Microscopic, chemical and spectroscopic investigations on emeralds of various origins

In dieser Arbeit werden die mikroskopischen, chemischen und spektroskopischen Charakteristika von 260 natürlichen Smaragden und 66 synthetischen „Smaragden“ untersucht. Die Konzentrationen der chemischen Elemente von Smaragden wurden mit Hilfe der LA-ICP-MS und EMS bestimmt. Ergänzende Raman- und IR spektroskopische Methoden ermöglichen es, die Herkunft der verschiedenen Smaragde und ihrer synthetischen Analoga zu bestimmen. Auf Grund der verschiedenen Gehalte von Si, Al und Be können synthetische „Smaragde“ von natürlichen getrennt werden. Die Smaragde von Malipo, Chivor und auch synthetische „Smaragde“ können von allen anderen natürlichen Smaragden wegen der unterschiedlichen Cr-, V-, und Fe-Gehalte von einander getrennt werden. Wegen der unterschiedlichen Mg-, Na-, K-Gehalte lassen sich eher „schiefer-gebundene“ Smaragde identifizieren. Dabei wird festgestellt, dass die Unterscheidung in „schiefer-„ und „nichtschiefer-gebundene“ Smaragd-Vorkommen im Wesentlichen nur die Endglieder einer offensichtlich kristallchemisch sehr variablen Mineralchemie der Berylle, bzw. Smaragde beschreibt, dass damit aber keinesfalls eine petrologisch vertretbare Trennung belegbar ist, sondern dass Smaragde nur das jeweils regierende chemische Regime unter geeigneten Druck-Temperatur-Bedingungen widerspiegeln. Einschlussmerkmale spielen eine große Rolle bei der Unterscheidung verschiedener Lagerstätten und Herstellungsmethoden. Zum Beispiel können die Smaragde der drei Lagerstätten Santa Terezinha, Chivor, und Kafubu mit Hilfe ihrer charakteristischen Pyriteinschlüsse identifiziert werden. Die Band-Positionen und FWHM -Werte der Raman-Bande bei 1068 cm-1 und der IR-Bande bei 1200 cm-1 ermöglichen eine Differenzierung zwischen synthetischen und natürlichen Smaragden, und können darüber hinaus auch Auskunft geben über die Lagerstätte. Zusammen mit chemischen Messwerten kann bewiesen werden, dass diese Banden von Si-O Schwingungen verursacht werden. Die Raman- und IR-Banden im Bereich der Wasserschwingungen und insbesondere das IR-Band um 1140 cm-1 führen zur Trennung von Flux-Synthesen, Hydrothermal-Synthesen und natürlichen Smaragden.

Investigation of the lithium ion mobility in cyclic model compounds and their ion conducting properties

