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4. STUDY AREA
The Abisko National Park is situated in northern Sweden
in the province Lappland at 6821'N/1999'E. The study
area in the sub province Torne Lappmark includes the
northern part of the Abisko National Park, part of lake
Abisko, the hills south of Abisko Ostra and the crests of
mount Njulla (1169m) and Slattatjakka (1191m). In
Scandinavia the northern limit of boreal forest is formed
by the birch. The forest limit in the study area is
determined by elevation and situated between 550m and
650m. It can be differentiated between the "subalpine
birch tree region" and the "alpine region" of alpine heaths,
meadows and tundra.
5. THE SLOPE WIND MODEL OF BREHM
Under stable conditions, the atmospheric boundary layer
shows special characteristics at slopes, and a sun driven
mecanism forces the air into a well defined movement
upwards.
Brehm (Brehm, 1986) parametrized the slope wind by
atmospheric stability, excess temperature (temperature
difference between the terrain at roughness length-height
and free atmosphere) and slope angle.
His model generates values for the geostrophic friction
coefficient c4, the heat transfer coefficient Cp and their
ratio KR Cg/Ch: which are defined by the following
equations:
^ (1)
K u* Ox /
n ah (2)
Where u* is the friction velocity, 6* the characteristic
temperature fluctuation, « Von Karman's constant, A the
excess temperature, p the coefficient between the
acceleration due to gravity and the potential temperature
of the surface g/©, and the temperature gradient of the
free atmosphere d@/dz.
BREHM generated values for c, and n in dependance of
the analog soil rosby number Ro for different slope
angles. Soil rosby number in turn is defined as follows:
- KA 3
Y Sina, zo (3)
Zo is the roughness length.
In order to calulate the analog soil rosby number for each
terrain pixel, we need the surface temperature, a vertical
temperature profile of the free atmosphere, a method to
Parametrize roughness length and a digital terrain for
slope angles and elevations.
The relations between rosby number and c, or m,
calculated by Brehm's slope wind model, are graphically
"presented in Brehm's study (Brehm, 1986) in two
graphics for different slope angles. The functional
dependance between cg / n and the rosby number for
661
any slope angle were fitted by a polynomial equation, so
that c, and n could be written as functions Cg = f(a,Ro)
and n = f(a,Ro).
6. PARAMETRIZATION OF SENSIBLE HEAT FLUX
Sensible heat flux can be written as follows:
H=-p cpus Ox (4)
where p is the air density and Cp is the specific heat of air
at constant pressure.
Replacing the parameters with de definitions of c, and n
in formula (1) and (2), equation (4) can be reformulated
in the following way:
Hzp Cp «cg (Roa) n(Ro,a) ABH (5)
The excess temperature as formulated by Brehm is the
temperature difference between the free atmosphere and
the surface defined at a level above the ground that
corresponds to roughness length.
Mannstein (Mannstein, 1991) assumes, that the radiation
temperature derived from thermal sensors of a remote
sensing devices represent the skin temperature of the
ground which is best represented at zero height.
Therefore, he adopts a formulation of Monin and
Zilitinkevich (Monin/Zilitinkevich, 1968) which expresses
the difference Ay between surface and zj-level as
follows:
Ag = -0.13 ©+ (tapas (6)
v is the kinematic viscosity of air.
Using the definitions for Cg and n, Aq can be written as:
s: : eg € AN BAT za 0.45
Ag 7 -0.13« n cg A( x ) (7)
For a given temperature difference A, between the
ground (derived by thermal sensors) and free
atmosphere, the temperature difference A between the z,
level and the atmosphere, as it will be used for the
model, can be found by itereation, so that the following
equation holds:
Ag = ^ * Aq (8)
As is the known temperature difference between satellite
temperature at n=0 and free atmosphere.
7. DETERMINATION OF THE MODEL PARAMETERS
7.1 Modelling of roughness length
Roughness length varies widly within a given land use
class. Mannstein distinguished only 3 land use types and
substituted each of them with a single value for
roughness length.
International Archives of Photogrammetry and Remote Sensing. Vol. XXXI, Part B7. Vienna 1996