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7.3 Moderator temperature feedback in thermal reactors 77
to travel to core boundaries and leak from the core and the opposite occurs with
decreases in mean free path. The effect of a temperature increase is to decrease mod-
erator density, increase neutron mean-free path, increase neutron leakage and reduce
reactivity. The scattering component of the moderator temperature coefficient of
reactivity is always negative.
Temperature increases in coolant/moderator cause a density increase and,
consequently, fewer coolant/moderator atoms in the reactor core. Since coolant/
moderators have non-zero absorption cross sections, temperature increase decrease
neutron absorptions. The absorption component of the coolant/moderator coeffi-
cient of reactivity is always positive.
Reactor design includes evaluation of the effect of moderator population on
available reactivity. Fig. 7.4 illustrates the effect.
Too little moderator is sub-optimal in producing available reactivity by slowing
neutrons to thermal energy. A reactor with too little moderator is said to be under-
moderated. Too much moderator is sub-optimal in producing available reactivity
because neutron absorptions override the effect of additional slowing down in the
moderator. A reactor with too much moderator is said to be over-moderated.
Light water reactors are designed to be under-moderated. That is, moderator
removal causes a reactivity decrease. Thus, a temperature increase in a liquid
moderator-coolant causes a decrease in density, a decrease in neutron slowing down
under-moderated over-moderated
k eff
REACTIVITY Resonance escape probability (p)
Thermal utilization factor (f)
MODERATOR-TO-FUEL RATIO (N m /N U )
AS TEMPERATURE INCREASES
FIG. 7.4
Effect of moderator-to-fuel ratio on reactivity in under-moderated and over-moderated
reactors.
Adapted from www.nuclear-power.net.