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COREDIV numerical simulation of high neutron rate JET-ILW DD pulses in view of extension to JET-ILW DT experiments

机译:高中比率JET-ILW DD脉冲的COREDIV数值模拟,延伸到JET-ILW DT实验

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摘要

Two high performance JET-ILW pulses, pertaining to the 2016 experimental campaign, have been numerically simulated with the self-consistent code COREDIV with the aim of predicting the ELM-averaged power load to the target when extrapolated to DT plasmas. The input power of about 33 MW as well as the total radiated power and the average density are similar in the two pulses, but for one of them the density is provided by combined low gas puff and pellet injection, characterized by low SOL density, for the other one by gas fuelling only, at higher SOT. density. Considering the magnetic configuration of theses pulses and the presence of a significant amount of Ni (not included in the version of the code used for these simulations), a number of assumptions are made in order to reproduce numerically the main core and SOL experimental data. The extrapolation to DT plasmas at the original input power of 33 MW, and taking into account only the thermal component of the alpha-power, does not show any significant difference regarding the power to the target with respect to the DD case. In contrast, the simulations at auxiliary power 40 MW, both at the original I-p = 3 MA and at I-p = 4 MA, show that the power to the target for both pulses is possibly too high to be sustained for about 5 s by strike-point sweeping alone without any control by Ne seeding. Even though the target power load may decrease to about 13-15 MW with substantial Ne seeding for both pulses, as from numerical predictions, there are indications suggesting that the control of the power load may be more critical for the pulse with pellet injection, due to the reduced SOL radiation.
机译:两种高性能的喷射器ILW脉冲有关2016年的实验活动,通过自我支撑的守则COREDIV进行了数值模拟,目的是当推断到DT等离子体时预测到目标的ELM平均功率负荷。两种脉冲中约33mW以及总辐射功率的输入功率和平均密度在两个脉冲中相似,但是对于其中之一的密度通过组合的低气体粉扑和颗粒注入提供,其特征在于低溶胶密度,适用于另一个通过气体加油,在较高的SOT处。密度。考虑到这些脉冲的磁构造和大量Ni的存在(不包括在用于这些模拟的代码的版本中),因此进行了许多假设,以便在数值上再现主核和溶胶实验数据。在基于33mW的原始输入功率下的推断到DT等离子体,并且仅考虑了α功率的热分量,并不显示关于靶相对于DD案例的功率的任何显着差异。相比之下,在原始IP = 3 mA和IP = 4 mA处的辅助功率40mW的模拟显示,在IP = 4 mA处,两种脉冲的目标可能太高而无法通过撞击持续约5秒点单独扫地,没有任何通过NE播种控制。尽管目标功率负载可能会减小到大约13-15兆瓦,但对于两个脉冲的大量播种,由于数值预测,存在指示,表明电力负载的控制可能对颗粒喷射的脉冲更为关键,因此减少溶胶辐射。

著录项

  • 来源
    《Nuclear fusion》 |2019年第5期|056026.1-056026.10|共10页
  • 作者单位

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Inst Plasma Phys & Laser Microfus Warsaw Poland;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Inst Plasma Phys & Laser Microfus Warsaw Poland;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Inst Plasma Phys & Laser Microfus Warsaw Poland;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Foschungszentrum Juelich GmbH Inst Energie & Klimaforsch Plasmaphys Julich Germany;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Univ Lisbon Inst Plasmas & Fusao Nucl Inst Super Tecn Lisbon Portugal;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Inst Plasma Phys & Laser Microfus Warsaw Poland;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Culham Sci Ctr Culham Ctr Fus Energy Culham England;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Foschungszentrum Juelich GmbH Inst Energie & Klimaforsch Plasmaphys Julich Germany;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|TEC Partner Assoc EUROFUS Belgian State LPP ERM KMS Brussels Belgium;

    Culham Sci Ctr EUROfus Consortium JET Abingdon OX14 3DB Oxon England|Foschungszentrum Juelich GmbH Inst Energie & Klimaforsch Plasmaphys Julich Germany;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    tokamak; integrated modeling; neon seeding; JET-ILW;

    机译:Tokamak;综合建模;霓虹播种;Jet-ILW;

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