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transient calculations of coolant mixing in vver-440/213 rpv

transient calculations of coolant mixing in vver-440/213 rpv

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Fig. 5: Tempreature distribution on the wall <strong>of</strong> RPV and pipe<br />

ECS INJECTION ABOVE THE CORE<br />

The assumed <strong>in</strong>itial conditions <strong>of</strong> the next <strong>transient</strong>: the reactor is <strong>in</strong> hot shut down condition, i.e.<br />

the ma<strong>in</strong> <strong>coolant</strong> pumps are stopped. There is natural circulation <strong>in</strong> two loops (2 nd and 6 th loops<br />

are opened), the <strong>coolant</strong> mass flow rate <strong>in</strong> these two loops is 40 kg/s. The temperature <strong>of</strong> the<br />

<strong>coolant</strong> is 140 o C, the pressure is 0,5 MPa. The ECCS <strong>in</strong>jects water <strong>in</strong>to the 4 th loop and through<br />

the hydro-accumulator nozzles. The mass flow <strong>of</strong> the <strong>in</strong>jected water is 50 kg/s, the temperature is<br />

35 o C.<br />

The duration <strong>of</strong> the <strong>transient</strong> was 60 s. In the calculation buoyancy was taken <strong>in</strong>to account, and<br />

because <strong>of</strong> the large <strong>coolant</strong> temperature differences temperature dependent material properties<br />

were used.<br />

For this simulation only the core and the structural elements above the core were modelled <strong>in</strong><br />

details. The goal was to simulate the <strong>mix<strong>in</strong>g</strong> <strong>in</strong> the upper plenum so this is the reason why the<br />

lower plenum was neglected for this case.<br />

Fig. 6: The model <strong>of</strong> the core and the upper plenum<br />

The <strong>in</strong>jected water cools down the <strong>coolant</strong> <strong>in</strong> the 4 th loop and enters <strong>in</strong>to the vessel <strong>in</strong> the 23 rd<br />

second. The colder water flows around the perforated reactor pit and passes through the

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