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334 11 Air Dispersion
Solution
First, determine the atmosphere stability using the Pasquill stability class described
in Table 11.1. It can be determined as class C stability. Note that this is still an
approximation because we are considering the wind speed to be uniform, which
may not be not the case in reality.
Anyways, with the class C stability the corresponding air dispersion coefficients
for rural area can be calculated using the equations in Table 11.4 as follows.
0:11x 0:11 5000
r y ¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffip ¼ p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ¼ 449:1m
1 þ 0:0001x 1 þ 0:0001 5000
0:08x 0:08 5000
r z ¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffip ¼ p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ¼ 282:8m
1 þ 0:0002x 1 þ 0:0002 5000
(a) The concentration at the plume center 5 km downwind can be determined
using Eq. (11.33) with z-H = 0 and y =0
_ m
Cx; 0; HÞ ¼
ð
2pr y r z u
0:1 8 3 3
¼ ¼ 2:09 10 ðkg=m Þ¼ 20:9ðlg=m Þ
2p 449:1 282:8 6
(b) The concentration on the ground right below the plume center at x = 5000 m
downwind is calculated using Eq. (11.33) with z =0, y = 0 and H = 120:
_ m H 2
ð
Cx; y; zÞ ¼ exp
2pr y r z u 2r 2 z
" #
2
1 120 3
¼20:9 exp ¼ 20:9 0:914 ¼ 19:1ðlg=m Þ
2 282:8
(c) The concentration at the ground right below the plume center at 2,000–6,000 m
downwind is calculated using Eq. (11.33) with z =0, y = 0 and H = 120:
_ m H 2
Cx; y; zÞ ¼ exp
ð
2pr y r z u 2r 2 z
where
0:11x
r y ¼ p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
1 þ 0:0001x
0:08x
r z ¼ p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
1 þ 0:0002x