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- Analysis (1)
- Beam geometry activation analysis (1)
- Big samples (1)
- Electronic scrap (1)
- Flux gradients (1)
- Instrumental analysis (1)
- Measurement regime (1)
- Phosphorus (1)
- Photon activation (1)
- Process control (1)
Large-volume instrumental photon and neutron activation analysis (IPAA resp. INAA) was used for
investigation of shredded electronic waste material. Sample masses from 1 to 150 grams were analysed
to obtain an estimate of the minimum sample size to be taken to achieve a representativeness
of the results which is satisfactory for a defined investigation task. Furthermore, the influence of
irradiation and measurement parameters upon the quality of the analytical results were studied. Finally,
the analytical data obtained from IPAA and instrumental neutron activation analysis (INAA),
both carried out in a large-volume mode, were compared. Values within the limits of satisfactory
agreement were found only partially. Analytical process control using on-site X-ray fluorescence
analysis performed during recycling of electronic waste is currently under development.
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.