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Featured researches published by A. Iwamoto.


Nuclear Fusion | 2000

Progress summary of LHD engineering design and construction

O. Motojima; Kenya Akaishi; H. Chikaraishi; H. Funaba; S. Hamaguchi; S. Imagawa; S. Inagaki; N. Inoue; A. Iwamoto; S. Kitagawa; A. Komori; Y. Kubota; R. Maekawa; S. Masuzaki; T. Mito; J. Miyazawa; T. Morisaki; K. Murai; T. Muroga; T. Nagasaka; Y. Nakamura; A. Nishimura; K. Nishimura; N. Noda; N. Ohyabu; A. Sagara; S. Sakakibara; R. Sakamoto; S. Satoh; T. Satow

In March 1998, the LHD project finally completed its eight year construction schedule. LHD is a superconducting (SC) heliotron type device with R = 3.9 m, ap = 0.6 m and B = 3 T, which has simple and continuous large helical coils. The major mission of LHD is to demonstrate the high potential of currentless helical-toroidal plasmas, which are free from current disruption and have an intrinsic potential for steady state operation. After intensive physics design studies in the 1980s, the necessary programmes of SC engineering R&D was carried out, and as a result, LHD fabrication technologies were successfully developed. In this process, a significant database on fusion engineering has been established. Achievements have been made in various areas, such as the technologies of SC conductor development, SC coil fabrication, liquid He and supercritical He cryogenics, development of low temperature structural materials and welding, operation and control, and power supply systems and related SC coil protection schemes. They are integrated, and nowadays comprise a major part of the LHD relevant fusion technology area. These issues correspond to the technological database necessary for the next step of future reactor designs. In addition, this database could be increased with successful commissioning tests just after the completion of the LHD machine assembly phase, which consisted of a vacuum leak test, an LHe cooldown test and a coil current excitation test. These LHD relevant engineering developments are recapitulated and highlighted. To summarize the construction of LHD as an SC device, the critical design with NbTi SC material has been successfully accomplished by these R&D activities, which enable a new regime of fusion experiments to be entered.


Nuclear Fusion | 2005

Foam materials for cryogenic targets of fast ignition realization experiment (FIREX)

Keiji Nagai; H. Azechi; Fuyumi Ito; A. Iwamoto; Y. Izawa; Tomoyuki Johzaki; R. Kodama; K. Mima; T. Mito; M. Nakai; Nobukatsu Nemoto; Takayoshi Norimatsu; Y. Ono; Keisuke Shigemori; H. Shiraga; K. A. Tanaka

Development of foam materials for cryogenically cooled fuel targets is described in this paper. The fabrication development was initiated as a part of the fast ignition realization experiment (FIREX) project at the ILE, Osaka University under a bilateral collaboration between Osaka University and National Institute for Fusion Science (NIFS). For the first stage of FIREX (FIREX-I), a foam cryogenic target was designed in which low-density foam shells with a conical light guide will be fuelled through a narrow pipe and will be cooled down to the cryogenic temperature. Acrylic polymer, resorcinol–formaldehyde (RF) resin, poly(4-methyl-1-pentene) (PMP), and polystyrene-based crosslinking polymer have been investigated as supporting materials for cryogenic fuel. The properties of the material and the present status of the material development are summarized.


Cryogenics | 1998

Extra AC losses for a CICC coil due to the non-uniform current distribution in the cable

T. Mito; K. Takahata; A. Iwamoto; R. Maekawa; N. Yanagi; T. Satow; O. Motojima; J. Yamamoto; Fumio Sumiyoshi; S. Kawabata; Naoki Hirano

Extra AC losses were observed during the Experiments on a Single Inner Vertical coil (EXISV). The Inner Vertical (IV) coils are the smallest poloidal coils for the Large Helical Device (LHD) and their inner and outer diameters are 3.2 m and 4.2 m, respectively. The coil consists of 16 pancake coils wound with cable-in-conduit conductor (CICC) whose strands are NbTi/Cu without any surface coating. Many causes for the extra AC losses were considered, such as the decrease of a contact resistance between strands due to the large electromagnetic force in the conductor or due to the stress during the coil winding process, etc. and possibilities were investigated from the experimental data. Finally, we found that a coupling current with a very long time constant of 124 s caused the AC loss increase. The coupling current with such a long time constant cannot be explained from the symmetric twisting configuration of the CICC but can be explained as a local loop current corresponding to a cyclic change of the non-uniform current distributions in the cable. The non-uniform current distribution could be induced by an asymmetry of the strand transposition in the cable. To verify the above reasoning, we did fundamental experiments on a two-strands-cable, which has an intended asymmetry in the cable twisting. Extra AC losses were also observed for an asymmetric two-strands-cable, and it was demonstrated that the non-uniform current distribution causes an increase of AC losses.


