Geoscience Reference
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2
, the function p(h) is the product of the nondecreasing
and nonincreasing functions. Hence, in
1
[ X
In the set
X
¼
X
ʩ
−
p(h) is either nondecreasing, or non-
increasing or has a maximum. Since for
8
h
2 X
F
ðÞ=
N
ðÞ
[
m
, then p(h)willbe
the nonincreasing function at
8
h
2
H
0
¼
f
h
:
h
h
0
g
, where
Z
h
0
p
ð
0
Þ
¼
w
ð
y
Þ
exp
½
uð
y
Þ
dy
0
The multitude of values h
≥
0, for which the following condition is valid, are
denoted by H
1
:
Z
w
ðÞ
exp
1
exp
w
ðÞ
F
ðÞ
vN
ðÞ
½
u
ðÞþ
½
u
ðÞ
dy
p
ðÞ
[
.
The obtained results are formulated as the following theorem.
Theorem The function p(h) is nonincreasing at
8
h
2
H
þ
[ð
H
0
\
H
Þ[ð
H
1
\
H
Þ
and nondecreasing at
8
h
2
H
\ð
E
n
H
0
Þ\ð
E
n
H
1
Þ
, where E ={h: h
Then p(h) will be the nonincreasing function at
8
h
2
H
1
\ X
≥
0}.
In a more general case
@
p
=@
can be presented in the form of the sum:
@
p
=@
z ¼
ð@
p
=@
z
Þ
EB
þð@
p
=@
z
Þ
O
þð@
p
=@
z
Þ
s
þð@
p
=@
z
Þ
M
þð@
p
=@
z
Þ
Z
þð@
=@
z
Þ
T
;
ð
4
:
44
Þ
p
where each of the terms on the right-hand side re
ects a change of the phyto-
plankton biomass due to changes in illumination and concentration of nutrient
elements (EB), sedimentation (O), temperature changes (
fl
), mortality (M), con-
sumption by zooplankton (Z) and turbulent mixing (T). According to Eq. (
4.43
), it
can be supposed that
˄
Þ
¼Af
1
ðÞ
f
2
ðÞ
½1
10
c
p
ð@
p
=@
z
Þ
EB
Ft
ð
;
p
;
z
:
At
ʳ
p << 1 we obtain
p
1
ð@
p
=@
z
Þ
EB
Af
1
ðÞ
f
2
ðÞ:
With an increasing depth in other stationary conditions the water temperature is
known to monotonically decrease, dropping sharply in the layer of the thermocline
(i.e., (
@
=@
z)
˄
≤
@
=@
z)
M
has the form of the sectionally
continuous non-positive function. However, due to the physical processes of
mixing a situation can appear when this monotonicity gets broken.
The values of the constituent (
p
0). The similar term (
p
@
p
=@
z)
Z
depend on the distribution of N(z).
The term (
@
p
=@
z)
T
is totally determined by the hydrological conditions through the
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