis of the STM results, showing the dimer atoms in on-top positions over sulfur atoms of the first adsorbate layer. When the surface is completely covered by the dimers, the surface is saturated at 0.75 ML. Oxygen adsorption: In agreement with earlier reports, oxygen adsorption and subsequent annealing to 700-900 K results in an unreconstructed (1x1) surface, covered by a c(2x2)-O overlayer at 0.5 ML coverage. Coadsorption of oxygen on an S-precovered surface (S-coverage below 0.5 ML) leads to a phase separation of the adsorbates (competitive adsorption). At low coverages, oxygen forms a p(2x2)-O phase, whereas at higher O-coverages a compression into a (1x2)-O phase is observed. Postannealing the (1x2)-O phase at 900 K in vacuum leads to a reduction of the sulfur concentration, indicating sulfur oxidation. Interestingly, the p(2x2)-O phase does not seem to be reactive, according to the AES results. A possible explanation may be that the more densely packed (1x2)-O phase can be regarded as an activated structure. This is also supported by the STM results. At S-coverages above 0.5 ML, the surface is completely poisoned with respect to oxygen adsorption. Nevertheless, heating the sulfur saturated Ir(110)-c(2x4)-S structure in an oxygen atmosphere, the sulfur concentration gradually drops to zero. At intermediate stages of this oxidation process, island formation is observed by STM, but the underlying formation processes remain to be resolved.

The synthesis and properties of metal phosphonates prepared using piperazine-based bisphosphonic acids have been investigated. The ligands N,N’-piperazinebis(methylenephosphonic acid) (H₄L), and the 2-methyl (H₄L-Me) and 2,5-dimethyl (H₄L 2,5-diMe) derivatives have been prepared using a modified Mannich reaction. Hydrothermal reaction of gels prepared from metal (II) acetates and the bisphosphonic acids results in the synthesis of four structures: STA-12, Ni VSB-5, Co H₂L.H₂O and Mg H₂L. STA-12, synthesised by reaction of Mn, Fe, Co or Ni acetate with H₄L or H₄L-Me, has been investigated further. STA-12 crystallises in the space group R⁻₃, and Ni STA-12 is the most crystalline version. Its structure was solved from synchrotron data (a = b = 27.8342(1) Å, c = 6.2421(3) Å, α = β = 90°, γ = 120°), and it has large 10 Å hexagonal shaped pores. Helical chains of Ni octahedra are coordinated by the ligands, resulting in phosphonate tetrahedra pointing towards the pore space. Water is present, both coordinated to the Ni²⁺ cations and physically adsorbed in the pores. Mixed metal structures based on Ni STA-12, where some Ni is replaced in the gel by another divalent metal (Mg, Mn, Fe or Co) can also be synthesised. Dehydration of STA-12 results in two types of behaviour, depending on the metal present. Rhombohedral symmetry is retained on dehydration of Mn and Fe STA-12, the a cell parameter decreasing compared to the as-prepared structures by 2.42 Å and 1.64 Å respectively. Structure solution of dehydrated Mn STA-12 indicates changes in the torsion angles of the piperazine ring bring the inorganic chains closer together. Fe and Mn STA-12 do not adsorb N₂, which is thought to be due to the formation of an amorphous surface layer. Dehydration of Ni and Co STA-12 causes crystallographic distortion. Three phases were isolated for Ni STA-12: removal of physically adsorbed water results in retention of rhombohedral symmetry, while dehydration at 323 K removes some coordinated water forming a triclinic structure. A fully dehydrated structure (dehydrated at 423 K) was solved from synchrotron data (a = 6.03475(5) Å, b = 14.9156(2) Å, c = 16.1572(7) Å, α = 112.5721(7)°, β = 95.7025(11)°, γ = 96.4950(11)°). The dehydration mechanism, followed by UV-vis and Infra-red spectroscopy, involves removal of water from the Ni²⁺ cations and full coordination of two out of three of the phosphonate tetrahedra forming three crystallographically distinct Ni and P atoms. No structural distortion takes place on dehydration of Ni and Co STA-12 prepared using the methylated bisphosphonate, and the solids give a higher N₂ uptake as a result. Dehydrated Ni and Co STA-12 were tested for adsorption performance for fuel related gases and probe molecules. Investigations were undertaken at low temperature with H₂, CO and CO₂, and ambient temperature with CO₂, CH₄, CH₃CN, CH₃OH and large hydrocarbons. Due to the presence of lower crystallinity, Co STA-12 has an inferior adsorption performance to Ni STA-12, although it has similar adsorption enthalpies for CO₂ at ambient temperature (-30 to -35 kJ mol⁻¹). Ni STA-12 adsorbs similar amounts of CO₂ and N₂ at low temperature, indicating the adsorption mechanisms are similar. Also, it adsorbs 10 × more CO₂ than CH₄ at low pressure, meaning it could be used for separation applications. Ni STA-12 adsorbs 2 mmol g⁻¹ H₂ with an enthalpy of -7.5 kJ mol⁻¹, the uptake being due to adsorption on only one-third of the Ni²⁺ cations. The uptake for CO is 6 mmol g⁻¹, with adsorption enthalpies ranging from -24 to -14 kJ mol⁻¹. This uptake is due to adsorption on all the Ni²⁺, meaning the adsorption enthalpies are high enough to allow the structure to relax. This is also observed for adsorption of CH₃CN and CH₃OH, where there is a return to rhombohedral symmetry after uptake. The adsorption sites in dehydrated Ni and Co STA-12 were investigated via Infra-red spectroscopic analysis of adsorbed probe molecules (H₂, CO, CO₂, CH₃CN and CH₃OH). The results indicate the adsorption sites at both low and ambient temperature are the metal cations and the P=O groups. The metal cation sites are also characterised as Lewis acids with reasonable strength. STA-12 was shown to have acidic activity for the liquid phase selective oxidations of 1-hexene and cyclohexene, although there is evidence active sites are coordinated by products and/or solvents during the reaction. STA-12 also demonstrates basic activity for the Knoevenagel condensation of ethyl cyanoacetate and benzaldehyde. Modification of STA-12 by adsorption of diamine molecules causes a slight increase in the basicity, and the highest conversions are where water and diamine molecules are both present.

