The heat source of RPV (fuel debris) was estimated based on the trend of the temperature around the RPV in the post-accident condition, water temperature of S/C, water injection amounts of feedwater (FDW) system and reactor core spray (CS) system. Figure 1 shows difference between flow paths of the FDW system and CS system. FDW system is a system that introduces the cooling water during the normal operation of BWR into the RPV. After flowing into the RPV, cooling water is accumulated in the space between reactor core shroud and the RPV (annulus), it will be flowing into the jet pump at the time when the water level reaches to the upper part of the jet pump mixer. If the integrity of the bottom of the RPV is maintained, the cooling water flowed in will accumulated inside the RPV and water level of the accumulated water will be raised. However, since increase in the water level was not observed, the bottom of the RPV has been damaged and the cooling water is estimated to be flown down from the damaged portion to the inside of the pedestal. That is, FDW system water injection cannot cools down the BWR reactor core portion but the bottom part of the RPV, even after the accident. While on the other hand, CS system is a core spray system during the coolant loss accident and is installed along the walls immediately above the core reactor core shroud. In the CS system water injection, the cooling water is flowing down the space from the reactor core to the bottom of the RPV and the scape can be cooled down. Based on the above, the fuel debris locations were estimated for each Unit.
Figure 1縲Flow path of FDW and CS systems
Shown below is the fuel debris distribution for each unit estimated from the trend of the plant parameters.
Figure 2 shows temperatures at several positions inside the PCV of Unit 1 along with changes in the quantity of injected water and measurement locations. In response to the changes in the quantity of injected water, the following characteristic changes in temperature were observed.
With the characteristics shown in (1), (2), and (3) above, it is estimated that the heat source is probably is small inside the RPV. From (3) and (4), it is assumed that a heat source may exist in the water injection channel for the FDW system and the heat removed in response to water injection has transferred to the S/C.
Figure 2縲Changes in Plant Parameter and Measurement Locations for Unit 1
Figure 3 shows the temperatures at several positions inside the PCV of Unit 2 along with changes in the amount of injected water and measurement locations. In response to the changes in the amount of injected water, the following characteristic temperature changes were observed.
With the characteristics shown in (1), (3), (4), and (5), it is estimated that a certain quantity of heat source may exist inside the RPV; from (2), it is assumed that the lower RPV head is closer to the heat source than the water supply nozzle (N4B). From (3), it is deemed that the removed heat had transferred to the S/C.
Figure 3縲Changes in Plant Parameter and Measurement Locations for Unit 2
Compared with Unit 1, the ambient temperature of the PRV is high, which was higher than 100ツーC even six months after the accident; as with Unit 2, it is assumed that a certain percentage of fuel debris exists in both of the RPV and PCV. The procedure for the above estimation is shown below:
With the characteristics shown in (1), (3), and (4) above, it is estimated that a heat source may exist inside the RPV.
Figure 4縲Changes in Plant Parameter and Measurement Locations for Unit