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where:
=
P
¼
y
2
2
V
2
y
3
2
Log
y
2
=
y
3
2
J
Log
y
2
=
2
þ
V
2
Log 1
þ
4
L
α
21
þ
=
y
3
2
V
3
y
3
2
Log
y
4
=
y
3
2
þð
V
3
þ
L
α
V
2
Þ
Log 1
þ
4
21
þ
L
0
V
3
y
4
2
þ
ð
V
4
þ
Þ
Log 1
þ
=
4
and
H
¼
V
2
y
3
2
Log
y
2
=
y
3
2
L
'
V
3
y
4
2
Log
y
3
=
y
4
2
V
3
y
3
2
Log
y
4
=
L
α
41
ð
þ
Þþ
21
ð
þ
Þ
y
3
2
21
ð Þ:
In this case, parameters appearing only in
P
*, like
V
4
, are modulating the
localization of the fixed point; hence, the values of the stationary concentrations
of the glycolytic metabolites [cf. Demongeot et al. (
2007a
,
2007b
) and Glade et al.
(
2007
) for a more general approach of the potential-Hamiltonian decomposition].
Let us suppose now that we measure the outflows
J
1
and
J
2
(cf. Fig.
4.12
). Then
from the system (S1) we can calculate the sharing parameter
þ
(which regulates the
pentose pathway and the low glycolysis dispatching) from the steady-state
equations equalizing the in- and outflows at each step. By denoting the stationary
state
x
*
α
{
x
i
*}
i ¼
1,4
, we have:
V
1
x
1
n
¼
x
1
n
V
2
x
2
=ð
x
2
Þ
V
2
x
3
=ð
x
3
Þ¼
=ð
1
þ
Þ¼
J
;
1
þ
L
α
1
þ
J
V
2
x
2
=ð
x
2
Þ¼
V
3
x
3
=ð
x
3
Þ
ð
1
αÞ
1
þ
J
1
;
1
þ
L
0
V
3
Þ=
¼
J
2
ð
V
4
þ
V
4
Hence, we can calculate
α
by using the following formula:
2
J
2
LV
2
ð
L
0
V
3
Þþα
L
0
V
3
Þ
α
V
4
þ
ð
JV
4
J
2
LV
2
ð
V
4
þ
Þ þ
J
1
V
4
J
2
K
0
¼
0
;
¼
0or
α
αð
1
K
Þþ
where we have denoted:
L
0
V
3
Þ
and
K
0
¼ð
L
0
V
3
Þ:
K
¼
JV
4
=
J
2
LV
2
ð
V
4
þ
J
1
V
4
J
Þ=
J
2
LV
2
ð
V
4
þ
When the flux of the
k
th step in a metabolic network has reached its stable
stationary value
Φ
k
, then the notion of control strength
C
ki
exerted by the metabolite
x
i
on this flux
Φ
k
is defined by (Kaczer and Burns
1973
; Wolf and Heinrich
2000
):
C
ki
¼ @
Log
ΔΦ
k
=@
Log
Δ
x
i
and we have:
8
k
¼
1
;
n
; Σ
i¼
1
;n
C
ki
¼
1
:
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