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dC 8 =
dt ¼ l
X 1 Y
ð
Þ=
Y
;
ʼ
where
c growth rate of respective microbial population with biomass X,
Y is biomass yield per unit of substrate consumed. Microbial biomass X is formed
with the following law:
is speci
dX
=
dt ¼ l
X
;
S þ K ð Þ , S is catabolic substrate concentration, R is the
function of physiological state, K S is saturation constant, numerically equal to that
substrate concentration at which microbial speci
l ¼ l max SR
=
where
c growth rate attains the half of
maximal value ( ʼ = 0.5 ʼ max ).
Natural wetlands and rice paddies deliver to the atmosphere more than 30 % of
global CH 4 emission. Flux C 3 can be parameterized by the following equation:
C 3 ¼ H r f 1 T ð f 2 ðÞ f 3 p ð f 4 r p ;
where H r
is heterotrophic respiration, T s
is soil
temperature, h is water table
position, r p is redox potential, functions fi i (i=1
4) parameterized the CH 4 emission
rates. Fluxes C 1 and C 2 that characterize major atmospheric CH 4 sinks are mainly
parameterized by its reaction with hydroxyl (OH) radical. These
-
uxes depend on
the OH levels and reaction rate. Under this, it is known that increase in methane
leads to positive feedback (Xu et al. 2007; Krapivin and Varotsos 2008).
The scheme of Fig. 6.27 is realized by global carbon cycle model (GCCM)
blocks of which are characterized in Fig. 6.29 and Table 6.25 . Many of the GCCM
blocks have form of coupled set of time-dependent advection, diffusion, and
reaction equations. Set of theoretical and empirical models for the carbon
fl
fl
fluxes of
Fig. 6.27 are realized by speci
c blocks, represented in Fig. 1.30 . (Kondratyev et al.
2003b; Degermendzhi et al. 2009; Williams and Follows 2011).
Fig. 6.29 Structure of the
GCCM. Notation is given in
Table 6.25
 
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