Analytische Chemie
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Organisationseinheit der BAM
- 1 Analytische Chemie; Referenzmaterialien (617)
- 6 Materialchemie (395)
- 8 Zerstörungsfreie Prüfung (293)
- 6.3 Strukturanalytik (171)
- 1.2 Biophotonik (137)
- 6.1 Oberflächen- und Dünnschichtanalyse (137)
- 1.1 Anorganische Spurenanalytik (120)
- 1.9 Chemische und optische Sensorik (92)
- 8.2 Zerstörungsfreie Prüfmethoden für das Bauwesen (85)
- 1.8 Umweltanalytik (77)
Paper des Monats
- ja (29)
Vortragstagung "Zerstörungsfreie Materialprüfung" vom 28. bis 30. Mai 1962 in Garmisch-Partenkirchen
(1962)
Die „Gesellschaft zur Förderung Zerstörungsfreier Prüfverfahren e. V.“ und der „Unterausschuß für Zerstörungsfreie Prüfung des Werkstoffausschusses beim Verein Deutscher Eisenhüttenleute“ hatten mit Garmisch-Partenkirchen als Ort für ihre Jahrestagung eine gute Wahl getroffen. Die Aula des Gymnasiums gab den Vorträgen einen Rahmen passender Größe, und Gelegenheiten zum geselligen Beisammensein waren reichlich vorhanden; vor allem die Erinnerung an den gemeinsamen Abend im „Bauerntheater“ wird den meisten Tagungsteilnehmern noch manches Schmunzeln entlocken.
Das Vortragsprogramm enthielt in gut ausgewogener Zusammenstellung Beiträge über Grundlagen und Anwendungen verschiedener Prüfmethoden sowie Erfahrungsberichte. Daß es in mehreren Vorträgen um die Gewinnung objektiver Maßstäbe bei der Deutung von Prüfergebnissen ging, ist besonders hervorzuheben.
Leider waren erst die Exkursionen am 30. 5. nach München zur Fa. Kraus-Maffei (die Reaktorbesichtigung war kurzfristig von Garching aus abgesagt worden) und zum Walchensee-Kraftwerk mit einem Umweg über den Sylvensteinspeicher vom Wetter nicht begünstigt. Vor allem den Damen hätte man für ihr an sich sehr reizvolles Programm wenigstens etwas mehr Wärme und Sonne gewünscht.
Den Organisatoren dieser Tagung gebührt volle Anerkennung für das gelungene Programm. Den vielen Regen und die nötig gewordene Änderung der Exkursionen kann man ihnen nicht zum Vorwurf machen.
Das Prinzip der Massenspektrometrie wird kurz erläutert. Anwendungsbereich und Grenzen der massenspektrometrischen Strukturuntersuchung werden am Beispiel von Massenspektren reiner Kohlenwasserstoffe demonstriert. Die Strukturgruppenanalyse von Mineralölen - Fragmentpeak-Methode, Molekülpeak-Methode - wird beschrieben.
Number-average molecular weights and inherent viscosities were found for the soluble members of an alkoxy-substituted copolyester series. A liquid-crystalline (high-temperature) phase was distinguisehd by IR and wide-angle X-ray scattering on molten and quenched samples in form of a nematic sanidic phase. In this phase no relationship exists between the orientation of the aromatic polyester backbone and that of the laterally attracted alkoxy groups. Further, it was proven by IR that only the polyester backbone can be aligned by shear stress. If the applied shear stress is very strong, the orientation of the stiff backbone becomes sensitive to disturbance caused by mechanical forces.
The main component of this program is a simultaneous representation of the unit cell and the calculated powder pattern. It allows the manipulation of the Crystal structure by moving selected atoms of the asymmetric unit. The resulting powder pattern can be directly compared to experimental data in order to obtain reliable starting values for further computations in refinement programs.
PowderCell 2.0 for Windows
(1998)
PowderCell contains a comfortable, user friendly visualization and modification tool for crystal structures. It provides on-line calculation of the corresponding powder diffraction patterns simulating a variety of experimental conditions. The common ICSD and Shelx file formats are supported for importing crystal structure information. It has control of automatic cell transformation and also derivation of subgroups. More than 740 different settings of the 230 space-group types are supported. Up to ten crystal structures can be considered simultaneously. A full pattern refinement enables the direct comparison with experimental diffractograms for quantitative phase analysis, lattice parameter refinement, polynomial background estimation, etc.
PowderCell as teaching tool
(1998)
PowderCell represents a user friendly program which supports the solution of scientific problems as well as teaching and education. Especially for the last one the program offers a lot of information regarding the space-group type as well as crystal structure used. Therefore, on some universities the program is used successfully to make students familiar with x-ray crystallography. The quasi-simultaneous diffraction pattern simulation visualized the changes caused by the respective crystal structure. However, it is also possible to vary different diffraction parameters and investigate the resulting changes in the interference intensity or the reflection position. In principle, the aim of the program is the intuitive generation of structure models. Therefore, special tools have been implemented to move (rotate or shift) or transform the crystal structure.
The formation of AlN films prepared by N+2 ion implantation into aluminium was investigated using X-ray and Auger photoelectron spectroscopy ( XPS, AES) as well as cross-sectional transmission electron microscopy (XTEM). After 100-keV N+2 implantation of low doses (1×1017 cm−2), the formation of hexagonal AlN nanocrystals (crystal size <5 nm, Ncrystal=1017 cm−3) was observed. Their orientation is strongly correlated with the aluminium matrix. With the dose increasing to 3×1017 cm−2, crystal growth follows, finally forming a homogeneous AlN-layer. Furthermore, the diffraction patterns show an increasing amount of misorientation with increasing dose. From the crystal size distribution, we conclude that continuous nucleation takes place. Samples implanted with an energy of 3 keV exhibit analogous behaviour. Nitride growth was further investigated using microstructured AlN formed by 3-keV implantation through movable TEM-masks (structure size: 15–150 mm).
In the case of high N+2 doses (D&5×1017 cm−2), AlN is detected by AES in the shielded area at a distance of up to 10 mm from the exposed region. The Diffusion coefficient was calculated to be 10−10 cm2 s−1. The formation of AlN proceeds in two steps.
After a continuous nucleation, diffusion-assisted Crystal growth takes place until a homogeneous AlN layer results.