Geoscience Reference
In-Depth Information
The value of t o is identi
ed with the year 1980, when the GHG concentrations
were known. To calculate
D
T CO 2 , one can use a more accurate formula by Krapivin
(1993).
Among simple formulas of calculations of the latitudinal distribution of average
temperature over the globe one can indicate the schemes proposed by Sergin
(1974):
T ðuÞ ¼T g þ cð sin 2
u T sin 2
uÞ;
ð 1
:
10 Þ
where
ˆ
is the latitude in radians,
ʳ
is the pole-equator temperature difference,
ˆ T is
the latitude at which T(
ˆ
)=T g . The latitudinal temperature variations can be
described:
T a ðu;
t Þ ¼T e 2
u
ð
T e T N
Þ=p
for the Northern hemisphere
;
T a ðu;
t Þ ¼T e 2
u
ð
T e T S
Þ=p
for the Southern hemisphere
;
where
(
=
T N ; min þ 2tT N ; max T N ; min
t D ;
t 2 0
½
;
0
;
5t D
;
=
T N ¼
T N ; min þ 2 t D t
ð
Þ T N ; max T N ; min
t D ;
t 2
ð
0
;
5t D ;
t D ;
(
T S ; max þ 2tT S ; min T S ; max
=
t D ;
t 2 0
½
;
0
;
5t D
;
= t D ;
T S ¼
T S ; max þ 2 t D t
ð
Þ T S ; min T S ; max
t 2
ð
0
;
5t D ; t D ;
T TN,min (T TS,min ) and T N,max (T S,max ) are minimum and maximum temperatures at the
North (South) Pole, respectively,
°
C; t ʔ
is the duration of the year in units of
measurements
ʔ
, T e is the equatorial temperature of the atmosphere,
°
C. Many
authors use the estimates T TN,min =
30
°
C, T N,max =0
°
C, T TS,min =
50
°
C, T S,
max =
C.
Of course, these zonally averaged temperatures scatter widely, which leads to
considerable errors. To more accurate re
10
°
C, T e =28
°
fl
ect the role of various factors in changes
of the basic climatic parameter
temperature, it is necessary to calculate the con-
tribution of each factor separately. This can be done with an assumed additivity of
the role of feedbacks:
ʔ
T a,nal =
ʔ
T a +
ʔ
T ΔTa,feedback. . In some models authors
introduce the feedback coef
cient
ʲ
:
ʔ
T a,nal =
ʲ · ʔ
T a . The
ʲ
parameter is
expressed through the ampli
cation index g:
ʲ
= 1/(1
g). The value of the g index
is equivalent
, which on a global scale is a function of T a . This
dependence can be roughly approximated by the formula
to albedo
ʱ
8
<
a ice
for T a T ice ;
T a Þ ¼
a free
for T a T free ;
:
a free þ b ð T free T Þ
for T ice \
T a \
T free
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