Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Nagaya, Yasunobu; Mori, Takamasa; Brown, F. B.*
Monte Karuro Keisanho Kodoka No Genjo; Dai-3-Kai Monte Karuro Shimyureshon Kenkyukai Hobunshu, p.105 - 115, 2004/12
The Monte Carlo perturbation method based on the differential operator sampling method has been widely used to obtain a small change in neutronic parameters or sensitivity. The method is very effective for fixed-source problems but a difficulty arises for eigenvalue problems because the fission source distribution is perturbed. Most Monte Carlo codes assume that the source distribution is unchanged after a perturbation is introduced. However, this assumption can lead to a significant error in the perturbation estimate. Recently, a method to estimate the perturbed fission source effect has been proposed. In this method, the additional weights for the differential coefficient of the fission source at fission sites are normalized in each cycle, and the effect is estimated by propagating the normalized additional weight between cycles. The method and benchmark results have been reviewed. It has been found that this method is very effective in perturbation calculations for the effective multiplication factor.
Yamamoto, Toshihiro; Miyoshi, Yoshinori
Journal of Nuclear Science and Technology, 41(2), p.99 - 107, 2004/02
Times Cited Count:38 Percentile:90.02(Nuclear Science & Technology)A new algorithm of Monte Carlo criticality calculations for implementing Wielandt's method is developed. In this algorithm, part of fission neutrons emitted during random walk processes are tracked within the same generation, and thus a fission source distribution in the next generation spread more widely. Applying this method intensifies a neutron interaction effect even in a loosely-coupled array where conventional Monte Carlo criticality calculation methods have difficulties, and a converged fission source distribution can be obtained with fewer generations. Computing time spent for one generation, however, increases because of tracking fission neutrons within the same generation, which eventually results in an increase of total computing time up to convergence. However, since a fission source convergence is attained with fewer source iterations, a reliable determination of convergence can easily be made even in a system with a slow convergence.
*; *; *
JAERI-Data/Code 99-016, 183 Pages, 1999/03
no abstracts in English
*
JAERI-Data/Code 97-016, 34 Pages, 1997/05
no abstracts in English
*
JAERI-Data/Code 97-011, 25 Pages, 1997/03
no abstracts in English
; *; *; *; *; *; *; Yokokawa, Mitsuo;
Joho Shori Gakkai Kenkyu Hokoku, 96(81), p.129 - 134, 1996/08
no abstracts in English
*; Tokuda, Shinji; Uyama, Tadao*
JAERI-Research 95-050, 29 Pages, 1995/07
no abstracts in English
PNC TN9410 90-099, 73 Pages, 1990/06
Fluid-structure interaction affects dynamic characteristics of LMFBR reactor structures, and should be taken into consideration in their seismic safety evalutions. This is due to that a reactor vessel of LMFBR is relatively thin-walled structure and it contains a large amount of liquid metal sodlum. In this study, natural frequencies of liquid-filled tanks (a flat bottom end plate type and a spherical head type) were analyzed by FINAS with a purpose of understanding the dynamic behavior of liquid-filled tanks. The analysis results by FINAS were found to be satisfactory accurate as compared to the exliting solutions. And a computational study was made on vibration characteristics of tanks and follwing knowledge was obtaind. (1)The lowest natural frequency of a shell takes place not in a beam mode, but in a higher order (5th10th) shell mode. (2)In case of a tank with a spherical head, elgenmode shapes are very complex; The spherical head part tends to vibrate mainly in the lower order shell modes, and the cylinderical part vibrate in the higher order modes. (3)The center of the spherical head becomes a nodal point in the beam modes and the shell modes. But in the axial modes, the center becomes a point of maximum amplitude.
Fujimura, Kaoru
JAERI-M 90-057, 28 Pages, 1990/03
no abstracts in English
JAERI-M 85-171, 20 Pages, 1985/11
no abstracts in English
JAERI-M 82-083, 47 Pages, 1982/07
no abstracts in English
; ; *; *; *; ;
Journal of Nuclear Science and Technology, 19(8), p.628 - 637, 1982/00
Times Cited Count:2 Percentile:32.87(Nuclear Science & Technology)no abstracts in English
Journal of the Physical Society of Japan, 51(6), p.2000 - 2009, 1982/00
Times Cited Count:7 Percentile:60.8(Physics, Multidisciplinary)no abstracts in English
Tsunematsu, Toshihide; Takeda, Tatsuoki; *; *; *
JAERI-M 7573, 12 Pages, 1978/03
no abstracts in English
Tsunematsu, Toshihide; Takeda, Tatsuoki
J.Comput.Phys., 28(2), p.287 - 293, 1978/02
Times Cited Count:4no abstracts in English
Amano, Tsuneo*;
JAERI-M 6401, 31 Pages, 1976/02
no abstracts in English