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Tidal Current Energy

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The Pebble Bed Modular Reactor<br />

245<br />

� 1<br />

application, the helium flow rate down through the core is about 184 kg � s and<br />

the pressure about 9 MPa.<br />

An account of the evolution of the PBMR from the HTR-Modul concept to<br />

today’s design is given in Ref. [6] .<br />

2.1 .<br />

Controlling the reactor<br />

The routine method for raising and lowering the reactor power output is unexpected.<br />

It depends on the so-called nuclear Doppler effect. This is an aspect of<br />

the physics of uranium, more specifically of the isotope uranium-238, which is<br />

of great importance for reactor control and particularly for reactor safety. During<br />

normal operation, about 30 � 10 9 nuclei of uranium-235 (which initially constitutes<br />

9.6% of the uranium in the equilibrium core) undergo fission every second<br />

for every watt of heat being produced. In each fission event, two or three highenergy<br />

neutrons are emitted. If at least one of these fission neutrons goes on to<br />

cause a further fission, the nuclear chain reaction ‘ diverges’ and the power level<br />

rises. If not, the reaction dies away.<br />

Counter-intuitively, the neutrons are effective in causing further fission only<br />

if they are first slowed down to very low ‘ thermal ’ energies. This happens in the<br />

course of multiple collisions within a moderator, for example with carbon nuclei<br />

in the graphite comprising the fuel spheres and reflector blocks of the PBMR, or<br />

with hydrogen nuclei in the coolant water in light water reactors.<br />

The obliging property of uranium-238 is that it absorbs some of these neutrons<br />

before they have slowed down sufficiently to cause further fissions in uranium-<br />

235. More particularly, the hotter the fuel becomes, the more intermediateenergy<br />

neutrons are absorbed by nuclei of uranium-238 and thus removed from<br />

the chain reaction process. There are then fewer low-energy neutrons flying<br />

around in the core to cause fission, the fission rate in the reactor falls away and<br />

the reactor power level drops. Such is the totally reliable Doppler effect.<br />

Now consider the effect of reducing the mass of helium in the reactor pressure<br />

vessel. The helium flow down through the fuel bed is reduced and the<br />

temperature of the fuel spheres therefore rises. Thanks to the Doppler effect, the<br />

reactor power level inevitably drops. Conversely, increasing the mass of helium<br />

in the system reduces the fuel temperature and therefore causes the power level<br />

to rise.<br />

The routine way of controlling the reactor power level is thus to adjust the<br />

mass flow of helium through the core either by releasing helium from the coolant<br />

circuit or by injecting more helium into it. If it is required to change the<br />

power level more rapidly, valves can be opened to allow a fraction of the helium<br />

to bypass the reactor core. This has the same effect as reducing the helium pressure,<br />

but acts faster.<br />

A further degree of control is afforded by raising or lowering the 24 control<br />

rods of the reactivity control system (RCS) surrounding the core. These are used<br />

principally to maintain the core temperature while power-level changes are<br />

being made by adjusting the helium pressure and also when it is necessary to

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