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

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RADIATION SAFETY GUIDES 361<br />

is 1 g/cm 3 . Since the activity of a radioactive particle is directly proportional <strong>to</strong><br />

its mass, we can describe the mean size of a radioactive aerosol by its activity mean<br />

aerodynamic diameter (AMAD) size. In radiation safety standards, particle sizes refer<br />

<strong>to</strong> the sizes of those particles whose aerodynamic behavior is equivalent <strong>to</strong> that of<br />

unit density particles.<br />

Thermodynamic Properties<br />

When particle sizes approach the size of air molecules, the random collisions with<br />

the air molecules impart enough energy <strong>to</strong> the aerosol particles <strong>to</strong> influence the<br />

motion of the aerosol particles. The resulting random motion of the air molecules<br />

is known as Brownian motion, and is the basis for the diffusion process. (The physics<br />

of Brownian motion was explained by Albert Einstein in the second of his four<br />

revolutionary papers during the annus mirabilis, the “miracle year” of 1905.) The<br />

mean thermal displacement during a time interval t, of particles suspended in a<br />

gaseous medium is independent of the particle density, and is given by<br />

s =<br />

<br />

RT Ct<br />

× ; (8.19)<br />

N 3πηd<br />

s is in cm when<br />

R = gas constant = 8.3 × 10 7 ergs/mol/K<br />

T = temperature, K<br />

N = Avogadro’s number = 6.02 × 10 23 molecules/mol<br />

t = time interval, seconds<br />

d = particle size, cm<br />

η = viscosity of the medium = 185 × 10 −6 g/cm/s for standard air<br />

C = Cunningham slip correction fac<strong>to</strong>r. This fac<strong>to</strong>r corrects for the fact that<br />

the air is not a continuous medium, but consists of discrete molecules.<br />

A particle may thus “slip” between molecules. This slip fac<strong>to</strong>r becomes<br />

increasingly important as the particle size approaches the mean free path<br />

of the gas molecules, and<br />

C = 1 + 1.7 λ/d, where λ = mean free path of the gas molecules = 6.7 × 10 −6<br />

cm for air at 25 ◦ C.<br />

Diffusion becomes increasingly important as a particle transport mechanism as the<br />

particle size decreases below 1 μm. The Table 8-6 shows the displacement during<br />

1 second by gravitational settling and by diffusion of a unit density particle of 3<br />

different sizes.<br />

TABLE 8-6. Effect of Particle Size on Displacement Distance by Diffusion and by<br />

Gravitational Settling<br />

PARTICLE SIZE DIFFUSION GRAVITATIONAL SETTLING<br />

(μm) (μm) (μm)<br />

0.1 22.4 0.6<br />

1.0 5.1 29.4<br />

10.0 1.5 2940

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