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Gyrokinetic simulations of the kinetic electron effects on the electrostatic instabilities on the ITER baseline scenario

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【作者】 张德兵赵鹏飞徐颖峰叶磊张先梅

【Author】 Debing ZHANG;Pengfei ZHAO;Yingfeng XU;Lei YE;Xianmei ZHANG;School of Physics, East China University of Science and Technology;Key Laboratory of Frontier Physics in Controlled Nuclear Fusion and Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences;College of Science, Donghua University;Member of Magnetic Confinement Fusion Research Centre, Ministry of Education;

【通讯作者】 叶磊;张先梅;

【机构】 School of Physics, East China University of Science and TechnologyKey Laboratory of Frontier Physics in Controlled Nuclear Fusion and Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of SciencesCollege of Science, Donghua UniversityMember of Magnetic Confinement Fusion Research Centre, Ministry of Education

【摘要】 The linear and nonlinear simulations are carried out using the gyrokinetic code NLT for the electrostatic instabilities in the core region of a deuterium plasma based on the International Thermonuclear Experimental Reactor(ITER) baseline scenario.The kinetic electron effects on the linear frequency and nonlinear transport are studied by adopting the adiabatic electron model and the fully drift-kinetic electron model in the NLT code,respectively.The linear simulations focus on the dependence of linear frequency on the plasma parameters,such as the ion and electron temperature gradients κLi,e≡R/LTi,e,the density gradient Kn≡R/Ln and the ion-electron temperature ratio τ=Te/Ti.Here,R is the major radius,and Te and Ti denote the electron and ion temperatures,respectively.LA=-(?rlnA)-1 is the gradient scale length,with A denoting the density,the ion and electron temperatures,respectively.In the kinetic electron model,the ion temperature gradient(ITG) instability and the trapped electron mode(TEM) dominate in the small and large kθ region,respectively,where kθ is the poloidal wavenumber.The TEMdominant region becomes wider by increasing(decreasing) κTeTi) or by decreasing Kn.For the nominal parameters of the ITER baseline scenario,the maximum growth rate of dominant ITG instability in the kinetic electron model is about three times larger than that in the adiabatic electron model.The normalized linear frequency depends on the value of τ,rather than the value of Te or Ti,in both the adiabatic and kinetic electron models.The nonlinear simulation results show that the ion heat diffusivity in the kinetic electron model is quite a lot larger than that in the adiabatic electron model,the radial structure is finer and the time oscillation is more rapid.In addition,the magnitude of the fluctuated potential at the saturated stage peaks in the ITGdominated region,and contributions from the TEM(dominating in the higher kθ region) to the nonlinear transport can be neglected.In the adiabatic electron model,the zonal radial electric field is found to be mainly driven by the turbulent energy flux,and the contribution of turbulent poloidal Reynolds stress is quite small due to the toroidal shielding effect.However,in the kinetic electron model,the turbulent energy flux is not strong enough to drive the zonal radial electric field in the nonlinear saturated stage.The kinetic electron effects on the mechanism of the turbulence-driven zonal radial electric field should be further investigated.

【Abstract】 The linear and nonlinear simulations are carried out using the gyrokinetic code NLT for the electrostatic instabilities in the core region of a deuterium plasma based on the International Thermonuclear Experimental Reactor(ITER) baseline scenario.The kinetic electron effects on the linear frequency and nonlinear transport are studied by adopting the adiabatic electron model and the fully drift-kinetic electron model in the NLT code,respectively.The linear simulations focus on the dependence of linear frequency on the plasma parameters,such as the ion and electron temperature gradients κLi,e≡R/LTi,e,the density gradient Kn≡R/Ln and the ion-electron temperature ratio τ=Te/Ti.Here,R is the major radius,and Te and Ti denote the electron and ion temperatures,respectively.LA=-(?rlnA)-1 is the gradient scale length,with A denoting the density,the ion and electron temperatures,respectively.In the kinetic electron model,the ion temperature gradient(ITG) instability and the trapped electron mode(TEM) dominate in the small and large kθ region,respectively,where kθ is the poloidal wavenumber.The TEMdominant region becomes wider by increasing(decreasing) κTeTi) or by decreasing Kn.For the nominal parameters of the ITER baseline scenario,the maximum growth rate of dominant ITG instability in the kinetic electron model is about three times larger than that in the adiabatic electron model.The normalized linear frequency depends on the value of τ,rather than the value of Te or Ti,in both the adiabatic and kinetic electron models.The nonlinear simulation results show that the ion heat diffusivity in the kinetic electron model is quite a lot larger than that in the adiabatic electron model,the radial structure is finer and the time oscillation is more rapid.In addition,the magnitude of the fluctuated potential at the saturated stage peaks in the ITGdominated region,and contributions from the TEM(dominating in the higher kθ region) to the nonlinear transport can be neglected.In the adiabatic electron model,the zonal radial electric field is found to be mainly driven by the turbulent energy flux,and the contribution of turbulent poloidal Reynolds stress is quite small due to the toroidal shielding effect.However,in the kinetic electron model,the turbulent energy flux is not strong enough to drive the zonal radial electric field in the nonlinear saturated stage.The kinetic electron effects on the mechanism of the turbulence-driven zonal radial electric field should be further investigated.

【基金】 supported by the National MCF Energy R&D Program of China (No.2019YFE03060000);National Natural Science Foundation of China (Nos. 12005063, 12375215 and 12175034);the Collaborative Innovation Program of Hefei Science Center,CAS (No. 2022HSC-CIP008)
  • 【文献出处】 Plasma Science and Technology ,等离子体科学和技术(英文版) , 编辑部邮箱 ,2024年09期
  • 【分类号】TL612
  • 【下载频次】3
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