Pub Date : 2025-01-06DOI: 10.1109/TASC.2025.3525839
{"title":"2024 Index IEEE Transactions on Applied Superconductivity Vol. 34","authors":"","doi":"10.1109/TASC.2025.3525839","DOIUrl":"https://doi.org/10.1109/TASC.2025.3525839","url":null,"abstract":"","PeriodicalId":13104,"journal":{"name":"IEEE Transactions on Applied Superconductivity","volume":"34 9","pages":"1-251"},"PeriodicalIF":1.7,"publicationDate":"2025-01-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10827842","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142938019","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-31DOI: 10.1109/TASC.2024.3520265
{"title":"IEEE Transactions on Applied Superconductivity Information for Authors","authors":"","doi":"10.1109/TASC.2024.3520265","DOIUrl":"https://doi.org/10.1109/TASC.2024.3520265","url":null,"abstract":"","PeriodicalId":13104,"journal":{"name":"IEEE Transactions on Applied Superconductivity","volume":"35 1","pages":"C4-C4"},"PeriodicalIF":1.7,"publicationDate":"2024-12-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10819278","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142905941","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-30DOI: 10.1109/TASC.2024.3523873
Shahriar Bakrani Balani;H. Milanchian;T. Salmi
Quench is an irreversible transition where the magnet locally loses its superconducting properties and becomes resistive. Early quench detection and a prompt protection system response are essential to avoid conductor damage. One of the conventional methods for accelerator magnet quench protection is to place resistive heaters on the surface of the coils. The protection heaters are stainless steel strips which are powered with a voltage pulse from capacitor bank discharge. Current is passing through the heaters, generating heat due to the resistivity of the stainless steel. Heat is transferred to the cable by conduction. There is at least one layer of polyimide film and the cable insulation (impregnated glass fiber) between the heater and the superconducting cable. Heater delay is defined as the required time to reach the current sharing temperature in the cable after heater firing. Typically predicting the heater delay requires numerical simulations which are computationally somewhat challenging and require expertise and need of specific software. In this study, we are providing a fast and easily accessible surrogate model for predicting the heater delay in Nb 3