The three-zone reactor

Let 72 and 73 be the attenuation factors in zones 2 and 3. In zone 3 the flux should remain finite at infinity. It must have the form

u3(r) = a3 e-73r. (10.5)

Подпись: We define image479 Подпись: (10.6) (10.7)

At radius R2, one writes the continuity of neutron flux and current, and obtains a relation between the coefficients a2 and b2 which appear in

Подпись: c Подпись: 72R2 + 1 —^ _ D2(72R2 + 1)— D3(1 + 73R2) 72R2 — 1 +< D2(72R2 — 1)+D3(1 + 73R2) Подпись: (10.8)

and

b2 = a2C є-1’*2*2

Подпись: Then
Подпись: (10.9)
Подпись: and

u2(r) = a2 e-‘2r(1 +C e2’l(r-Rl)). (10.10)

Note that, as expected, b2 cancels out for large values of R2 and, also, if the properties of medium 3 are the same as those of medium 2.

The value of a2 is obtained from the value of the neutron current at

(72 +(!/*!))

R1

Подпись: J R) Подпись: N0 4^R2 image489 Подпись: c '2R1 1 e2'2(R1 -Rfl^ . 72R1 + 1 J (10.11)

r = Rp.

Подпись: V Подпись: c 72R1 - 1 72R1 + 1 Подпись: (10.12)

Defining

Подпись: U2(r) Подпись: N0e-72(r-R1)(1 +C e-272(R2-r)) 4WD2(1 + 72R1)(1 -D e-272(R2-R1))' Подпись: (10.13)

one obtains