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Phase diagram of water

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Macroscopic cross-sections for natural<br />

uranium (Σ t<br />

= Σn i<br />

σ ti<br />

)<br />

Factors affecting chain reaction<br />

1) For each thermal neutron absorbed, η effective fast neutrons emitted<br />

η < ν, mean number produced (ν =2.42 for 235 U), because not all<br />

neutrons absorbed by fuel cause fission. Nat U (0.72% 235 U) η =1.33<br />

2) Some fast neutrons cause fission before slowing down which<br />

increases the number <strong>of</strong> neutrons by the fast fission factor ε<br />

3) The probability that a neutron will avoid resonance capture by 238 U<br />

the resonance escape probability p - depends on the moderator<br />

4) The fraction <strong>of</strong> thermal neutrons that are absorbed by the fuel in the<br />

core (fuel, moderator, can) is called the thermal utilization factor f<br />

5) There are a fraction l f <strong>of</strong> fast neutrons and a fraction l t <strong>of</strong> thermal<br />

neutrons that leak out <strong>of</strong> the reactor<br />

The neutron multiplication factor k is therefore given by:<br />

k = ηεpf(1− l f ) (1− l t )<br />

For infinite core k ∞ = ηεpf<br />

Four factors formula<br />

Neutron Moderation<br />

Moderator is a medium for reducing the kinetic energy <strong>of</strong> neutrons from<br />

MeV to thermal level without losing many in the ‘resonant trap’ <strong>of</strong> 238 U<br />

m<br />

M<br />

For 180 deg scattering<br />

neutron<br />

E s = [(M − m)/(M + m)] 2 E i = [(A − 1)/(A + 1)] 2 E i<br />

For 0 deg scattering<br />

E s = E i<br />

Averaging, E s = ½{1 + [(A − 1)/(A + 1)] 2 }E s<br />

nucleus<br />

= [(A 2 + 1)/(A + 1) 2 ]E s<br />

(Averaging over all angles gives the same result)<br />

1<br />

H<br />

12<br />

C<br />

238<br />

U<br />

A 1 12 238<br />

E s /E i 0.5 0.86 0.99<br />

How many collisions required to reduce neutron energy from<br />

2 MeV to 1 eV ? (factor <strong>of</strong> 2 10 6 )<br />

Put (E s /E i ) n = 1/(2.10 6 ) = 5.10 −7<br />

eg 1 H gives n ~ 21, 12 C gives n ~ 96<br />

Moderating Ratio, MR<br />

Good moderators require<br />

• large σ elastic (σ el )<br />

• low σ capture (σ c )<br />

• significant loss in KE per collision<br />

• chemical stability (in hot, radioactive environment)<br />

Moderating ratio, MR = (1− E s /E i ) σ el /σ c<br />

Reactor Control<br />

H 2 O 62; D 2 O 4830; C 216<br />

If the neutron flux increases to a higher level than that needed for a<br />

stable chain reaction, how can the reactor be controlled, ie how can<br />

equilibrium be restored?

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