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
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 H 0 \ H Þ[ð H 1 \
H Þ and nondecreasing at 8 h 2 H 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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