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RRFM 2009 Transactions - European Nuclear Society

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Fig. 3:<br />

Surface temperature over the width<br />

of the typical fuel plate of FRM II<br />

averaged over a whole cycle of<br />

60 days of full power operation.<br />

Next is shown the evolution with time of the temperature profile of the hot fluid element at a width in the<br />

channel of 5.0 cm (compare Fig. 3):<br />

• NBK calculated the absolute maximum values to lie at the bottom borders over an extent of the<br />

plates of only some mm (height =-35cm in Fig. 4). But this is not fairly true when respecting also<br />

the axial heat transfer in the plates, which cannot be neglected at the plate ends.<br />

The description of NBK shows the typical effect of heat transfer in the plates at the meat<br />

edge, where a clear local maximum in the power distribution occurs over a few mm only. The<br />

peak is fairly drawn down and in the actual case it will be not higher than the broad maximum<br />

value inside at the plate surface. This can also be confirmed by plausibility considerations.<br />

• At reactor start the power in the inner core region is shoved down by the CR being present above<br />

-7 cm (relative to the core mid plane CMP). The hottest point at the plates is located down at<br />

about -20 cm and reaches slightly more than 90°C.<br />

• With operation time during a cycle the hottest point at plates surface moves up towards the CMP<br />

and becomes clearly cooler, about 80°C till the operation cycle end at 60 FPDs. The CR is then<br />

nearly totally removed and the power density is rather symmetrically around the CMP, although<br />

the temperatures remain higher at the bottom side, since the coolant water comes from the top.<br />

228 of 455

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