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ORNL-TM-7207 - the Molten Salt Energy Technologies Web Site

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36<br />

immediately because of deposition of energy by fast neutrons and prompt<br />

gammas, Because <strong>the</strong> heat capacity of <strong>the</strong> moderator in a zone is always<br />

at least five times that of <strong>the</strong> fuel, <strong>the</strong> effect of direct transient mad-<br />

erator heating would be negligible.<br />

The reflector and vessel coefficients would probably be very slow in<br />

taking effect because of large heat capacities and Pow fuel flow rates.<br />

Their total is dominated by a negative expansion tern.<br />

3 0 1 e 7 B 3 Belayed-neutron effects<br />

Table 21. Delayed-neutron fraction, 6<br />

Contributor Fissiom fraction Contribution t o B<br />

2 q J 0,55<br />

235~ 0.23<br />

B1 u e. oni urn 0.22<br />

0.0014<br />

Q.OOP5<br />

0 * 00046<br />

Total B 0.0034<br />

An unusual aspect of MSRs 1s that <strong>the</strong> fuel circulates fast enough to<br />

remove significant numbers of delayed-neutron precursors from <strong>the</strong> core be-<br />

fore <strong>the</strong> neutrons are emitted. The Lmped-parmeter kinetics equations<br />

are taken as<br />

and<br />

.. ....<br />

,. . .,<br />

".IW

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