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Dive into the research topics where S. Kawasaki is active.

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Featured researches published by S. Kawasaki.


Nuclear Fusion | 2004

Global particle balance and wall recycling properties of long duration discharges on TRIAM-1M

M. Sakamoto; M. Yuno; S.-I. Itoh; K. Hanada; K. Nakamura; H. Zushi; E. Jotaki; M. Hasegawa; S.V. Kulkarni; Atsuhiro Iyomasa; S. Kawasaki; Hiroshi Nakashima

The longest tokamak discharge, with a duration of 11 406 s (3 h 10 min), has been achieved. The global particle balance has been investigated. In the longest discharge, the global balance between the particle absorption and release of the wall was achieved at t ~ 30 min. After that, the plasma density was maintained by the recycling flux alone until the end of the discharge. The maximum wall inventory is about 3.6 × 1020 H at t ~ 30 min, but it is finally released from the wall at the end of the discharge. The hydrogen release seems to be caused by the temperature increase in the whole toroidal area of the main chamber. Moreover, it has been observed that there is a large difference between the properties of wall recycling in the continuous gas feed case (i.e. static condition) and in the additional gas puff case (i.e. dynamic condition). In the static condition, the effective particle confinement time increases to ~10 s during the 1 min discharge and it increases to ~100 s before the global balance in the longest discharge. In the dynamic condition, the decay time of the electron density just after the gas puff, i.e. the effective particle confinement time, is constant at 0.2–0.3 s during the discharge. The large difference in the effective particle confinement time between the static and dynamic conditions seems to be caused by the reduction in the recycling coefficient due to the enhanced wall pumping resulting from the additional gas puff.


Nuclear Fusion | 2014

Role of energetic electrons during current ramp-up and production of high poloidal beta plasma in non-inductive current drive on QUEST

S. Tashima; H. Zushi; M. Isobe; K. Hanada; H. Idei; K. Nakamura; A. Fujisawa; K. Matsuoka; M. Hasegawa; Y. Nagashima; S. Okamura; Santanu Banerjee; S. Kawasaki; Hiroshi Nakashima; A. Higashijima

A scenario for non-inductive current ramp-up has been demonstrated using electron cyclotron waves in the spherical tokamak QUEST. The configuration was characterized by a high toroidal magnetic mirror ratio of 2 and a steady vertical magnetic field of more than 10% of the toroidal magnetic field. The generation and confinement of energetic electrons having energy greater than 10?keV were studied using hard x-rays. Because of the energetic electron pressure, a natural divertor formed with an inboard poloidal field null at the high poloidal beta (approximately 3?4).


Plasma Science & Technology | 2011

Non-Inductive Start up of QUEST Plasma by RF Power

K. Hanada; H. Zushi; H. Idei; Kazuo Nakamura; M. Ishiguro; S. Tashima; E. Kalinnikova; M. Sakamoto; M. Hasegawa; A. Fujisawa; A. Higashijima; S. Kawasaki; Hiroshi Nakashima; Haiqing Liu; Osamu Mitarai; T. Maekawa; A. Fukuyama; Y. Takase; J. Qian

Both start-up and sustainment of plasma were successfully achieved by fully non-inductive current drive using microwave with a frequency of 8.2 GHz. Plasmas current of 15 kA was implemented for 1 s. Magnetic surface reconstruction exhibited a plasma shape with an aspect ratio of below 1.5. The plasma current was dependent significantly on the launched microwave power and vertical magnetic field, while not affected by the mode of launched wave and the toroidal refractive index. Hard X-ray (HXR) emitted from energetic electrons accelerated by the microwave was observed, and the discharge with a plasma current over 4 kA followed the same trend as the number of photons of 10 keV to 12 keV. This suggests that the plasma current may be driven by energetic electrons. Based on the experimental conditions, alternative explanations of how the plasma current could be driven are discussed.


