Directional Distribution of Radiation around an Accident at a Uranium Fuel Factory in Tokai-mura, 1999
JUN TAKADA
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SHINJI SUGA
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KAZUHIDE KITAGAWA
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MASAYORI ISHIKAWA
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SEIJI TAKEOKA
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MASAHARU HOSHI
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HIROMITSU WATANABE
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AKIHIRO ITO
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NORIHIKO HAYAKAWA
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Research Institute for Radiation Biology and Medicine, Hiroshima University Kasumi 1-chome
, Hiroshima 734 - 8553,
Japan
(Received, July 19, 2000) (Revision received, September 25, 2000) (Accepted, December 18, 2000)
Tokaimura / Criticality accident / Radiation / Directional dependence / Residential areas A beta-ray survey was carried out on concrete walls of the boundary and buildings after a criticality accident at a factory of JCO Co. Ltd. at Tokai-mura. A remarkable distribution of beta counts was observed on the walls depending on the complex internal and external structures of buildings surrounding a precipitation vessel containing uranium 23 days after the accident. The directional distribution function, based on the beta counts on the walls, was consistent with data concerning the neutron dose rate measured in several directions during the accident, suggesting an anisotropic neutron distribution to the residential area.
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A criticality accident, which occurred at the uranium conversion facilities of JCO Co.
Ltd. in Tokai-mura, Japan on September 30, 1999, caused radiation exposure to not only
workers, but also residents1). The critical state, which occurred at 10 : 35 am, was terminated
by draining off cooling water around the precipitation vessel (PV) at 6 : 30 am on October 1.
The evacuation of people within a 350 m zone began at 15 : 30 on the same day1). During the
accident, neutrons and gamma rays exposed people around the factory. The gamma ray and
neutron dose rates were reported to be 0.84 mSv/h (gamma) at 11 : 36, 0.5 mSv/h (gamma)
and 4.5 mSv/h (neutron) at the boundary of the factory at 19 : 09 on Sep. 30, as the maximum
values1, 2). This neutron exposure to residents was completely different from that in the
Chernobyl atomic power plant accident, and nuclear weapon tests where there was no direct
neutron exposure to the population around the site3).
A dosimetry study for residents is urgently important under such circumstances. Japan
Atomic Energy Research Institute (JAERI) reported external doses as a function of
distance2, 4). We focus here on the directional dependence of radiation from the criticality
accident due to the complex structures of the buildings between the source and the residential
area. The enriched uranium and fission products were kept in the PV (450 mm in inner
diameter) of the building where the accident occurred during our measurements. Sand-bag
walls were built on Oct. 2 for radiation protection of the residents located around the facility.
Several concrete walls were built instead of sand-bag after our measurement on Oct. 26, 1999.
A radiological survey was conducted mainly for beta counting on the wall of the boundary
and of the building after the accident under the present condition.
MATERIALS AND METHODS
Beta counting was conducted at about 1-m height on the walls using a ZnS (Ag) plastic
sintilator (Aloka TCS-352, active area of 72 cm2). The detection efficiencies for beta rays
(Emax = 310 keV) and gamma ray (Eav = 1253 keV) of Co-60 are 14.3 and 1.3 (%/2),
respectively. Each measurement was done for one minute. The main measurements were carried out
on the boundary wall, which was made of concrete with 3 cm thick exists, the length between
northeast and southwest was 880m, as shown in Fig. 1 on Oct. 23 25. The values at three
points with 80 cm intervals, which were measured at each site of the boundary wall, were
averaged. The sites on the outer wall of facility where measurements were made on Oct. 26
are shown in Fig. 2. The number of measurements was one for each site in this case. The
Fig. 1. Local map of the facility for uranium fuels factory in Tokai where the accident took place. Beta
counting was carried out on walls B1, B2 and B3 at the boundary of the factory.
Fig. 2. Measurement sites on the outer wall of the buildings around the critical uranium source. The
number of high beta count sites (more than 10 kcpm) is indicated by circles. The sites of maximum
beta counts on walls B1 and B2 are marked by bars. The values of No. 911 of the C building were
estimated to be more than 10 kcmp from the corresponding gamma dose rates (see Table 1).
entire wall is also made of the same material and thickness (autoclaved light concrete with 10
cm thickness, Siporex, Sumitomo Metal Mining Co., Ltd.,).
A clear distribution of beta counts was observed on the western B1 and northern B2
walls, as shown in Fig. 3. In this figure, the net count was evaluated from the gross counts
subtracted by the background value of 137 cpm, which was assumed to be average one for
data beyond 300 m from the northwestern corner of the wall. Moreover, each point was
recalculated by smoothing with neighboring points (ni = (ni 1 + ni + ni+1)/3). The maximum net
values were about 3 sigma (12 cpm) of the raw background counts in the B1 and B2 walls. On
the other hand, the level of net counts on the eastern wall (B3) was about within one sigma
of the background count. Therefore, the distribution of beta count rate on this B3 wall was not
clear due to the distant area about 500 m east away from the uranium source.
The distribution of beta counts in the B1 wall had a maximum at 85 m from the
northwestern corner with full width at half maximum (FWHM) of 40 m. The count rates sharply
Fig. 3. Net beta counts on walls B1 and B2 plotted as a function of the distance from the
northwestern corner on October 23 25 1999. The data were smoothed by 3 continuous points.
decreased toward southern side from this site. This may have been due to the shielding of the
E-building for radiation, as shown in Fig. 2. The distribution of the beta count rate at the B2
wall had the maximum value at 50 m from the northwestern corner with a FWHM of 29 m.
An obvious distribution of beta count rates was also observed on the outer wall of several
buildings, as shown in Fig. 2 and Table 1. The most remarkable site was No. 7 of the
Dbuilding with a beta count of 31 kcpm. The values were about 30-times higher than those on
neighboring sites of both sides on the same wall. There was no concrete wall but two iron
doors between site No. 7 and the uranium source in the C-building. Neutrons passing through
the iron door from the source might strongly irradiate the wall at site No. 7. We notice that
site No. 7 of the D-building is on one line between the source in the C-building and the
maximum site of the B1 wall. Moreover, a remarkable distribution of beta counts was observed on
the outer walls of the C-building of the facility where the accident occurred. Sites No. 7 and
No. 8 at the northeastern wall of the C-building exhibited more than 10 kcpm. This wall has
no glass windows. The distance between the source and the residents is more than 400 m, and
several buildings exist in the northeastern direction. In the northweste (...truncated)