To initiate a fusion reaction, deuterium and tritium must be heated to over 100 million degrees Celsius to form plasma, which is then maintained by a strong magnetic "cage". However, when turbulence is excited in the plasma, the plasma flows out of the magnetic "cage". Therefore, turbulence is an important topic in fusion research, and its suppression is essential to the realization of a fusion power plant. For turbulence suppression, an understanding of the physical mechanism of turbulence excitation is essential, and LHD is the perfect device to tackle this challenge. For example, generally turbulence measurement is not easy, but we have successfully measured not only its amplitude but also its spatial profile and propagation direction using precision laser diagnostics.
A research group led by Assistant Professor Toshiki Kinoshita (Research Institute for Applied Mechanics, Kyushu University), Professor Kenji Tanaka (National Institute for Fusion Science, National Institutes on Natural Sciences) and Professor Akihiro Ishizawa (Graduate School of Energy Science, Kyoto University) et al. performed experiments in which the density (amount of electrons and ions) of the hydrogen plasma was changed under identical heating conditions to gain a comprehensive understanding of turbulence in LHD. At the same time, the turbulence was measured in detail.
As a result, it was found that turbulence is most suppressed at a certain density (transition density), and below the transition density, it decreases with increasing density (purple region in Figure 2), but above the transition density, it begins to increase (orange region in Figure 2). Furthermore, it was observed that the turbulence propagation direction reverses after the transition density. This result implies that the turbulence nature changes around the transition density (turbulence transition).
Then, to corroborate the turbulence transition, simulations were performed on the Raijin supercomputer. As a result, we found that the turbulence observed below the transition density was mainly caused by the ion-temperature gradient, while that above it was mainly caused by the pressure gradient and plasma resistivity. Moreover, we identified that this change in the turbulence is an important physical mechanism of turbulence suppression. Thus, by making full use of experiments and simulations, we revealed that the observed turbulence suppression was due to a change in the turbulence mode, i.e., turbulence transition.
In addition, experiments under the same conditions were conducted in deuterium plasmas and compared with hydrogen plasmas. As a result, we found that turbulence transitions occur at higher density for the deuterium plasma, i.e., turbulence is suppressed at higher density (Figure 3). Furthermore, surprisingly, the turbulence observed above the transition density is clearly suppressed in deuterium plasmas. The turbulence suppression observed at high density in deuterium plasmas implies that it will be further suppressed in the higher-density and heavier-mass deuterium/tritium mixture plasmas envisioned for fusion power generation. This is a favorable result for early realization of fusion power generation.
This study shows that turbulence is most suppressed during the turbulence transition and the turbulence transition density is higher in deuterium plasmas than in hydrogen plasmas. The different transition densities mean that turbulence transition condition is not determined solely by electron density. The next step is to identify the turbulence transition condition based on the physical background of turbulence, and to develop innovative operation scenarios with low-turbulence conditions for fusion power plants. We would also like to extend our research into an extrapolation to deuterium/tritium mixed plasmas and their application to plant design in order to find efficient solutions for realizing fusion energy.
Research Report:Turbulence transition in magnetically confined hydrogen and deuterium plasmas
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Advanced Fusion Research Center
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