Pasupati Nath Khan , Sumit Pahan , A. Sengupta , Tessy Vincent
{"title":"Recovery of radio chemically pure 90Sr suitable for milking clinical grade 90Y from high level liquid waste: A process developmental investigation","authors":"Pasupati Nath Khan , Sumit Pahan , A. Sengupta , Tessy Vincent","doi":"10.1016/j.nxsust.2025.100111","DOIUrl":null,"url":null,"abstract":"<div><div>Radio chemically pure <sup>90</sup>Y is desired for its use as radio therapeutic agent. As a modern practice <sup>90</sup>Y, is milked from its parent <sup>90</sup>Sr, thus the radiochemical purity of resulted <sup>90</sup>Y will be governed by the purity of its parent Sr. High level liquid waste (HLLW) generated from the spent nuclear fuel reprocessing contains ample quantity of <sup>90</sup>Sr, the parent of its β decaying product <sup>90</sup>Y. In our previous studies it was explored that BOC8A/ Nitrooctane can be preferably used to recover <sup>90</sup>Sr in 0.01 M HNO<sub>3</sub> from HLLW with ∼1 % Am (III) & Eu (III) contamination. Thus, <sup>90</sup>Sr recovered needs multi step purification before milking <sup>90</sup>Y. To minimise the number of step in purification to obtain ultrapure <sup>90</sup>Sr (10<sup>−9</sup> Ci alpha / Ci Sr) a well-known hydrophilic supramolecule 18C6 is introduced in the stripping step. A new process scheme has been developed using BOC8A, 18C6 and Tetra-2-ethylhexyl diglycolamide etc. CHON based extractant to obtain highly pure <sup>90</sup>Sr product. The mechanism and effect of different parameters on stripping of Sr with 18C6 have also been investigated in detail. The stripping phenomenon has been found to be spontaneous at 298 K and the change in Gibb’s free energy was found to be - 22.9 kJ mol<sup>−1</sup>K<sup>−1</sup></div></div>","PeriodicalId":100960,"journal":{"name":"Next Sustainability","volume":"6 ","pages":"Article 100111"},"PeriodicalIF":0.0000,"publicationDate":"2025-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Next Sustainability","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2949823625000145","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Radio chemically pure 90Y is desired for its use as radio therapeutic agent. As a modern practice 90Y, is milked from its parent 90Sr, thus the radiochemical purity of resulted 90Y will be governed by the purity of its parent Sr. High level liquid waste (HLLW) generated from the spent nuclear fuel reprocessing contains ample quantity of 90Sr, the parent of its β decaying product 90Y. In our previous studies it was explored that BOC8A/ Nitrooctane can be preferably used to recover 90Sr in 0.01 M HNO3 from HLLW with ∼1 % Am (III) & Eu (III) contamination. Thus, 90Sr recovered needs multi step purification before milking 90Y. To minimise the number of step in purification to obtain ultrapure 90Sr (10−9 Ci alpha / Ci Sr) a well-known hydrophilic supramolecule 18C6 is introduced in the stripping step. A new process scheme has been developed using BOC8A, 18C6 and Tetra-2-ethylhexyl diglycolamide etc. CHON based extractant to obtain highly pure 90Sr product. The mechanism and effect of different parameters on stripping of Sr with 18C6 have also been investigated in detail. The stripping phenomenon has been found to be spontaneous at 298 K and the change in Gibb’s free energy was found to be - 22.9 kJ mol−1K−1
放射化学纯净的90Y用于放射治疗剂。作为一种现代做法,90Y是从其母体90Sr中提取的,因此所得到的90Y的放射化学纯度将由其母体sr的纯度决定。乏核燃料后处理产生的高水平废液(HLLW)含有大量的90Sr,其β衰变产物90Y的母体。在我们之前的研究中,我们探索了BOC8A/硝基辛烷可以很好地用于从HLLW中回收90Sr,回收率为0.01 M HNO3,回收率为1 % Am (III) &;Eu (III)污染。因此,回收的90Sr在挤奶90Y之前需要进行多步净化。为了最大限度地减少纯化步骤,以获得超纯90Sr(10−9 Ci α / Ci Sr),在剥离步骤中引入了一种著名的亲水超分子18C6。以BOC8A、18C6、四-2-乙基己基二甘醇酰胺等为原料,提出了一种新的工艺方案。以CHON为基础的萃取剂,获得高纯度的90Sr产品。研究了不同工艺参数对18C6溶出Sr的机理和影响。在298 K时发现剥离现象是自发的,吉布自由能的变化量为- 22.9 kJ mol−1K−1