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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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TABLE 12-3. Delayed Neutrons from the Fission of 235 U<br />

CRITICALITY 653<br />

YIELD, MEAN GENERATION<br />

GROUP percent TIME, seconds YIELD × MEAN TIME<br />

i ni Ti ni × Ti<br />

1 0.0267 0.33 0.009<br />

2 0.0737 0.88 0.065<br />

3 0.2526 3.31 0.836<br />

4 0.1255 8.97 1.125<br />

5 0.1401 32.78 4.592<br />

6 0.0211<br />

<br />

ni = 0.6397<br />

80.39 1.688<br />

<br />

ni Ti = 8.315<br />

and the power level increase in 1 second would be<br />

n<br />

n0<br />

= e t<br />

T = e 1<br />

0.2 = 150 fold.<br />

Such rapid increases in the power level as calculated in the example above would<br />

make it extremely difficult, if not impossible, <strong>to</strong> control a reac<strong>to</strong>r. Fortunately, the<br />

calculation above is not applicable <strong>to</strong> a real reac<strong>to</strong>r because, although the mean<br />

lifetime of a single neutron from birth until absorption is about 0.001 second, the<br />

mean lifetime of a whole generation of a large number of neutrons is much greater<br />

than 0.001 second. This increased mean generation time is due <strong>to</strong> the fact that<br />

0.6407% of fission neutrons are delayed, that is, they are emitted for as long as 80.39<br />

seconds after fission. Six distinct groups of delayed neutrons are observed, each group<br />

having its own mean delay time. Table 12-3 lists these groups, <strong>to</strong>gether with their<br />

mean delay (or generation) time.<br />

The mean generation time for all the fission neutrons of a given generation is<br />

6<br />

ni Ti<br />

¯T<br />

i=0<br />

=<br />

6<br />

= 8.315 + (100.0000 − 0.6397) × 10−3<br />

= 0.084 second.<br />

100<br />

ni<br />

i=0<br />

The group i = 0 is the group of prompt neutrons, whose yield is 99.359% and whose<br />

mean generation time is 0.001 second.<br />

If k, is equal <strong>to</strong> or greater than 0.006407, the reac<strong>to</strong>r is said <strong>to</strong> be in the prompt<br />

critical condition, since the chain reaction can be sustained by the prompt neutrons<br />

alone. If k is less than 0.006407, the reac<strong>to</strong>r is in the delayed critical condition,<br />

because the delayed neutrons are essential <strong>to</strong> sustaining the chain reaction. In the<br />

delayed critical condition, the reac<strong>to</strong>r period is sufficiently long <strong>to</strong> allow the power<br />

level <strong>to</strong> be easily controlled.<br />

W Example 12.5<br />

Compute the reac<strong>to</strong>r period and the increase in power level in 1 second for the<br />

case where the mean neutron generation time is 0.084 second for excess reactivity

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