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

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W = workload, Gy/wk,<br />

T = occupancy fac<strong>to</strong>r, and<br />

F = actual cross-sectional area of the beam at 1 meter, cm 2 .<br />

EXTERNAL RADIATION SAFETY 563<br />

The barrier transmission fac<strong>to</strong>r for leakage radiation is given in NCRP 147 as<br />

BL = 1000 × P × d2 L<br />

.<br />

W × T<br />

The fac<strong>to</strong>r of 1000 accounts for the fact that leakage radiation at a distance of 1 m<br />

from the target may not exceed 0.1% of the workload.<br />

The scattered radiation barrier transmission is found by substituting the appropriate<br />

values in<strong>to</strong> Eq. (10.33). The value of α for 90 ◦ scatter is found in Table 10-8.<br />

Bps = P<br />

αWT × d2 sca × d2 400<br />

sec ×<br />

F<br />

−6 Sv<br />

20 × 10<br />

Bps =<br />

wk<br />

4.26 × 10−4 × 800 Gy<br />

× (1 m)<br />

× 1<br />

wk 2 × (6.3m) 2 400 cm2<br />

×<br />

225 cm2 = 4.1 × 10−3 .<br />

The number of TVLs <strong>to</strong> attain this degree of attenuation is<br />

n = log 1<br />

Bps<br />

1<br />

= log<br />

= 2.4.<br />

−3<br />

4.1 × 10<br />

The required maximum transmission of leakage radiation is calculated by substituting<br />

the appropriate values in Eq. (10.33):<br />

BL = 1000 × P × d2 L<br />

W × T<br />

=<br />

−6 Gy<br />

1000 × 20 × 10 × (6.3m)2<br />

wk<br />

800 Gy<br />

= 9.9 × 10<br />

wk<br />

−4 .<br />

The number <strong>to</strong> TVLs required <strong>to</strong> reach 9.9 × 10 −4 is<br />

n = log 1<br />

BL<br />

1<br />

= log<br />

= 3. −4<br />

9.9 × 10<br />

According <strong>to</strong> the recommended design practice, when the two calculated barrier<br />

thicknesses are close <strong>to</strong>gether, as in this case, we add 1 HVL <strong>to</strong> the thicker barrier.<br />

If the two barrier thicknesses differ by a TVL or more, we simply use the thicker<br />

barrier. In this example, the barrier thickness for the leakage radiation is not<br />

much greater than that for the scattered radiation. We therefore add 1 HVL <strong>to</strong> the<br />

thicker barrier. In Table 10-9, we find TLV1 and the TLVe for 6-MV X-rays <strong>to</strong> be 34and<br />

29-cm concrete respectively. Since 3.3 HVL = 1 TVL, the required barrier<br />

thickness is<br />

tsecondary = 34 cm + (3 − 1) × 29 cm +<br />

29 cm<br />

3.3<br />

= 101 cm.

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