Geoscience Reference
In-Depth Information
For the
first factor, a linear model T a =
ʺ
t +
ʔ
T a can be taken resulting with
ʔ
R =
½
ʺ 1 (
T a ) 2 +
T a t. It is plausible that the second factor is somewhere between zero and the
shift in the zero upcrossing time of air temperature, 0
ʔ
ʔ
t m ≤ ʺ 1
≤ ʔ
ʔ
T a . Then we have
s
l c ½ q L ð h 0 þ Dh Þ k 1 ð R þ DR Þ
3
t ð t m þ Dt m Þ ¼
ð
8
:
13
Þ
ʔ
t m is the strongest, since ice thickness change and positive degree-days
change appear under the cube root. The cube root was obtained from a simple model for
the increase of solar radiation and decrease of albedo during the melting period, and it
could be changed into a general power law
The role of
ʽ
,0<
ʽ
<1.
8.4.3 Numerical Modelling
A numerical model can be used to produce projections for the future ice seasons. If air
temperature change only is considered, the
first order analytic model is usually quite good,
but to examine the in
fl
uence of snow accumulation and qualitative changes, numerical
models provide a more
ranta 2009a; Yang et al. 2012).
An example is shown in Fig. 8.15 for southern Finland, where model simulations for a
firm basis (e.g., Lepp
ä
'
normal
'
winter are compared with those for winters where the mean air temperatures are
1 and 5
°
C higher or lower than the present (1980
2010) baseline. In the numerical model,
-
the lake freezes during the
first strong cold spell. The observed, present average maximum
annual ice thickness of 45 cm decreases by 5 cm for the
rst 1
°
C warming, 20 cm for the
next 3
°
C warming, and 10 cm for the
final 2
°
C increase. The ice break-up date also shifts
Fig. 8.15
Model sensitivity to
the air temperature. The black
solid line is the reference of
present climate. The grey solid
lines show the modelled ice
thickness based on air
temperature decrease by 5 and
1 ° C, and the grey dashed line
show modelled ice thickness
based on air temperature
increase by 5 and 1 ° C (Yang
et al. 2012)
0.0
-0.2
-0.4
-0.6
-0.8
-1.0
Oct
Nov
Dec
Jan
Feb
Mar
Apr
May
Jun
Time of year
 
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