IEEE Transactions on Applied Superconductivity | 2004

Asymmetrical normal-zone propagation observed in the aluminum-stabilized superconductor for the LHD helical coils

N. Yanagi; S. Imagawa; Yoshimitsu Hishinuma; Kazutaka Seo; K. Takahata; S. Hamaguchi; A. Iwamoto; Hirotaka Chikaraishi; H. Tamura; Sadatomo Moriuchi; S. Yamada; A. Nishimura; T. Mito; O. Motojima

Transient normal-transitions have been observed in the superconducting helical coils of the Large Helical Device (LHD). Stability tests have been performed for an R&D coil as an upgrading program of LHD, and we observed asymmetrical propagation of an initiated normal-zone. In some conditions, a normal-zone propagates only in one direction along the conductor and it hence forms a traveling normal-zone. The Hall electric field generated in the longitudinal direction in the aluminum stabilizer is a plausible candidate to explain the observed asymmetrical normal-zone propagation.


Nuclear Fusion | 2009

Plasma physics and laser development for the Fast-Ignition Realization Experiment (FIREX) Project

H. Azechi; K. Mima; Yasushi Fujimoto; Shinsuke Fujioka; H. Homma; M. Isobe; A. Iwamoto; Takahisa Jitsuno; Tomoyuki Johzaki; R. Kodama; Mayuko Koga; K. Kondo; Junji Kawanaka; T. Mito; Noriaki Miyanaga; O. Motojima; M. Murakami; Hideo Nagatomo; Keiji Nagai; M. Nakai; H. Nakamura; Tuto Nakamura; Tomoharu Nakazato; Yasuyuki Nakao; Katsunobu Nishihara; Hiroaki Nishimura; Takayoshi Norimatsu; T. Ozaki; H. Sakagami; Y. Sakawa

Since the approval of the first phase of the Fast-Ignition Realization Experiment (FIREX-I), we have devoted our efforts to designing advanced targets and constructing a petawatt laser, which will be the most energetic petawatt laser in the world. Scientific and technological improvements are required to efficiently heat the core plasma. There are two methods that can be used to enhance the coupling efficiency of the heating laser to the thermal energy of the compressed core plasma: adding a low-Z foam layer to the inner surface of the cone and employing a double cone. The implosion performance can be improved in three ways: adding a low-Z plastic layer to the outer surface of the cone, using a Br-doped plastic ablator and evacuating the target centre. An advanced target for FIREX-I was introduced to suit these requirements. A new heating laser (LFEX) has been constructed that is capable of delivering an energy of 10 kJ in 10 ps with a 1 ps rise time. A fully integrated fast-ignition experiment is scheduled for 2009.


Physics of Plasmas | 2009

Shock Hugoniot and temperature data for polystyrene obtained with quartz standard

N. Ozaki; Tomokazu Sano; Masahiro Ikoma; Keisuke Shigemori; Tomoaki Kimura; Kohei Miyanishi; T. Vinci; F. H. Ree; H. Azechi; Takuma Endo; Yoichiro Hironaka; Y. Hori; A. Iwamoto; Toshihiko Kadono; Hideo Nagatomo; M. Nakai; Takayoshi Norimatsu; Takuo Okuchi; Kazuto Otani; Tatsuhiro Sakaiya; Katsuya Shimizu; Akiyuki Shiroshita; Atsushi Sunahara; Hideki Takahashi; R. Kodama

Equation-of-state data, not only pressure and density but also temperature, for polystyrene (CH) are obtained up to 510 GPa. The region investigated in this work corresponds to an intermediate region, bridging a large gap between available gas-gun data below 60 GPa and laser shock data above 500 GPa. The Hugoniot parameters and shock temperature were simultaneously determined by using optical velocimeters and pyrometers as the diagnostic tools and the α-quartz as a new standard material. The CH Hugoniot obtained tends to become stiffer than a semiempirical chemical theoretical model predictions at ultrahigh pressures but is consistent with other models and available experimental data.


Physical Review B | 2011

Laser-shock compression and Hugoniot measurements of liquid hydrogen to 55 GPa

Tomokazu Sano; Norimasa Ozaki; Tatsuhiro Sakaiya; Keisuke Shigemori; Masahiro Ikoma; Tomoaki Kimura; Kohei Miyanishi; Takuma Endo; Akiyuki Shiroshita; Hideki Takahashi; Tatsuya Jitsui; Y. Hori; Yoichiro Hironaka; A. Iwamoto; Toshihiko Kadono; M. Nakai; Takuo Okuchi; Kazuto Otani; Katsuya Shimizu; Tadashi Kondo; R. Kodama; K. Mima

KYOKUGEN, Center for Quantum Science and Technology under Extreme Conditions,Osaka University, Toyonaka, Osaka 560-8531, Japan(Dated: January 7, 2011)The principal Hugoniot for liquid hydrogen was obtained up to 55 GPa under laser-driven shockloading. Pressure and density of compressed hydrogen were determined by impedance-matching toa quartz standard. The shock temperature was independently measured from the brightness of theshock front. Hugoniot data of hydrogen provide a good benchmark to modern theories of condensedmatter. The initial number density of liquid hydrogen is lower than that for liquid deuterium, andthis results in shock compressed hydrogen having a higher compression and higher temperature thandeuterium at the same shock pressure.