Efficient energy storage and conversion is playing a key role in overcoming the present and future challenges in energy supply. Batteries provide portable, electrochemical storage of green energy sources and potentially allow for a reduction of the dependence on fossil fuels, which is of great importance with respect to the issue of global warming. In view of both, energy density and energy drain, rechargeable lithium ion batteries outperform other present accumulator systems. However, despite great efforts over the last decades, the ideal electrolyte in terms of key characteristics such as capacity, cycle life, and most important reliable safety, has not yet been identified. rnrnSteps ahead in lithium ion battery technology require a fundamental understanding of lithium ion transport, salt association, and ion solvation within the electrolyte. Indeed, well-defined model compounds allow for systematic studies of molecular ion transport. Thus, in the present work, based on the concept of ‘immobilizing’ ion solvents, three main series with a cyclotriphosphazene (CTP), hexaphenylbenzene (HBP), and tetramethylcyclotetrasiloxane (TMS) scaffold were prepared. Lithium ion solvents, among others ethylene carbonate (EC), which has proven to fulfill together with pro-pylene carbonate safety and market concerns in commercial lithium ion batteries, were attached to the different cores via alkyl spacers of variable length.rnrnAll model compounds were fully characterized, pure and thermally stable up to at least 235 °C, covering the requested broad range of glass transition temperatures from -78.1 °C up to +6.2 °C. While the CTP models tend to rearrange at elevated temperatures over time, which questions the general stability of alkoxide related (poly)phosphazenes, both, the HPB and CTP based models show no evidence of core stacking. In particular the CTP derivatives represent good solvents for various lithium salts, exhibiting no significant differences in the ionic conductivity σ_dc and thus indicating comparable salt dissociation and rather independent motion of cations and ions.rnrnIn general, temperature-dependent bulk ionic conductivities investigated via impedance spectroscopy follow a William-Landel-Ferry (WLF) type behavior. Modifications of the alkyl spacer length were shown to influence ionic conductivities only in combination to changes in glass transition temperatures. Though the glass transition temperatures of the blends are low, their conductivities are only in the range of typical polymer electrolytes. The highest σ_dc obtained at ambient temperatures was 6.0 x 10-6 S•cm-1, strongly suggesting a rather tight coordination of the lithium ions to the solvating 2-oxo-1,3-dioxolane moieties, supported by the increased σ_dc values for the oligo(ethylene oxide) based analogues.rnrnFurther insights into the mechanism of lithium ion dynamics were derived from 7Li and 13C Solid- State NMR investigations. While localized ion motion was probed by i.e. 7Li spin-lattice relaxation measurements with apparent activation energies E_a of 20 to 40 kJ/mol, long-range macroscopic transport was monitored by Pulsed-Field Gradient (PFG) NMR, providing an E_a of 61 kJ/mol. The latter is in good agreement with the values determined from bulk conductivity data, indicating the major contribution of ion transport was only detected by PFG NMR. However, the μm-diffusion is rather slow, emphasizing the strong lithium coordination to the carbonyl oxygens, which hampers sufficient ion conductivities and suggests exploring ‘softer’ solvating moieties in future electrolytes.rn

Influence of spatial constraints in non-crystalline regions on the polymer dynamics in semi-crystalline polyethylene: a solid state NMR study

A broad variety of solid state NMR techniques were used to investigate the chain dynamics in several polyethylene (PE) samples, including ultrahigh molecular weight PEs (UHMW-PEs) and low molecular weight PEs (LMW-PEs). Via changing the processing history, i.e. melt/solution crystallization and drawing processes, these samples gain different morphologies, leading to different molecular dynamics. Due to the long chain nature, the molecular dynamics of polyethylene can be distinguished in local fluctuation and long range motion. With the help of NMR these different kinds of molecular dynamics can be monitored separately. In this work the local chain dynamics in non-crystalline regions of polyethylene samples was investigated via measuring 1H-13C heteronuclear dipolar coupling and 13C chemical shift anisotropy (CSA). By analyzing the motionally averaged 1H-13C heteronuclear dipolar coupling and 13C CSA, the information about the local anisotropy and geometry of motion was obtained. Taking advantage of the big difference of the 13C T1 relaxation time in crystalline and non-crystalline regions of PEs, the 1D 13C MAS exchange experiment was used to investigate the cooperative chain motion between these regions. The different chain organizations in non-crystalline regions were used to explain the relationship between the local fluctuation and the long range motion of the samples. In a simple manner the cooperative chain motion between crystalline and non-crystalline regions of PE results in the experimentally observed diffusive behavior of PE chain. The morphological influences on the diffusion motion have been discussed. The morphological factors include lamellar thickness, chain organization in non-crystalline regions and chain entanglements. Thermodynamics of the diffusion motion in melt and solution crystallized UHMW-PEs is discussed, revealing entropy-controlled features of the chain diffusion in PE. This thermodynamic consideration explains the counterintuitive relationship between the local fluctuation and the long range motion of the samples. Using the chain diffusion coefficient, the rates of jump motion in crystals of the melt crystallized PE have been calculated. A concept of "effective" jump motion has been proposed to explain the difference between the values derived from the chain diffusion coefficients and those in literatures. The observations of this thesis give a clear demonstration of the strong relationship between the sample morphology and chain dynamics. The sample morphologies governed by the processing history lead to different spatial constraints for the molecular chains, leading to different features of the local and long range chain dynamics. The knowledge of the morphological influence on the microscopic chain motion has many implications in our understanding of the alpha-relaxation process in PE and the related phenomena such as crystal thickening, drawability of PE, the easy creep of PE fiber, etc.