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- Beam geometry activation analysis (1)
- Big samples (1)
- CdTe-Modules (1)
- Flux gradients (1)
- Geopolymere (1)
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- Instrumental analysis (1)
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Along with the globally increasing energy demand the application of renewable energy sources is
urgently required. According to national regulations and international treaties (e.g. Kyoto Protocol)
these sources shall be sustainably available at reasonable financial effort and non-polluting during
production, use and waste treatment. Using photovoltaic sources (PV), these requirements can
clearly be met. All industry has to follow the best available technology and an integrative life cycle
approach for their products and production. PV thin film technology strictly responds to this obligation.
In order to save material resources and to minimise undesirable landfill recycling of spent PV
modules is necessary. Recycling of multi-component materials containing mixed metals typically
consists of three parts: liberation, separation, and recovery. In our study (RESOLVED an EU
Demonstration Project) the focus is on liberation and separation. The converting layer (CdTe) was
liberated (removed) from the glass carrier by sandblasting and separated subsequently from the
blast material (e.g. corundum) and other components using stepwise different separation techniques.
Both the glass substrate and CdTe are subject to re-use. The overall feasibility of the recycling
process is primarily governed by the efficiency of the procedure applied to the separation of CdTe
from the rest (blasting material, glass residues, etc.). This was performed by water-based flotation.
Several flotation procedures were studied regarding their separation yields. The distribution of
CdTe in the phases involved (flotate, water, residue) was measured using energy dispersive X-ray
fluorescence spectrometry (EDXRS) intended for future routine application and by instrumental
large-volume photon activation analysis (IPAA) as a reference procedure. The results of both analytical
methods were in satisfactory agreement.
We have developed a very fast and entirely gas-phase based purification technique for carbon nanotubes (CNT) that allows removing metal and metal oxide impurities with high effectiveness. CNT agglomerates from chemical vapor deposition (CVD) synthesis which contained carbon encapsulated catalysts were injected into an atmospheric plasma torch. Very high heating rates allow for quasi-instantaneous vaporization of catalyst particles. This way, metal vapors are hyposized to break mechanically instable encapsulations and effuse from incomplete ones faster than thermally induced graphitization stabilizes such particle encapsulations. The ash content of multi-walled (MW) CNT samples was reduced to less than 15% of the initial value within a few milliseconds. Also the metal content of single-walled (SW) CNT agglomerates was significantly reduced. Repeated injection of CNT agglomerates into the plasma torch resulted in higher-purity products of improved structural integrity and increased oxidation resistance.
In activation analysis of traces in small samples, the non-equivalence of the activating radiation doses of sample and calibration material gives rise to sometimes tolerable systematic errors. Conversely, analysis of major components usually demands high trueness and precision. To meet this, beam geometry activation analysis (BEAMGAA) procedures have been developed for instrumental photon (IPAA) and neutron activation analysis (INAA) in which the activating neutron/photon beam exhibits broad, flat-topped characteristics. This results in a very low lateral activating flux gradient compared to known radiation facilities, however, at significantly lower flux density. The axial flux gradient can be accounted for by a monitor-sample-monitor assembly. As a first approach, major components were determined in high purity substances as well as selenium in a cattle fodder additive.
C, N, O, F and P can be analyzed by instrumental photon activation analysis (IPAA) including decay curve analysis. The interference of 30P (T1/2 = 149.9 s) by 15O (T1/2 = 122.2 s) can be ruled out by direct positron measurement making use of the largely different maximum β+-energies of both nuclides (3.24 MeV and 1.73 MeV, respectively). Interference by carbon (11C) can be avoided by sub-threshold activation with 17 MeV bremsstrahlung. The short half-life of 30P allows a high productivity of the method. Reliability was demonstrated in the range of 0.2%2% P (detection limit = 40 µg/g). Analysis of a certified reference material (BCR-CRM 063) yielded excellent agreement with the certified data.