Nuclear Fusion | 2007

A study on temperature effects on hydrogen recycling and molybdenum impurity emission from a movable limiter in TRIAM-1M Tokamak

R. Bhattacharyay; H. Zushi; K. Nakashima; Taiichi Shikama; M. Sakamoto; N. Yoshida; Shinichiro Kado; Keiji Sawada; Y. Hirooka; K. Nakamura; K. Hanada; H. Idei; M. Hasegawa; K.N. Sato; M. Ogawa; O. Takaki; K. Sasaki; H. Xu; S. Kawasaki; Hiroshi Nakashima; Aki Higashijima

In order to investigate the surface temperature effects on plasma fuel recycling and impurity release from the plasma facing components, plasma discharges have been performed under selected plasma–wall interaction (PWI) conditions in the high-field superconducting tokamak, TRIAM-1M. By moving a water-cooled molybdenum movable limiter (ML) beyond the last closed flux surface, as defined by poloidal limiters, the surface temperature profile on it is varied. Hot spots have been observed on the ML surface in such conditions. The release behaviour of fuel as well as impurity particles from the ML surface has been studied as a function of hot spot temperature (Thot) by means of wide range spectroscopy (200–1600 nm). A critical Thot is found to be ~2100 K above which the emission of both hydrogen and impurity particles enhances significantly. This is indicative of some thermally activated process playing an important role in PWIs between the limiter and the edge plasma. With the rise in hot spot temperature localized PWI at the ML is found to dominate the global recycling even when external fuelling is stopped.


Nuclear Fusion | 2006

Electron cyclotron current drive experiments in LHCD plasmas using a remote steering antenna on the TRIAM-1M tokamak

H. Idei; K. Hanada; H. Zushi; K. Ohkubo; M. Hasegawa; S. Kubo; S. Nishi; A. Fukuyama; K.N. Sato; Kazuo Nakamura; M. Sakamoto; Atsuhiro Iyomasa; S. Kawasaki; Hiroshi Nakashima; Aki Higashijima; T. Notake; T. Shimozuma; S. Ito; Hiroyuki Hoshika; N. Maezono; K. Nakashima; M. Ogawa

A remote steering antenna was recently developed for electron cyclotron heating and current drive (ECH/ECCD) experiments on the TRIAM-1M tokamak. This is the first application of the remote steering antenna concept for ECH/ECCD experiments, which have conditions relevant to the International Thermonuclear Experimental Reactor (ITER). Fundamental ECH and ECCD experiments were conducted in the ITER frequency from the low field using this antenna system. In addition to the angles near 0°, the launcher was a symmetric direction antenna with an extended steering-angle capability of ±(8°–19°). The output beam from the antenna was a well-defined Gaussian with a proper steering angle. The Gaussian content and the steering-angle accuracy were 0.85 and −0.5°, respectively. The high power tests measured the antenna transmission efficiency at 0.90–0.94. The efficiencies obtained in the low and high power tests were consistent with the calculations using higher-order modes. In order to excite the pure O/X-modes in the oblique injection, two polarizers were used to control the elliptical polarization of the incident beam for the ECCD experiments. The fundamental O/X-mode ECH/ECCD was applied to lower hyrid current drive plasmas at the optimized incident polarization. In the X-mode experiment, at medium density (~1 × 1019 m−3), clear differences in the plasma current and the hard x-ray intensity were observed between the co- and counter-steering injections due to the ECCD effect on the coupling of forward fast electrons.


symposium on fusion technology | 2003

Sensorless sensing of plasma horizontal position on HT-7

Kazuo Nakamura; Z.S. Ji; B. Shun; P.Q. Qin; S.-I. Itoh; K. Hanada; M. Sakamoto; E. Jotaki; M. Hasegawa; Atsuhiro Iyomasa; S. Kawasaki; Hiroshi Nakashima

Abstract Sensorless sensing experiments of the plasma horizontal position have been carried out in the superconducting tokamak HT-7. The horizontal position is calculated from the vertical field coil current and voltage in two ways. The calculations are made focusing on the low frequency component and the ripple frequency component of the power supply. In the latter case, there is no drift problem and the error is lower than 2% of the plasma minor radius.


Plasma Science & Technology | 2016

Power Balance Estimation in Long Duration Discharges on QUEST

K. Hanada; H. Zushi; H. Idei; Kazuo Nakamura; M. Ishiguro; S. Tashima; E. Kalinnikova; Y. Nagashima; M. Hasegawa; A. Fujisawa; A. Higashijima; S. Kawasaki; Hiroshi Nakashima; Osamu Mitarai; A. Fukuyama; Y. Takase; X. Gao; Haiqing Liu; J. Qian; M. Ono; R. Raman

Fully non-inductive plasma start-up was successfully achieved by using a well-controlled microwave source on the spherical tokamak, QUEST. Non-inductive plasmas were maintained for approximately 3–5 min, during which time power balance estimates could be achieved by monitoring wall and cooling-water temperatures. Approximately 70%–90% of the injected power could be accounted for by calorimetric measurements and approximately half of the injected power was found to be deposited on the vessel wall, which is slightly dependent on the magnetic configuration. The power distribution to water-cooled limiters, which are expected to be exposed to local heat loads, depends significantly on the magnetic configuration, however some of the deposited power is due to energetic electrons, which have large poloidal orbits and are likely to be deposited on the plasma facing components.


