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Computational Biology Programme, Scottish Crop Research Institute, Dundee, United Kingdom
Correspondence: Address reprint requests to Dr. J. Liu, Computational Biology Programme, Scottish Crop Research Institute, Dundee DD2 5DA, UK. Tel.: 44-0-1382-562426; E-mail: jliu{at}scri.sari.ac.uk.
| ABSTRACT |
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| INTRODUCTION |
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![]() | (1) |
As discussed by Segre (2004)
, a metabolic network can be described by its hardware and software. The hardware is represented by a static reaction network, and the software is the underlying regulatory strategies. In the context of constraint-based analysis, the hardware can define matrix S and vector J. If Eq. 1 is assumed to be valid, constraint-based analysis may use it to analyze integrated functions of the network. No kinetic information is further required (Klamt and Stelling, 2003
; Price et al., 2003
). However, the software of the network has some noticeable features. Enzymatic reactions are highly nonlinear in character as a consequence of the dependence of reaction rates on substrate concentrations and regulations. Moreover, enzymes can be saturated by their substrates, and consequently, the reaction rates are limited by maximal reaction rates (Palsson, 2000
; Famili et al., 2003
). In relatively simple networks with those features, it has been shown that establishment of a stable state requires specific constraints on kinetic parameters, particularly maximal reaction rates (Liu, 1999a
,b
, 2001
). To obtain a stable steady state based on the parameters in literature, many of the parameters need to be adjusted (Aon and Cortassa, 2002
; Rohwer and Botha, 2001
; Teusink et al., 2000
). Although many of the kinetic parameters may not be readily obtained, some of them can be derived from measurable quantities. For example, maximal reaction rates are directly related to concentrations of enzymes that can be measurable at proteomic level. In constraint-based analysis, maximal reaction rates were referred to as the capacity constraints (Palsson, 2000
; Famili et al., 2003
). Moreover, investigation of non-isolated Michaelis-Menten-type reaction suggests that the conventional kinetic forms are valid under a range of in vivo conditions. For example, if the concentration ratio of enzyme versus substrate is not very high, Michaelis-Menten formalism is applicable for non-isolated reactions (Stoleriu et al., 2004a
,b
). Therefore, in addition to maximal reaction rates, kinetic description of a metabolic network may be reliably obtained.
In this article, we introduce the concept of kinetic constraints for metabolic networks based on kinetic description of enzymatic reactions and show that maximal reaction rates are the constraints only for isolated reactions. In a biochemical network, we show that constraints for formation of a steady state require specific relationships between maximal reaction rates of all enzymes. Reversibility of reactions at system boundary or branching point may significantly impact on kinetic constraints. Moreover, regulations can impose severe constraints on the formation of steady states, and co-regulated networks may significantly enhance these constraints. Furthermore, the theory developed is applied to analyze the kinetic constraints for an actual network that describes sucrose accumulation in the sugar cane culm.
| RESULTS |
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![]() | (2) |
and k are the maximal reaction rate and Michaelis-Menten constant of the enzyme, respectively. For an isolated enzymatic reaction, the reaction capacity is limited by the maximal enzymatic rate. For example, the flux through an isolated enzyme E1, J1, is limited by the maximal reaction rate of E1,
; namely
In a biochemical network, many enzymatic reactions with various limited reaction capacities interplay. How do the interacting enzymatic reactions form a steady state? In this work, we refer to kinetic constraints as the constraints of forming steady states due to the interplay of enzymatic kinetics. In the Appendix, we summarize the principle and relevant topics of kinetic constraints in detail. Here, for introducing the concept of kinetic constraints, we analyze a sequential reaction network with two enzymatic reactions:
If we assume that the flux catalyzed by E1, J1, is the input of the network, a steady state of the network is
![]() | (3) |
and k2 are the maximal reaction rate and Michaelis-Menten constant of E2, respectively. The value S2 is the metabolite concentration. Equation 4 can be readily derived from Eq. 3, as
![]() | (4) |
Therefore, J1 must be smaller than the smaller one of
and
Clearly, when the reaction catalyzed by E1 is isolated, the constraint for J1 is described only by
However, when the two reactions interact, J1 is restricted by kinetic properties of both enzymes:
and
For a sequential network with n enzymes, kinetic constraints,
and
( i = 2 ...n), can be readily derived following the derivation of Eq. A6. Clearly, these constraints only need the maximal reaction rates and they do not need Michaelis-Menten constants for any enzyme. Analysis of the simple example shows that the concept of kinetic constraints is important for understanding the formation of steady states in a biochemical network.