Nuclear Fusion | 2007

Achievement of high availability in long-term operation and upgrading plan of the LHD superconducting system

S. Imagawa; N. Yanagi; S. Hamaguchi; T. Mito; K. Takahata; H. Tamura; S. Yamada; R. Maekawa; A. Iwamoto; H. Chikaraishi; S. Moriuchi; H. Sekiguchi; K. Ooba; M. Shiotsu; T. Okamura; A. Komori; O. Motojima

The Large Helical Device (LHD) is not only the largest stellarator for the research of fusion plasma near a reactor region but also the largest superconducting system. Availability higher than 98% has been achieved in the long-term continuous operation both in the cryogenic system and in the power supply system. It is due to the robustness of the systems and efforts of maintenance and operation. One big problem is the shortage of cryogenic stability of a pair of pool-cooled helical coils. Composite conductors had been developed to attain sufficient stability at high current density. However, it was revealed that a normal-zone could propagate below the cold-end recovery current by additional heat generation due to the slow current diffusion into a thick pure aluminium stabilizer. Besides, a novel detection system with pick-up coils along the helical coils revealed that normal-zones were initiated near the bottom of the coil where the field is not the highest. Therefore, the cooling condition around the innermost layers, the high field area, will be deteriorated at the bottom of the coil by bubbles gathered by buoyancy. In order to raise the operating currents, methods for improving the cryogenic stability have been examined and stability tests have been carried out with a model coil and small coil samples. We selected a method to lower temperatures of the coil and an additional cooler has been installed at the inlet of the coil. The outlet temperatures of the coil have been successfully lowered to 3.8 from 4.4 K of the saturated temperature, as planned.


Cryogenics | 2001

Kapitza conductance of an oxidized copper surface in saturated He II

A. Iwamoto; R. Maekawa; T. Mito

The heat transfer from a metal to He II is determined by Kapitza conductance at the interface. Surface temperature estimation of the metal is used for the study of Kapitza conductance. The surface temperature is usually extrapolated from the temperature gradient in the metal. In the case of the metal with a coated layer, however, it is difficult to estimate the surface temperature. A similar case is applied for the superconductor of the helical coil of the large helical device (LHD). The copper surface is chemically treated by oxidation in order to improve the heat transfer characteristics in He I. It is planned that the helical coil will be cooled by He II in the phase II upgrade. The Kapitza conductance of the conductor has to be estimated for a stability analysis. Therefore, the heat transfer from the oxidized copper surface to the saturated He II has been measured using an oxygen-free copper cylinder. To investigate the thermal resistance in the oxidized layer, two coating surfaces are prepared: (a) coated with Stycast; (b) coated with Stycast on the oxidation layer. In this paper, the Kapitza conductance of the chemically oxidized copper surface is discussed.


Nuclear Fusion | 2000

Overview of long pulse operation in the Large Helical Device

M. Fujiwara; Y. Takeiri; T. Shimozuma; T. Mutoh; Y. Nakamura; S. Yamada; S. Sudo; K. Kawahata; Y. Oka; M. Sato; N. Noda; A. Iiyoshi; K. Adachi; Kenya Akaishi; N. Ashikawa; H. Chikaraishi; P. de Vries; M. Emoto; H. Funaba; M. Goto; K. Ida; H. Idei; K. Ikeda; S. Imagawa; S. Inagaki; M. Isobe; A. Iwamoto; S. Kado; O. Kaneko; S. Kitagawa

The Large Helical Device is the worlds largest heliotron type helical system, with the plasma confining magnetic field being generated by only external superconducting coils. One of the main objectives of the LHD project is to sustain high temperature plasmas for a long time in steady state. The plasma vacuum vessel and the divertor are water cooled, and a heat load of 3 MW can be removed continuously. The NBI, ECH and ICRF heating systems, diagnostic instruments and data acquisition system are designed for long pulse operation. The present status of these systems and the recent experimental results of long pulse operation are reviewed. A steady state discharge with NBI was obtained for 35 s. The ECH discharge duration was extended to 120 s with a duty factor of 95%. Plasma sustainment by ICRF alone was achieved for 2 s. The performance of these long pulse operations is summarized.

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K. Takahata

Graduate University for Advanced Studies

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S. Imagawa

Graduate University for Advanced Studies

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Keiji Nagai

Tokyo Institute of Technology

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