Plasma and Fusion Research
Volume 21, 1303027 (2026)
Letters
- 1)
- Graduate School of Frontier Science, The University of Tokyo, Kashiwa 277-8561, Japan
- 2)
- National Institute for Fusion Science, National Institutes of Natural Sciences, Toki 509-5292, Japan
- 3)
- Graduate School of Engineering, Kyoto University, Nishikyo, Kyoto 615-8530, Japan
Abstract
Microscale turbulence drives not only particle and heat transport but also energy exchange between different particle species. Previous local gyrokinetic studies have shown that turbulent energy exchange can exceed collisional exchange in weakly collisional plasmas, and that ion temperature gradient (ITG) turbulence may hinder ion heating by alpha-heated electrons. In addition, it has been clarified that trapped electron mode (TEM) turbulence transfers energy from electrons to ions, thereby enhancing ion heating. In this work, we extend these studies by examining the impact of turbulent energy exchange on the global temperature profiles at a steady state using the one-dimensional transport solver GOTRESS. For the case of DIII-D discharge #128913, turbulent energy exchange has minimal influence on temperature profiles. However, in the case of enhanced electron heating in a DIII-D-like tokamak plasma, energy transfer from hot electrons to cold ions driven by TEM turbulence becomes comparable to, or even exceeds, the collisional contribution, leading to a significant increase in the ion temperature profile. For ITER Baseline and SPARC standard H-mode scenarios, the turbulent energy exchange is largely compensated by the collisional one, producing only small effects. These results indicate that the impact of turbulent energy exchange on the global temperature profiles in steady-state conditions of future fusion reactor scenarios is expected to be negligibly small, although it can become significant in situations such as plasma start-up phases, where the heating power is strongly unbalanced between electrons and ions.
Keywords
microturbulence, energy exchange, energy flux, temperature profile, tokamak plasmas
Full Text
References
- [1] T. Kato et al., Phys. Plasmas 31, 062510 (2024).
- [2] T. Kato et al., Phys. Plasmas 32, 122303 (2025).
- [3] H. Sugama et al., Phys. Plasmas 3, 2379 (1996).
- [4] H. Sugama et al., Phys. Plasmas 16, 112503 (2009).
- [5] M. Honda, Comput. Phys. Commun. 231, 94 (2018).
- [6] M. Honda and E. Narita, Phys. Plasmas 26, 102307 (2019).
- [7] H. Takenaga et al., Nucl. Fusion 43, 1235 (2003).
- [8] G. Vlad et al., Nucl. Fusion 38, 557 (1998).
- [9] M. Erba et al., Nucl. Fusion 38, 1013 (1998).
- [10] A.E. White et al., Phys. Plasmas 15, 056116 (2008).
- [11] J. Candy, Phys. Plasmas 20, 082503 (2013).
- [12] C. Holland et al., Validation of gyrokinetic transport simulations using DIII-D core turbulence measurements, Proc. 22nd Int. Conf. on Fusion Energy 2008 (Geneva, Switzerland, 2008).
- [13] T. Rafiq et al., Phys. Plasmas 20, 032506 (2013).
- [14] J. Weiland, Collective Modes in Inhomogeneous Plasmas: Kinetic and Advanced Fluid Theory, (CRC Press, 1999).
- [15] A.Y. Pankin et al., Phys. Plasmas 25, 052505 (2018).
- [16] J.E. Kinsey et al., Transport model testing and comparisons using the ITER and DIII-D profile databases, European Physical Society Meeting, (Berchtesgaten, Germany, 1997).
- [17] N.T. Howard et al., Nucl. Fusion 65, 016002 (2024).
- [18] P. Rodriguez-Fernandez et al., J. Plasma Phys. 86, 865860503 (2020).
- [19] M. Hoppe et al., J. Plasma Phys. 88, 905880317 (2022).
![[Plasma and Fusion Research]](/PFR/pfr_header.gif)