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ORNL-4191 - the Molten Salt Energy Technologies Web Site

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0 2 4 6810<br />

LLLLLLU 1<br />

INCHES<br />

COOLING CHANNEL<br />

/<br />

69<br />

Fig. 5.6. Reactor Cell Construction - Component Support Penetration<br />

first with a %in. air gap between <strong>the</strong> two. A sim-<br />

ilar second plate and air gap would be provided<br />

for <strong>the</strong> floor. During reactor opetai ion, cooling<br />

air would be circulated through <strong>the</strong> gap at a ve-<br />

locity of about 50 fps to remove <strong>the</strong> heat gener-<br />

ated by gamma absorptions in <strong>the</strong> wall. Cooling<br />

air is also used in <strong>the</strong> removable roof plugs, <strong>the</strong><br />

air duct connections being flanged to facilitate<br />

removal. The total heat losses from <strong>the</strong> reactor<br />

cell are estimaled to be a maximum of 800,000<br />

0RhlL-OWG 67-40644A<br />

Btu/hr. The <strong>the</strong>rmal shield could tolerate loss of<br />

cooling air for up to 1 hr without an excessive<br />

temperature rise.<br />

A 3/,,-in.-lhick carbon steel membrane is in-<br />

stalled inside <strong>the</strong> inner 3-in.-thick steel wall<br />

mentioned above. This membrane is hermetically<br />

tight and would satisfy <strong>the</strong> containment leak-rate<br />

requirements. The membrane is continuous around<br />

<strong>the</strong> top plugs and also at <strong>the</strong> penetrations of <strong>the</strong><br />

cell, as shown in Fig. 5.7. The space between it

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