Shigeki Maruyama
Toshiba
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12th International Conference on Nuclear Engineering, Volume 1 | 2004
Yoshihisa Nishi; Nobuyuki Ueda; Izumi Kinoshita; Tomonari Koga; Satoshi Nishimura; Tsugio Yokoyama; Shigeki Maruyama; Kimitaka Kimura; Shigeo Kasai
CRIEPI (Central Research Institute of Electric Power Industry) has been developing the 4S reactor (Super Safe, Small and Simple reactor) for application to dispersed energy supply and multipurpose use, with Toshiba Corporation [1,2,3,4]. Electrical output of the 4S reactor is from 10MW to 50MW, and burn-up reactivity loss is regulated by neutron reflectors. The reflector that surrounds the core is gradually lifted up to control the reactivity according to core burn-up. 30year core lifetime without refueling can be achieved with the 10MW 4S (4S-10M) reactor. All temperature feedback reactivity coefficients, including coolant void reactivity, of the 4S-10M are negative during the 30year lifetime. A neutron absorption rod is set at the center of the reactor core with the ultimate shutdown rod. The neutron absorption rod used during the former 14 years is moved to the upper part of the reactor core, and the operation is continued through the latter 16 years. The pressure loss of the reactor core is lower than 2kg/cm2 to enable effective utilization of the natural circulation force, and the average burn-up rate is 76GWD/t. To suppress the influence of the scale disadvantage, loop-type reactor design is one of the candidates for the 4S-10M. The size of the reactor vessel can be miniaturized by adopting the loop type design (4S-10ML). In the 4S-10ML design, integrated equipment which includes primary and secondary electromagnetic pumps (EMPs), an intermediate heat exchanger (IHX) and a steam generator (SG) is adopted and collocated by the reactor vessel. The decay heat removal systems of 4S-10ML consist of the reactor vessel air cooling system (RVACS) and SGACS (a similar system to the RVACS, with air cooling of the outside of the integrated equipment vessel). They are completely passive systems. To decrease the construction cost of the reactor building, a step mat structure and the horizontal aseismic structure are adopted. 4S-10ML has unique features in the cooling systems such as integrated equipment and two separate passive decay heat removal systems which operate at the same time. To evaluate the design feasibility, the transition analyses were executed by the CERES code developed by CRIEPI [5]. In this paper, the design concept of 4S-10ML, and the results of the plant transition analyses are described.© 2004 ASME
Volume 5: High-Pressure Technology; ASME NDE Division | 2012
Noriyasu Kobayashi; Souichi Ueno; Kota Nomura; Makoto Ochiai; Yuko Kitajima; Shigeki Maruyama
It has been demonstrated that magnetic resonant coupling is effective for improving the characteristics of ECT sensor, especially the lift-off-dependent reduced sensitivity and noise. The lift-off-dependent reduced sensitivity and noise are caused by the decrease of voltage gain from the exciter coil to detector coil. Magnetic resonant coupling is generally usable to increase the voltage gain from the transmitter coil to the receiver coil. Magnetic resonant coupling was applied to ECT in these experiments to investigate the phenomena of magnetic resonant coupling in the ECT. In the ECT setup, the voltage gain G increased more than 6 times by magnetic resonant coupling at a frequency of 105 kHz. The voltage gain ratio (GR/GNR) was rising 1.12 times when the lift-off length increased from 1mm to 2 mm. This result verified that magnetic resonant coupling has the potential for improving the characteristics of ECT. The EDM slit signal and the lift-off noise were calculated from the experimental results, respectively. Using magnetic resonant coupling, the EDM slit signal increased 1.5 times and the lift-off noise was reduced by 34 % at a lift-off length of 2mm. these results confirmed that magnetic resonant coupling is effective for improving the characteristics of ECT. Additional experiments were performed in order to verify the effect of magnetic resonant coupling for the wobbling (lift-off) noise in the tube inspection. In the vibration test of the ECT sensor inside the tube, the lift-off noise decreased by 28 % on average by magnetic resonant coupling. In the scanning test of the ECT sensor inside the tube, the wobbling and other noises were obviously reduced by magnetic resonance coupling.Copyright
Progress in Nuclear Energy | 2005
Nobuyuki Ueda; Izumi Kinoshita; Akio Minato; Shigeo Kasai; Tsugio Yokoyama; Shigeki Maruyama
Archive | 2007
Shoko Suyama; Yoshiyasu Ito; Shigeki Maruyama; Norihiko Handa
Archive | 2006
Norihiko Iida; Yoshiyasu Ito; Shigeki Maruyama; Akiko Suyama; 茂樹 丸山; 義康 伊藤; 章子 須山; 式彦 飯田
Archive | 2012
Noriyasu Kobayashi; Souichi Ueno; Kota Nomura; Makoto Ochiai; Yuko Kitajima; Shigeki Maruyama; Hiroya Ichikawa
Archive | 2004
Ryo En; Norihiko Iida; Shuichi Inagaki; Yoshiyasu Ito; Tsuneji Kameda; Shigeki Maruyama; Akiko Suyama; 茂樹 丸山; 常治 亀田; 義康 伊藤; 修一 稲垣; 章子 須山; 式彦 飯田
Archive | 2004
Norihiko Iida; Yoshiyasu Ito; Tsuneji Kameda; Shigeki Maruyama; Akiko Suyama; 茂樹 丸山; 常治 亀田; 義康 伊藤; 章子 須山; 式彦 飯田
Archive | 2011
Takehisa Hino; Masataka Tamura; Yoshimi Tanaka; Wataru Kono; Toru Sakamoto; Toshinori Terashima; Katsuhiko Sato; Noboru Jimbo; Shigeki Maruyama
Archive | 2009
Shigeki Maruyama; Naoto Yoshihara; 茂樹 丸山; 直人 吉原