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Scaling of H-mode edge pedestal pressure for a Type-I ELM regime in tokamaks

机译:托卡马克中I型ELM方案的H模式边缘基座压力缩放

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Scaling of H-mode edge pedestal pressure for a Type-I ELM regime based on a simple analytical formula (Hatae T et al 2001 Nucl. Fusion 41 285) can be significantly improved by introducing shaping factors into the scaling, which is motivated by a recent development of the MHD model for the critical pressure gradient (Snyder P B et al 2002 Phys. Plasmas 5 2037, Lao L L et al 2002 ITPA H-mode Edge Pedestal Physics Topical Group Meeting (San Diego)). The physics basis of these shaping factors is an enhancement of the critical pressure gradient determined by a high toroidal mode number, n, ideal ballooning mode through the effect of the magnetic well. On an increase in the magnetic well, peeling and ballooning modes decouple and the critical gradient is determined by the intermediate n mode, which enhances the critical gradient substantially. The improved scaling can reproduce the pedestal pressure reasonably well for ASDEX-U, JET and JT-60U Type-I ELMy data archived in the International Pedestal Database version 3. [References: 26]
机译:基于简单分析公式(Hatae T等人,2001 Nucl。Fusion 41 285)的I型ELM方案的H模式边缘基座压力的缩放可通过将缩放因子引入缩放来显着改善。临界压力梯度的MHD模型的最新发展(Snyder PB等人,2002 Phys.Plasmas 5 2037,Lao LL等人,2002 ITPA H模式边缘基座物理专题小组会议(圣地亚哥))。这些成形因子的物理基础是通过磁阱的作用来提高临界压力梯度,该临界压力梯度是由高环形模数n(理想的膨胀模式)确定的。随着磁阱的增加,剥离模式和膨胀模式解耦,并且临界梯度由中间n模式确定,这大大提高了临界梯度。改进的缩放比例可以很好地重现国际基座数据库版本3中存储的ASDEX-U,JET和JT-60U I型ELMy数据的基座压力。[参考:26]

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