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Water retention rate ( R wat )
Lake water
M W
Inflow ( Q . C in )
Outflow ( Q . C = M . R wat )
Sedimentation
rate ( R sed )
Internal
loading
( M S . R res )
Sedimentation
( M W . R sed )
Internal loading
rate ( R res )
M S
Lake sediments
Particulate fraction ( PF )
V . d C /d t
Q . C in
Q . C
M W . R sed . PF
M S . R res
=
+
d C /d t
=
change in concentration in lake water
C
=
M W / V ; V
=
lake volume
Fig. 4.12 The basic mass-balance equation for a lake
with internal loading.
T w
=
V / Q ; Q
=
water discharge
C in
=
tributary concentration
conditions, because the sediment concentrations
of these substances mainly reflect sediment redox-
conditions and low redox values may appear
in sediments of most lakes. On the other hand,
sediment Ca concentrations more closely reflect
typical lake properties on a scale from low to
high calcareous conditions.
0
=
Q · C in
Q · C
M W · R sed · PF
+
M S · R res
(in)
(out)(sedimentation)(resuspension)
where V is the lake volume (usually m 3 or km 3 ),
C is the concentration of the substance in the
lake water (units usually g L −1 or kg m −3 ; C
is the M W / V ), C in is the concentration of the
substance in the tributary ( C in has the same
dimension as C ), Q is the tributary water dis-
charge to the lake (usually expressed as m 3 yr −1
or m 3 month −1 ), R sed is the sedimentation rate
of a given substance in the lake (like all rates,
R sed has the dimension 1/time and its unit is usu-
ally 1/day, 1/month or 1/year), M W is the mass
(
4.2.4 Mass-balance modelling for lakes
The basic aim of mass-balance calculations is
to quantify fluxes so that large and important
fluxes may be identified and differentiated from
small fluxes. The aim of this section, however, is
not to give a full mathematical account of all the
processes shown in Fig. 4.2, only to give a brief
introduction to mass-balance modelling and to
illustrate some basic concepts with a focus on
sedimentation in lakes.
A simple mass-balance model for a lake is
depicted in Fig. 4.12. A typical mass-balance
model envisions the lake as a 'tank reactor' in
the sense that the lake mixes completely during
an interval of time d t . The flow of suspended
particulate matter (or a given contaminant) to
and from such a lake, and net sedimentation may
be described by the following equation (this is
the steady-state solution to the equation given
in Fig. 4.12):
amount) of the substance in the lake water
(units often in g or kg), PF is the particulate
fraction (dimensionless), the only fraction that
can settle out in lakes due to the influence of
gravitation, M S
=
amount) of the
substance on the lake bed (units in g or kg), R res
is the internal loading rate, or resuspension rate
(units usually in 1/day, 1/month or 1/year). The
steady-state assumption means that a change in
lake concentration (d C ) of the given substance
per unit of time (d t ; usually in g L −1 month −1 or
kg m −3 yr −1 ) is set to zero.
The lake water retention time ( T , in days,
months or years) is a fundamental concept in
lake studies. It is defined as the ratio between the
is the mass (
=
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