Geoscience Reference
In-Depth Information
h
i
1
=
4
1
=
4
1
a
o
Þ
1
Þ
1
T
s
¼ E
o
ð
1
aÞ=r
E
o
1
þ Da
ð
1
a
o
þ
E
a
=
ð
ð
1
:
12
Þ
E
o
≪
1, expand the function of the right-hand part of
the Eq. (
1.12
) into Taylor series by degrees
Assuming
ʔʱ ≪
1 and E
a
=
E
o
and write
ʔʱ
and E
a
=
first terms of
the series:
n
o
1
=
4
Þ
1
1
þ
E
a
=
T
s
E
o
1
a
o
E
o
ð
Þ=r
1
þ
0
:
25
Da
ð
1
a
o
ð
1
:
13
Þ
It follows from Eq. (
1.13
) that the temperature at not so strong anthropogenic
impacts is the sum of the terms describing the bonds in the system
“
surface-
atmosphere
, without account of anthropogenic factors, and the terms T
1
and T
2
,
representing the contribution of heat and aerosols emissions, respectively:
”
1
=
4
E
a
=
Þ
1
E
o
1
a
o
E
o
96
E
o
;
T
1
¼ 0
:
25 1
a
o
ð
ð
Þ=r
:
046E
a
=
1
=
4
Þ
1
E
o
1
a
o
T
2
¼ 0
:
25 1
a
o
ð
ð
Þ=r
Da
96
:
046
Da:
Note that the contribution of T
1
in present conditions is very small. Assuming
that E
a
=4
10
−
5
cal/cm
2
min and, hence, E
a
=
E
o
¼ 8
21
10
4
,
×
:
then
T
1
= 0.0079
C. Thus the direct impact of the global energy on the atmospheric
average temperature is now negligible. It follows from the expression for T
1
that to
raise the atmospheric temperature by 0.5
°
°
C due to thermal emissions, the condition
E
a
=
E
o
¼ 0
:
0052 should be satis
ed, and this means an increase of anthropogenic
heat
fluxes to the environment by a factor of 63.4. This is equivalent to energy
release at the annual burning of 570
fl
10
9
t of conventional fuel.
If we assume that the energy production is proportional to the size of population,
then T
1
¼ 96
×
E
o
, where G is the population density, men/km
2
;
˃
S
is
the land area, km
2
; k
TG
is the per capita amount of produced energy, cal/min.
If we neglect the impact of aerosol on the atmospheric thermal regime, then the
direct radiation E, its change dE and the change of atmospheric turbidity dB will be
related as: dE/E =
:
046k
TG
G
r
S
=
k
B
dB, where k
B
= 0.1154 km
2
/t is the proportion coef
cient, B is
the amount of anthropogenic aerosols, t/km
2
. After integrating this equation, we
obtain: E ¼ E
o
ð
1
a
o
Þ
exp
k
B
B
−
nition
of albedo, E ¼ E
o
ð
1
aÞ
¼E
o
ð
1
a
o
þ DaÞ
. Equating these expressions for E,
we obtain
ʔʱ
=
−
(1
− ʱ
o
)[1
−
exp(
−
k
B
B)]. Hence, a temperature change due to
pollution of the atmosphere by anthropogenic aerosols is equal to:
ð
Þ
. On the other hand, according to the de
1
=
4
1
exp
k
B
B
25 E
o
1
a
o
T
2
¼
0
:
ð
Þ=r
½
ð
Þ
¼
62
:
43 1
exp
k
B
B
½
ð
Þ
:
Since the average emission of anthropogenic aerosols is estimated by many
authors at 300
10
6
t/year, and the average period of the aerosols residence in the
atmosphere is estimated at 3 weeks, 17.262
×
10
6
tons of particles, on the average,
×
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