Critical masses

We give a schematic determination of critical sizes and masses of two model homogeneous reactors: a lead cooled fast neutron reactor and a heavy-water moderated thermal neutron reactor.

Fast reactor

In the one-group diffusion formalism, the critical size of a spherical homo­geneous reactor is given by equation (3.38)

2T2 — L

ki = 1 + — дГ (3-78)

with

Подпись:^

c _ xa _ 3sasT which leads to the minimum size of the sphere,

image167(3.80)

Подпись: nn image169

The physical characteristics of the medium components are given in table 3.3. The relative atomic concentrations are also given in table 3.3. The relative concentration of 232Th and 233U are in the proportion required for regeneration:

The number of lead atoms is taken as set to that of the fuel atoms. Table 3.4 gives the macroscopic cross-sections.

Table 3.3. Physical properties of the elements of the model fast reactor. Cross-sections are in barns. n is the relative pro­portion of the element.

p

Of

Oa

Of

n

232Th

11.72

10

0.458

0.014

0.435

233U

18.95

10

2.999

2.742

0.065

Pb

11.35

10

0.01

0

0.5

Подпись: Table 3.4. Macroscopic cross-sections (cm) for the model fast reactor. £s £a Ef 0.327 1.28 x 10-2 5.94 x 10-3

With a value of v = 2.53 one gets

Подпись: (3.82)ki= VP = 1.17

Ea

Подпись: Lc image173 Подпись: 8.6 cm Подпись: (3.83)

and

image176 Подпись: (3.84)

and

The mass of the fuel is around 7.2 metric tons.