Matches in SemOpenAlex for { <https://semopenalex.org/work/W4386697072> ?p ?o ?g. }
- W4386697072 endingPage "1354350" @default.
- W4386697072 startingPage "1354350" @default.
- W4386697072 abstract "As an indispensable component of X-ray free electron lasers and future ring electron-positron colliders, a 1.3GHz 9-cell superconducting cavity provides higher acceleration voltage and higher RF power per unit length, and saves equipment space. During testing and operation, superconducting cavities often need to be cooled gradually from the ambient temperature (300K) to the superconducting temperature (4.5K or less). To avoid plastic deformation of materials and seal leaking caused by high thermal stress, the cooling rates in each stage and the temperature differences on the cavity must be properly controlled. Currently, a less effective manual control strategy is typically used, whose main limitations include a low level of automation, a high reliance on the experience of the operating personnel, and a fairly lengthy time due to low efficiency. In this paper, a 1.3GHz 9-cell superconducting cavity and its helium vessel were taken as the research subjects, six different mechanical structures of the helium vessel were designed, and six different three-dimensional thermal-flow coupling models were established. For each structural model, the temperature distribution and cooling strategy were analyzed using fluid numerical simulation software. The influence of inlet parameters on the cooling process was analyzed, and the appropriate mechanical structure model was recommended. The results showed that: During the cooling process, the closer the superconducting cavity is to the inlet, the lower the temperature is. The cooling rate is faster in the early stage in which the temperature difference can be reduced by 50% within the first 30 minutes. After experimental test verification, the total cooling time is about 650 min (10.8h or so), and the deviation between the simulation results and the experimental test results is less than 7%, which shows the simulation results can well predict the actual cooling process for 1.3GHz 9-cell superconducting cavity. The research work in this paper can lay a good foundation for the further R&D status of the superconducting cavity." @default.
- W4386697072 created "2023-09-14" @default.
- W4386697072 creator A5009002450 @default.
- W4386697072 creator A5009927645 @default.
- W4386697072 creator A5013520118 @default.
- W4386697072 creator A5027398228 @default.
- W4386697072 creator A5030306177 @default.
- W4386697072 creator A5038837596 @default.
- W4386697072 creator A5041284997 @default.
- W4386697072 creator A5044931969 @default.
- W4386697072 creator A5046329976 @default.
- W4386697072 creator A5061663049 @default.
- W4386697072 creator A5063235838 @default.
- W4386697072 creator A5067741005 @default.
- W4386697072 creator A5072836468 @default.
- W4386697072 date "2023-10-01" @default.
- W4386697072 modified "2023-10-06" @default.
- W4386697072 title "Comprehensive Dynamic Numerical Simulation of Cooling Process for a 1.3GHz 9-cell Superconducting Cavity Based on Different Structures" @default.
- W4386697072 cites W1480161190 @default.
- W4386697072 cites W1660556003 @default.
- W4386697072 cites W1890903183 @default.
- W4386697072 cites W1990519364 @default.
- W4386697072 cites W2029365170 @default.
- W4386697072 cites W2103906961 @default.
- W4386697072 cites W2340995374 @default.
- W4386697072 cites W2965812631 @default.
- W4386697072 cites W3103210248 @default.
- W4386697072 cites W3116066814 @default.
- W4386697072 cites W3117895760 @default.
- W4386697072 cites W3185077247 @default.
- W4386697072 doi "https://doi.org/10.1016/j.physc.2023.1354350" @default.
- W4386697072 hasPublicationYear "2023" @default.
- W4386697072 type Work @default.
- W4386697072 citedByCount "0" @default.
- W4386697072 crossrefType "journal-article" @default.
- W4386697072 hasAuthorship W4386697072A5009002450 @default.
- W4386697072 hasAuthorship W4386697072A5009927645 @default.
- W4386697072 hasAuthorship W4386697072A5013520118 @default.
- W4386697072 hasAuthorship W4386697072A5027398228 @default.
- W4386697072 hasAuthorship W4386697072A5030306177 @default.
- W4386697072 hasAuthorship W4386697072A5038837596 @default.
- W4386697072 hasAuthorship W4386697072A5041284997 @default.
- W4386697072 hasAuthorship W4386697072A5044931969 @default.
- W4386697072 hasAuthorship W4386697072A5046329976 @default.
- W4386697072 hasAuthorship W4386697072A5061663049 @default.
- W4386697072 hasAuthorship W4386697072A5063235838 @default.
- W4386697072 hasAuthorship W4386697072A5067741005 @default.
- W4386697072 hasAuthorship W4386697072A5072836468 @default.
- W4386697072 hasBestOaLocation W43866970721 @default.
- W4386697072 hasConcept C116915560 @default.
- W4386697072 hasConcept C117896860 @default.
- W4386697072 hasConcept C120665830 @default.
- W4386697072 hasConcept C121332964 @default.
- W4386697072 hasConcept C127413603 @default.
- W4386697072 hasConcept C131584629 @default.
- W4386697072 hasConcept C137727706 @default.
- W4386697072 hasConcept C159985019 @default.
- W4386697072 hasConcept C168834538 @default.
- W4386697072 hasConcept C184779094 @default.
- W4386697072 hasConcept C189166818 @default.
- W4386697072 hasConcept C192562407 @default.
- W4386697072 hasConcept C201289731 @default.
- W4386697072 hasConcept C204366326 @default.
- W4386697072 hasConcept C204530211 @default.
- W4386697072 hasConcept C26873012 @default.
- W4386697072 hasConcept C536315585 @default.
- W4386697072 hasConcept C54101563 @default.
- W4386697072 hasConcept C546029482 @default.
- W4386697072 hasConcept C57879066 @default.
- W4386697072 hasConcept C74650414 @default.
- W4386697072 hasConcept C7694927 @default.
- W4386697072 hasConcept C78519656 @default.
- W4386697072 hasConcept C97355855 @default.
- W4386697072 hasConceptScore W4386697072C116915560 @default.
- W4386697072 hasConceptScore W4386697072C117896860 @default.
- W4386697072 hasConceptScore W4386697072C120665830 @default.
- W4386697072 hasConceptScore W4386697072C121332964 @default.
- W4386697072 hasConceptScore W4386697072C127413603 @default.
- W4386697072 hasConceptScore W4386697072C131584629 @default.
- W4386697072 hasConceptScore W4386697072C137727706 @default.
- W4386697072 hasConceptScore W4386697072C159985019 @default.
- W4386697072 hasConceptScore W4386697072C168834538 @default.
- W4386697072 hasConceptScore W4386697072C184779094 @default.
- W4386697072 hasConceptScore W4386697072C189166818 @default.
- W4386697072 hasConceptScore W4386697072C192562407 @default.
- W4386697072 hasConceptScore W4386697072C201289731 @default.
- W4386697072 hasConceptScore W4386697072C204366326 @default.
- W4386697072 hasConceptScore W4386697072C204530211 @default.
- W4386697072 hasConceptScore W4386697072C26873012 @default.
- W4386697072 hasConceptScore W4386697072C536315585 @default.
- W4386697072 hasConceptScore W4386697072C54101563 @default.
- W4386697072 hasConceptScore W4386697072C546029482 @default.
- W4386697072 hasConceptScore W4386697072C57879066 @default.
- W4386697072 hasConceptScore W4386697072C74650414 @default.
- W4386697072 hasConceptScore W4386697072C7694927 @default.
- W4386697072 hasConceptScore W4386697072C78519656 @default.
- W4386697072 hasConceptScore W4386697072C97355855 @default.
- W4386697072 hasFunder F4320335641 @default.