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Heat loads on JET plasma facing components from ICRF and LH wave absorption in the SOL

机译:SOL中ICRF和LH波的吸收会给JET等离子体组件带来热负荷

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摘要

In JET, lower hybrid (LH) and ion cyclotron resonance frequency (ICRF) wave absorption in the scrape-off layer can lead to enhanced heat fluxes on some plasma facing components (PFCs). Experiments have been carried out to characterize these heat loads in order to: (i) prepare JET operation with the Be wall which has a reduced power handling capability as compared with the carbon wall and (ii) better understand the physics driving these wave absorption phenomena and propose solutions for next generation systems to reduce them. When using ICRF, hot spots are observed on the antenna structures and on limiters close to the powered antennas and are explained by acceleration of ions in RF-rectified sheath potentials. High temperatures up to 800 ℃ can be reached on locations where a deposit has built up on tile surfaces. Modelling which takes into account the fast thermal response of surface layers can reproduce well the surface temperature measurements via infrared (IR) imaging, and allow evaluation of the heat fluxes local to active ICRF antennas. The flux scales linearly with the density at the antenna radius and with the antenna voltage. Strap phasing corresponding to wave spectra with lower k values can lead to a significant increase in hot spot intensity in agreement with antenna modelling that predicts, in that case, an increase in RF sheath rectification. LH absorption in front of the antenna through electron Landau damping of the wave with high N components generates hot spots precisely located on PFCs magnetically connected to the launcher. Analysis of the LH hot spot surface temperature from IR measurements allows a quantification of the power flux along the field lines: in the worst case scenario it is in the range 15-30MWm~(-2). The main driving parameter is the LH power density along the horizontal rows of the launcher, the heat fluxes scaling roughly with the square of the LH power density. The local electron density in front of the grill increases with the LH launched power; this also enhances the intensity of the LH hot spots.
机译:在JET中,刮除层中较低的混合(LH)和离子回旋共振频率(ICRF)波吸收会导致某些面向等离子体的组件(PFC)上的热通量增加。为了表征这些热负荷,已经进行了实验,以:(i)使用与碳壁相比降低了功率处理能力的Be壁进行JET操作,以及(ii)更好地理解驱动这些波吸收现象的物理学原理并为下一代系统提出解决方案以减少它们。使用ICRF时,会在天线结构上和靠近有源天线的限制器上观察到热点,并通过RF整流的鞘电势中离子的加速来解释热点。在瓷砖表面堆积沉积物的地方,可以达到800℃的高温。考虑到表面层快速热响应的建模可以很好地重现通过红外(IR)成像进行的表面温度测量,并可以评估有源ICRF天线局部的热通量。通量与天线半径处的密度和天线电压呈线性比例关系。与具有较低k值的波谱相对应的带相位调整可以导致热点强度显着增加,这与天线建模相一致,在这种情况下,天线建模可以预测RF护套整流的增加。通过电子Landau衰减具有高N成分的波,可以在天线前面吸收LH,从而在与发射器磁性连接的PFC上精确定位热点。通过IR测量分析LH热点表面温度可以量化沿磁力线的功率通量:在最坏的情况下,其范围为15-30MWm〜(-2)。主要驱动参数是沿着发射器水平行的LH功率密度,热通量大致与LH功率密度的平方成比例。格栅前面的局部电子密度随LH发射功率的增加而增加。这也增强了LH热点的强度。

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  • 来源
    《Nuclear fusion》 |2011年第10期|p.103018.1-103018.16|共16页
  • 作者单位

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    Max-Planck-Institut fur Plasmaphysik, EURATOM-Assoziation, Garching, Germany;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    Association Euratom-IPPLM, Hery 23, 01-497 Warsaw, Poland;

    Max-Planck-Institut fur Plasmaphysik, EURATOM-Assoziation, Garching, Germany;

    Association EURATOM-Belgian State, ERM-KMS, Brussels, Belgium;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    EURATOM-ENEA sulla Fusione, C.R. Frascati, Roma, Italy;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    Association EURATOM-Belgian State, ERM-KMS, Brussels, Belgium;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    Association EURATOM-Belgian State, ERM-KMS, Brussels, Belgium;

    Association EURATOM-IPP.CR, Za Slovankou 3, 182 21 Praha 8, Czech Republic;

    CEA, IRFM, F-13108 Saint-Paul-Lez-Durance, France;

    EFDA-CSU, Culham Science Centre, Abingdon, 0X14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

    JET-EFDA, Culham Science Centre, OX14 3DB, Abingdon, UK Euratom/CCFE Association, Culham Science Centre, Abingdon, OX 14 3DB, UK;

  • 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);
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  • 正文语种 eng
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