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

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Solution<br />

Dn,p<br />

=<br />

The dose rate due <strong>to</strong> the n, p reaction is calculated from Eq. (6.108).<br />

RADIATION DOSIMETRY 269<br />

4 neutrons<br />

10<br />

cm2 a<strong>to</strong>ms<br />

cm2<br />

× 1.49 × 1024 × 1.75 × 10−24<br />

/s kg a<strong>to</strong>m × 0.63 MeV × 1.6 × 10−13 J<br />

MeV<br />

1 J/kg<br />

−9 Gy<br />

= 2.628 × 10<br />

s ,<br />

or, the close rate per hour = 2.628 × 10 −9 Gy/s × 3.6 × 10 3 s/h<br />

˙Dn,p = 9.5 μGy<br />

h<br />

<br />

0.95 mrad<br />

<br />

.<br />

h<br />

The au<strong>to</strong>-integral gamma-ray dose rate is calculated with Eq. (6.82). The gammaray<br />

“activity,” from Eq. (6.109) is<br />

4 neutrons<br />

A = 10<br />

cm2 a<strong>to</strong>ms<br />

cm2<br />

× 5.98 × 1025 × 3.3 × 10−25<br />

/s kg a<strong>to</strong>m<br />

5 ′′<br />

Bq′′<br />

= 1.973 × 10<br />

kg .<br />

The dose rate from this uniformly distributed gamma ray emitter is calculated from<br />

Eq. (6.82):<br />

˙Dγ = AS<br />

m<br />

× ϕ × Gy<br />

s .<br />

The absorbed fraction, ϕ, for the 2.23-MeV gamma ray is found, by interpolating<br />

in Table 6-8 between the 2.000 and 4.000 MeV values, <strong>to</strong> be 0.278, and , the dose<br />

rate in an infinitely large mass whose specific activity is 1 Bq<br />

, is calculated from<br />

kg<br />

Eq. (6.81):<br />

= 1.6 × 10 −13 × 2.23 MeV<br />

γ<br />

Gy<br />

= 3.57 × 10−13 Gy/s<br />

Bq/kg .<br />

The au<strong>to</strong>-integral gamma-ray dose rate, therefore, is<br />

or<br />

˙Dγ<br />

5 Bq<br />

Gy/s<br />

= 1.973 × 10 × 0.278 × 3.57 × 10−13<br />

kg Bq/kg<br />

−8 Gy<br />

= 1.96 × 10<br />

s<br />

71 μ Gy<br />

h<br />

<br />

7.1 mrad<br />

<br />

.<br />

h<br />

(1.96 × 10 −6 rad/s)

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