Lesson 6 Tutorial

Q: The effective dose rate to a person standing on a surface contaminated with gamma emitters is measured as 2 μSv/h at a height of 1 m above the ground. Using the extended-area-source formula introduced in Section 6.14 (Worked Example 3),

D˙(h)=ΓCln[A×W+h2h2]\dot{D}(h) = \Gamma C \cdot \ln\left[\frac{A \times W + h^2}{h^2}\right]

where Γ\Gamma is the specific gamma constant, CC is the activity per unit area (Bq/m2^2), A=10A = 10 m is the effective length of the contaminated area, W=5W = 5 m is the width, and hh is the measurement height, show that the dose rate at a height of 0.25 m (e.g. the head of a small dog or the legs of a child) is greater than 2 μSv/h but less than 7.5 μSv/h.

Answer:

Step 1: Find ΓC\Gamma C using the measurement at h=1h = 1 m.

2=ΓCln[10×5+1212]=ΓCln(51)=ΓC×3.9322 = \Gamma C \cdot \ln\left[\frac{10 \times 5 + 1^2}{1^2}\right] = \Gamma C \cdot \ln(51) = \Gamma C \times 3.932

ΓC=23.932=0.509 μSv/h\Gamma C = \frac{2}{3.932} = 0.509 \ \mu\text{Sv/h}

Step 2: Calculate the dose rate at h=0.25h = 0.25 m.

D˙(0.25)=0.509ln[10×5+0.2520.252]=0.509ln[50.06250.0625]=0.509ln(801.0)\dot{D}(0.25) = 0.509 \cdot \ln\left[\frac{10 \times 5 + 0.25^2}{0.25^2}\right] = 0.509 \cdot \ln\left[\frac{50.0625}{0.0625}\right] = 0.509 \cdot \ln(801.0)

D˙(0.25)=0.509×6.686=3.40 μSv/h\dot{D}(0.25) = 0.509 \times 6.686 = 3.40 \ \mu\text{Sv/h}

Result: 2.0 μSv/h < 3.4 μSv/h < 7.5 μSv/h — QED.

Physical interpretation: Reducing the height by a factor of 4 (1.0 m → 0.25 m) only increases the dose rate by a factor of ~1.7, not the factor of 16 that an inverse-square (point-source) law would predict. This is because the contamination is an extended planar source, not a point source: the dose rate depends logarithmically on height, not quadratically. The same formula applied in Section 6.14 to a contaminated floor inside a decommissioned facility also covers the analogous yellowcake-road case at the mining end of the cycle.