Les travaux présentés dans ce manuscrit de doctorat s'inscrivent dans la thématique du stockage inter-saisonnier de l'énergie solaire thermique pour l'habitat et le tertiaire (eau chaude sanitaire et chauffage). Le stockage thermochimique en air humide est une des solutions les plus prometteuses, en particulier avec un réacteur à lit fixe. Le bromure de strontium et l'alun de potassium ont été sélectionnés comme réactifs pour leurs caractéristiques énergétiques lors de réactions d'hydratation et de déshydratation. L'étude est constituée d'avancées théoriques, de nombreuses expérimentations et d'un modèle numérique détaillé. Une étude thermodynamique a démontré l'existence d'une droite de charge qui relie les conditions d'entrée et de sortie de l'air humide au passage du réactif. Les équations régissant les réactions chimiques, les transferts massiques et thermiques et la conservation de la quantité de mouvement ont été établies et un modèle numérique monodimensionnel couplant ces phénomènes a été développé. Des essais sur différents échantillons des deux sels et pour divers conditions opératoires ont été effectués dans le but de comprendre les phénomènes physico-chimiques ainsi que pour valider l'étude théorique et le modèle numérique. / This PhD thesis focuses on seasonal solar thermal energy storage for household applications such as production of heat and domestic hot water. Thermochemical storage was chosen for that purpose. The specific solid/gas reactions with water vapor, also called hydration/dehydration reactions, were used with a multi-scale global approach. The level of the reactor was identified as the critical level of that multi-scale approach. As a consequence, the integrated fixed-bed reactor technology in a moist air open loop system was adopted. A theoretical, experimental and numerical methodology was used for the study where strontium bromide and potassium alum salts were chosen as reactive materials. The corresponding reactions are: + 5 (H2O) ↔ (with Δhr=67.4 kJ/molwater and Δsr=175 J/K.molwater) + 9 (H2O) ↔ < KAl(SO4)2.12H2O > (with Δhr=44.2 kJ/molwater and Δsr=109.8 J/K.molwater) The first salt exhibits very good thermochemical properties. On the other hand, the main advantages of potassium alum are its low cost and the fact that it presents no sanitary risk. More than 30 cycles with 3 different samples of potassium alum and more than 25 cycles with 4 samples of strontium bromide under various stationary and dynamic operating conditions were carried out in order to understand the phenomena. The main experimental results were the following ones: • A very good stability and reproducibility of physical and chemical phenomena was observed for both materials. • A thermal reaction front was also observed. • A thermal hysteresis for both salts was found. • Based on that last observation a theoretical equation named charge-discharge line was developed. Experimental results with both salts validate the charge-discharge line theory. • A correlation between reaction kinetics, temperature rise due to the reaction, power of the reaction and the operating conditions was observed. The criterion for that correlation is the affinity of the reaction. A proportional correlation between affinity and reaction kinetics, temperature rise and power of the reaction was observed. • Spontaneous hydration and over-hydration reactions do not produce any particular difficulties or problems. • Pressure drop through the reactor and evolution of salts volume were also measured. Experimental energy density was measured in the range of 350 kWh/m3 for strontium bromide and 240 kWh/m3 for the potassium alum. • In general, strontium bromide is a very good candidate material for seasonal storage, while potassium alum cannot provide satisfying temperature rise and power. The equations governing those phenomena were also established and used to develop a 1D numerical model with partial differential equations coupling chemical phenomena, mass and thermal transfer phenomena and momentum conservation. Verification, validation and confirmation of this model under a very large range of operating conditions were carried out based on the experimental results of strontium bromide. A total of 19 different test cases were studied in order to validate the numerical model. The effect of humidity, temperature, quantity of reactive material and air flow were studied both for stationary and dynamic conditions. The numerical model was able to provide very satisfying results.