Agriculture Reference
In-Depth Information
h
H
a
()
()
2
u
z
dz
=
u
z
dz
.
(27)
h
h
a
If we solve these integrals, keeping in mind that the functional form of u ( z ) is given by
Eq. (19), we get
1
h
1
+
2
exp
β
1
4
4
H
h a
=
H
1
+
ln
.
(28)
β
3
The temperature inside the canopy air space, T a , is determined diagnostically using Eq.
(12). In that formula the three aerodynamic resistances, r a , r b , and r d , are calculated as
follows:
1
2
kH
1
h
1
z
d
a
r
r
=
exp
β
1
1
+
ln
(29)
a
H
d
u
2
H
k
H
d
σβ
ln
*
z
0
1
β
C
P
k
s
s
r
=
(30)
b
u
H
d
1
h
*
4
H
L
ln
1
exp
β
1
a
d
z
4
H
o
1
2
kH
1
h
1
h
a
r
=
exp
β
1
exp
β
1
1
d
H
d
u
2
H
2
H
σβ
ln
*
z
0
1
h
exp
β
1
2
H
h
2
+
ln
(31)
H
d
z
k
ln
g
z
o
The values for the leaf shelter factor, P s , and transfer coefficient, C s , used in the
simulation are listed in Mihailovic and Kallos (1997) [22]. The effect of atmospheric
nonneutrality in Eqs. (29)-(31) (i.e., their dependence on T a and T r ) is included in u * and
accordingly in other calculations. In Eqs. (29)-(31) is supposed a logarithmic wind profile
above a canopy.
In a sparse tall grass canopy (one in which the plant spacing is the order of the canopy
height or larger), K s is strongly affected by processes in the environmental space, including
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