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Regional Basic Professional Training Course in Korea

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❙ 345 ❙<br />

5. SITING CONSIDERATIONS<br />

(σx = σy = σh = (Aht) kh and σz = (Azt) kz ). There were only two stability categories: neutral<br />

and weak diffusion. The limit between these two classes was the vertical temperature<br />

gradient. Parameters2 used <strong>in</strong> the formulation of standard deviations were adjusted on the<br />

extremely numerous distributions observed of pollutants <strong>in</strong> suspension result<strong>in</strong>g from<br />

short‐duration emissions [5.6].<br />

In the French‐German model [5.7], standard deviations no longer come from<br />

experimental data, but result from considerations of the atmospheric turbulence spectra<br />

and their <strong>in</strong>fluence on the diffusion process. There are three stability categories, the limit<br />

between the classes is a function of either vertical temperature gradient and w<strong>in</strong>d speed or<br />

both fluctuations of w<strong>in</strong>d direction and w<strong>in</strong>d speed.<br />

This new set of standard deviations corrects problems that occurred when us<strong>in</strong>g Doury's<br />

(overestimation of concentrations for high w<strong>in</strong>d speeds) or Pasquill's (overestimation of<br />

concentrations for low w<strong>in</strong>d speeds) standard deviations.<br />

Under stable meteorological conditions, for a puff, whose <strong>in</strong>itial dimensions that are<br />

small relative to its dimensions at the <strong>in</strong>stant of observation, the concentration per unit<br />

volume (along x, y and z) at <strong>in</strong>stant t can be written as:<br />

AV(<br />

x,<br />

y,<br />

z,<br />

t)<br />

⎡<br />

2<br />

2⎤<br />

2<br />

2<br />

QE 1 ( x−x<br />

⎡ ⎛ ⎞ ⎛ + ⎞⎤<br />

oo−ut)<br />

( y−yo)<br />

1(<br />

z−zo)<br />

1(<br />

z zo)<br />

exp−<br />

⎢ + ⎥•⎢exp<br />

⎜<br />

⎜−<br />

⎟<br />

⎟+<br />

exp ⎜<br />

⎜−<br />

⎟<br />

3<br />

2<br />

2<br />

2<br />

⎥<br />

2 ( 2π)<br />

σ σ σ 2⎢⎣<br />

σx<br />

σy<br />

⎥⎦<br />

⎣ ⎝ 2 σz<br />

⎠ ⎝ 2 σz<br />

⎠⎦<br />

= 2<br />

x y z<br />

<strong>in</strong> which AV = activity per unit volume <strong>in</strong> air<br />

Q = quantity of activity released<br />

E = specific law for <strong>in</strong>crease or decrease of activity<br />

e.g. radioactive decay or depletion by dry or wet deposition

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