Plasma and Fusion Research

Volume 17, 1402037 (2022)

Regular Articles


A Fast Electron Transport Model for Lower Hybrid Wave Sustained Plasmas
Akira EJIRI, Hibiki YAMAZAKI, Yuichi TAKASE, Naoto TSUJII, Osamu WATANABE, Yi PENG, Kotaro IWASAKI, Yuki AOI, Yongtae KO, Kyohei MATSUZAKI, James H.P. RICE, Yuki OSAWA, Charles P. MOELLER1), Yasuo YOSHIMURA2), Hiroshi KASAHARA2), Kenji SAITO2), Tetsuo SEKI2) and Shuji KAMIO2)
The University of Tokyo, Kashiwa 277-8561, Japan
1)
General Atomics, San Diego, CA 92186, U.S.A.
2)
National Institute for Fusion Science, Toki 509-5292, Japan
(Received 20 October 2021 / Accepted 10 March 2022 / Published 13 May 2022)

Abstract

In the TST-2 spherical tokamak (ST), non-inductive start-up by lower-hybrid waves (200 MHz) has been studied and a plasma current of 27 kA was achieved. For a comprehensive understanding of the wave sustained plasmas, a fast electron transport model combined with an X-ray emission model is constructed. The electrons in the model show a velocity random walk induced by the wave and collisional slowing down. Simultaneously, they show diffusion in real space. Electron generation and loss at the limiters are also considered. Using the model we can calculate the powers, such as the power from the wave to electrons (i.e., deposition power), collisional bulk electron heating power, power to the limiters. In addition, plasma current, electron density, neutral density, X-ray spectrum expected by a certain measurement system are obtained. Comparison with experimental data shows that a major part of the LHW deposition power is lost by fast electrons hitting the outboard limiter, while a minor part is used to heat cold bulk electrons. The diffusion in real space is well described by the RF induced radial transport, which is often used to interpret fast ion diffusion in ICRF heating. The present work suggests that the RF induced transport of fast electrons is the dominant loss mechanism.


Keywords

rf induced transport, lower hybrid wave, spherical tokamak, fast electron

DOI: 10.1585/pfr.17.1402037


References

  • [1] Y. Takase et al., Nucl. Fusion 41, 1543 (2001).
  • [2] Y. Takase et al., Nucl. Fusion 51, 063017 (2011).
  • [3] Y. Takase et al., Nucl. Fusion 53, 063006 (2013).
  • [4] T. Wakatsuki et al., Nucl. Fusion 54, 093014 (2014).
  • [5] T. Shinya et al., Nucl. Fusion 55, 073003 (2015).
  • [6] T. Shinya et al., Nucl. Fusion 57, 036006 (2017).
  • [7] S. Yajima et al., Plasma Fusion Res. 13, 3402114 (2018).
  • [8] N. Tsujii et al., Nucl. Fusion 57, 126032 (2017).
  • [9] A. Ejiri et al., 27th Int. Conf. Fusion Energy 2018 IAEA-CN-258 (Proc. 27th Int. Conf. Fusion Energy 2018, Gandhinagar (Ahmedabad) Gujarat, India, 2018) IAEA, Vienna (2018).
  • [10] L. Chen et al., Nucl. Fusion 28, 389 (1988).
  • [11] S. Yajima et al., Nucl. Fusion 59, 066004 (2019).
  • [12] M. Honda, Jpn. J. Appl. Phys. 52, 108002 (2013).
  • [13] A. Hayashi, internal report Inst. Plasma Phys. (IPPJ. AM-19) Nagoya Univ., Japan (1981).
  • [14] Y.K. Kim et al., it NIST: Electron-Impact Cross Section Database - Intro https://physics.nist.gov/PhysRefData/Ionization/intro.html
  • [15] H. Togashi et al., Plasma Fusion Res. 10, 1202082 (2015).
  • [16] N. Tsujii et al., Plasma Fusion Res. 15, 2402010 (2020).
  • [17] D.M. Tucker et al., Medical Physics 18, 211 (1991).
  • [18] Atomic form factors, http://lampx.tugraz.at/~hadley/ss1/crystaldiffraction/atomicformfactors/formfactors.php
  • [19] S.M. Kaye et al., Nucl. Fusion 37, 16657 (1997).
  • [20] S. Tsuda et al., Plasma Fusion Res. 10, 1202064 (2015).
  • [21] T. Yoshinaga et al., J. Plasma Fusion Res. 81, 333 (2005).
  • [22] J. Wesson Tokamaks 4th ed. (Oxford Univ. Press, 2011).