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RRFM 2009 Transactions - European Nuclear Society

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Calculated/Experimental (C/E)<br />

Axial Position *F8 F6<br />

-17.8 1.11 1.12<br />

-12.8 1.14 1.16<br />

-7.8 1.11 1.14<br />

-2.8 1.14 1.15<br />

2.2 1.04 1.06<br />

7.2 1.00 1.01<br />

12.2 0.96 0.96<br />

17.2 0.85 0.91<br />

22.2 0.81 0.82<br />

27.2 0.87 0.89<br />

Table 2: Ratio (C/E) of calculated to experimental total nuclear heating in Stainless steel (SS304) core<br />

calorimeter<br />

4.2 Molybdenum Core Calorimeter<br />

The heating of molybdenum is expected to be dominated by gamma heating since has a<br />

relatively high atomic number (Z) compared to stainless steel (Z~29). Figure 4 presents total<br />

nuclear heating rates for a molybdenum core calorimeter. The *F8 and F6 tallies are still in<br />

good agreement. Below the core centreline, there are large discrepancies between the<br />

calculated and experimental values. Better agreement is observed above the core centreline.<br />

1.0<br />

0.9<br />

Pulsed height tally (*F8)<br />

Track length estimate (F6)<br />

Experimental<br />

Total nuclear heating (W/g)<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

-20 -10 0 10 20 30<br />

Axial distance with respect to the core centerline (cm)<br />

Figure 4: Total nuclear heating in a Molybdenum core calorimeter<br />

403 of 455

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