IEEE Transactions on Plasma Science | 2014

Shape Reconstruction of RF-Driven Divertor Plasma on QUEST

Kazuo Nakamura; H. Fujita; Xiaolong Liu; Erbing Xue; Fan Xia; Osamu Mitarai; Kenichi Kurihara; Y. Kawamata; M. Sueoka; M. Hasegawa; K. Tokunaga; H. Zushi; K. Hanada; A. Fujisawa; K. Matsuoka; H. Idei; Y. Nagashima; S. Kawasaki; Hiroshi Nakashima; A. Higashijima; K. Araki; A. Fukuyama

In the present RF-driven plasma with a lot of high-energy electrons, there may be anisotropic plasma pressure, which makes difficult a usual equilibrium analysis, but the CCS method can reconstruct the plasma shape precisely regardless of the anisotropy. And the plasma current effect in the open magnetic surfaces outside of the closed magnetic surfaces is considered in the RF-driven plasma. Further high-energy particle guiding center orbits are calculated aiming at estimation of the open-magnetic-surface current distribution.


Nuclear Fusion | 2004

Current ramp-up experiments in full current drive plasmas in TRIAM-1M

K. Hanada; Kazuo Nakamura; M. Hasegawa; S.-I. Itoh; H. Zushi; M. Sakamoto; E. Jotaki; S.V. Kulkarni; Atsuhiro Iyomasa; S. Kawasaki; Hiroshi Nakashima; N. Yoshida; K. Tokunaga; T. Fujiwara; Osamu Mitarai

Four types of plasma current ramp-up experiments in full non-inductively lower hybrid current driven (LHCD) plasmas were executed in TRIAM-1M: (1) current start-up by a combination of electron cyclotron resonance heating (ECRH) and LHCD, (2) tail heating by additional LHCD, (3) bulk heating by ECRH and (4) spontaneous ramp-up by a transition to enhanced current drive (ECD) mode. The time evolutions of plasma current during four types of ramp-up phase were adjusted by a simple model with two different time constants, which are a time defined by the total current diffusion time and a time constant for improving the current drive efficiency. In the case of (1) and (4), the latter time constant is significant during the current ramp-up phase. The improvement in the current drive efficiency in the ECD mode is likely to be caused by the increase in the effective refractive index along the magnetic field of the lower hybrid wave.


Physics of Plasmas | 2008

Study of magnetic configuration effects on plasma boundary and measurement of edge electron density in the spherical tokamak compact plasma wall interaction experimental device using Li sheet beam

R. Bhattacharyay; H. Zushi; T. Morisaki; Y. Inada; T. Kikukawa; S. Watanabe; K. Sasaki; T. Ryoukai; M. Hasegawa; K. Hanada; K.N. Sato; K. Nakamura; M. Sakamoto; H. Idei; Tomokazu Yoshinaga; S. Kawasaki; Hiroshi Nakashima; Aki Higashijima

Two-dimensional lithium beam imaging technique has been applied in the spherical tokamak CPD (compact plasma wall interaction experimental device) to study the effects of magnetic field configurations on rf plasma boundary in the absence of any plasma current, and also for the measurement of a two-dimensional edge electron density profile. With the present working condition of the diagnostics, the minimum measured electron density can be ∼1.0×1016m−3; this is considered to be the definition for the plasma boundary. The performance of the lithium sheet beam is absolutely calibrated using a quartz crystal monitor. Experimental results reveal that magnetic field configuration, either mirror or so-called null, critically affects the rf plasma boundary. A sharp lower boundary is found to exist in magnetic null configuration, which is quite different from that in the weak mirror configuration. Theoretical calculations of particle drift orbit and magnetic connection length (wall-to-wall) suggest that only mirror...

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Hiroshi Nakashima

Brigham and Women's Hospital

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