44
K. Hashimoto
Fig. 2.24 Plot of variables
and fitted line on
x-y coordinate (Ref. [28])
(a) Beam trip experiment
(b) Beam restart experiment
decay of B1 data just after the trip, as noted above. For an actual ADS, a neutron
counter should be placed at a position far from a spallation target. Table 2.3 also
shows that the results of the LSIKM for beam trip data are consistent with those of
the integral count technique except for counter B1.
As seen from Tables 2.3 and 2.4, the present subcriticality obtained using the
counters other than B1 has a slight counter-position dependence compared with
K. Hashimoto
Fig. 2.24 Plot of variables
and fitted line on
x-y coordinate (Ref. [28])
(a) Beam trip experiment
(b) Beam restart experiment
decay of B1 data just after the trip, as noted above. For an actual ADS, a neutron
counter should be placed at a position far from a spallation target. Table 2.3 also
shows that the results of the LSIKM for beam trip data are consistent with those of
the integral count technique except for counter B1.
As seen from Tables 2.3 and 2.4, the present subcriticality obtained using the
counters other than B1 has a slight counter-position dependence compared with