| Literature DB >> 35480374 |
Bart Verlinden1,2,3, Karen Van Hecke1, Andreas Wilden4, Michelle Hupert5, Beatrix Santiago-Schübel5, Richard J M Egberink6, Willem Verboom6, Piotr M Kowalski3,7, Giuseppe Modolo4, Marc Verwerft1, Koen Binnemans2, Thomas Cardinaels1,2.
Abstract
Reprocessing of spent nuclear fuel aims at improving resource efficiency and reducing its radiotoxicity and heat production in the long term. The necessary separation of certain metal ions from the spent fuel solutions can be achieved using different solvent extraction processes. For the scenario of the EURO-GANEX process, the use of the new, modified diglycolamide 2,2'-oxybis(N,N-didecylpropanamide) (mTDDGA) was recently proposed to simplify the current solvent composition and reduce extraction of fission products. Before further developing the process based on this new ligand, its stability under ionizing radiation conditions needs to be studied. For this reason, gamma irradiation experiments were conducted followed by analyses with high performance liquid chromatography coupled to a mass spectrometer (HPLC-MS). The determined degradation rate of mTDDGA was found to be lower than that of the reference molecule N,N,N',N'-tetra-n-octyl-diglycolamide (TODGA). Many identified degradation compounds of both molecules are analogues showing the same bond breaking, although also unreported de-methylation, double/triple de-alkylation and n-dodecane addition products were observed. This journal is © The Royal Society of Chemistry.Entities:
Year: 2022 PMID: 35480374 PMCID: PMC9036757 DOI: 10.1039/d1ra08761d
Source DB: PubMed Journal: RSC Adv ISSN: 2046-2069 Impact factor: 3.361
Fig. 1Chemical structures of (R,S) and (S,S)-mTDDGA.
Fig. 2TODGA and mTDDGA concentrations as a function of the absorbed dose and presence of an HNO3 aqueous phase during irradiation. The data for TODGA was taken from Verlinden et al.[1] The initial concentration was 0.05 mol L−1 for both ligands. Error bars represent the standard deviation of three analysis runs. The Y-axis is scaled with the natural logarithm.
Determined dose constants, resulting from the linear least square regression of the natural logarithm of the measured concentrations as a function of the absorbed dose. Dose constants for TODGA were based on data from Verlinden et al.[1] The intersection with the y axis for the linear fitting was set at the initial concentration, prepared by accurate weighing
| Sample |
|
|---|---|
| 0.05 mol L−1 TODGA | −3.7 ± 0.2 |
| 0.05 mol L−1 TODGA in contact with 2.5 mol L−1 HNO3 | −3.4 ± 0.1 |
| 0.05 mol L−1 mTDDGA | −2.9 ± 0.1 |
| 0.05 mol L−1 mTDDGA in contact with 2.5 mol L−1 HNO3 | −2.8 ± 0.3 |
Fig. 3Scheme with degradation compounds of mTDDGA, with the peak area of their corresponding [M + H]+ species as a function of the absorbed dose for the irradiation in contact with 2.5 mol L−1 HNO3 (solid, orange) and the neat organic phase (dotted, blue). Chemical structures show the degradation compounds [M], while the m/z ratio corresponds to the protonated [M + H]+ species.
Fig. 4Degradation compounds of mTDDGA, with the peak area of their corresponding [M + H]+ species as a function of the absorbed dose for the irradiation in contact with 2.5 mol L−1 HNO3 (solid, orange) and the neat organic phase (dotted, blue). Chemical structures show the degradation compounds [M], while the m/z ratio corresponds to the protonated [M + H]+ species.
Retention time (RT) of the chromatographic peaks. If there are two separated peaks for both diastereomers, two retention times are shown
|
| RT 1 (min.) | RT 2 (min.) | |
|---|---|---|---|
| DC I | 581.56 | 7.82 | 8.34 |
| DC II | 354.37 | 4.07 | |
| DC III | 370.37 | 3.25 | |
| DC IV | 398.4 | 4.17 | |
| DC V | 326.34 | 3.30 | |
| DC VI | 426.39 | 3.51 | 3.89 |
| DC VII | 442.39 | 3.06 | 3.22 |
| DC VIII | 441.41 | 2.66 | |
| DC IX | 301.25 | 1.54 | |
| DC X | 456.4 | 3.66 | 3.84 |
| DC XI | 298.35 | 1.27 | |
| DC XII | 230.21 | 1.54 | |
| DC XIII | 200.20 | 1.69 | |
| DC XIV | 214.22 | 1.59 | |
| DC XV | 340.36 | 2.67 | |
| DC XVI | 520.55 | 11.13 | |
| DC XVII | 522.56 | 11.89 | |
| DC XVIII | 538.56 | 10.80 | |
| DC XIX | 610.58 | 10.51 | |
| DC XX | 524.54 | 11.72 | |
| DC XXI | 696.69 | 12.73 | |
| DC XXII | 707.70 | 13.34 | |
| mTDDGA | 721.72 | 13.87 |
Fig. 5Combined ion chromatograms of the most intense signals in irradiated mTDDGA samples with an initial concentration of 0.05 mol L−1 mTDDGA irradiated with or without contact to an aqueous phase of 2.5 mol L−1 HNO3.
Fig. 6Visualization of the values of the radical Fukui functions on the isodensity surface of mTDDGA (in e a.u.−3), increasing from blue to green and red. Following colors are used for the representation of the atoms: white: hydrogen, red: oxygen, blue: nitrogen, cyan: carbon. The high isodensity (reddish colors) indicates parts of the molecule prone to the radical attack.