In general, biochemical networks can be very complicated (Stryer, 1997
). They can be unidirectional, reversible, branched, or cyclic, and regulations of enzymes exist in all networks. To understand how steady states are formed in a complex network with regulations, it is essential to understand how kinetic constraints for formation of steady states are affected by network structures and regulations. We therefore analyze how reaction interactions and regulations affect kinetic constraints using the examples in Table 1. In the following, we will assume that for all networks J1 is the input flux, and it is at the system boundary.
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In the Appendix, Network 1 is analyzed in detail. It is shown that, if all reactions follow irreversible Michaelis-Menten kinetics (see Principle for Deriving Kinetic Constraints: Irreversible Michaelis-Menten Kinetics for All Reactions as an Example, in the Appendix), the kinetic constraints for formation of a steady state are independent of all Michaelis-Menten constants for enzymes E1, E3 to En, although they are dependent on k2 and k2b. If reversible reactions do not occur at system boundary or branching point (see Effects of Reversible Reactions on Kinetic Constraints, in the Appendix), the above conclusion remains. However, if the reactions at system boundary or branching point become reversible, the reversibility of these reactions significantly impacts on kinetic constraints. Again, the significances of the results are discussed in detail in the Appendix. In the following, we further discuss a special case in which k2 = k2b, to show how the constraints are related to maximal reaction rates.
For k2 = k2b, the constraints for formation of a steady state at which all metabolite concentrations are non-negative and finite (Eq. A12) become
![]() | (5) |
If the constraints do not satisfy Eq. 5, Network 1 cannot establish a steady state in the sense that the concentrations of at least one metabolite are not non-negative and finite.
Kinetic constraints for cyclic networks with Michaelis-Menten kinetics
As an example, we analyze Network 2. At a steady state, the following mass-balance equation must be valid:
![]() | (6) |
For kn = knc, the constraints for formation of a steady state at which all metabolite concentrations are non-negative and finite are
![]() | (7) |
Michaelis-Menten constants are not required for theoretically analyzing the constraints, but they are set to be unity for numerical simulation. Following Eq. 7, a steady state requires that the smallest of
must be larger than 4.5. Fig. 1 shows the dependence of the evolution of the network on
In Fig. 1, a and b, we fix
In Fig. 1 a,
the network settles onto a steady state for all metabolites. However, in Fig. 1 b,
and although S2 and S3 are still able to reach a steady state, S4 accumulates infinitely. Therefore, the network as a whole cannot reach a steady state. In a similar manner, if
then S2 cannot reach a steady state; and if
then S3 cannot reach a steady state. If
are smaller than 4.5 simultaneously, none of S1, S2, and S3 is able to reach a steady state (Fig. 1 c). In Fig. 1, ac, S5 always establishes a steady state (data not shown).
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Regulation and kinetic constraints
When an enzyme is regulated, its kinetic properties change. How do regulations affect kinetic constraints for formation of steady states in a network? Following the above analysis, we know that kinetic constraints depend on the network structure. It is expected that different regulations such as activation and inhibition may also affect the constraints in different ways, since kinetic constraints depend on description of kinetics. In the following, we examine effects of substrate inhibition. However, any network with known regulation rules can be analyzed using the same approach.
A classic regulation is Michaelis-Menten kinetics with substrate inhibition (Degn, 1968
; Shen and Larter, 1994
). Network 3 shows a sequential network with E2 being inhibited by its substrate S2. The kinetic equation for Michaelis-Menten kinetics with substrate inhibition can be readily derived (Degn, 1968
; Shen and Larter, 1994
). A steady state for Network 3 is described by
![]() | (8) |
is the equilibrium constant for substrate inhibition (Degn,1968
Based on Eq. 8, we obtain that, to establish a steady state at which all metabolite concentrations, Si (i = 2,...n), are non-negative and finite, the following constraints must be satisfied:
![]() | (9) |
in this sequential network.
Network 4 is a cyclic pathway based on Network 2 with E2 being inhibited by its substrate S2. For the cyclic pathway, the constraints for formation of steady states are described as
![]() | (10) |
in this cyclic network. Following Eq. 10, we know that if
for any enzyme Ei (i = 3,...n 1), substrate inhibition of E2 becomes an important constraint for formation of a steady state. Only if
is larger than all of
for i = 3,...n 1, the inhibition becomes unimportant for formation of steady states.
The analysis can be extended to include a network with any complexity. For example, if Jn in Network 4 is an input to another pathway that is assumed to be the same as Network 4, we have Network 5. In addition to Eq. 10, the kinetic constraints for Network 5 also require Eq. 11:
![]() | (11) |
To clearly demonstrate how kinetic constraints due to regulation and complexity of network restrict the formation of steady states, we analyze Network 4 with five enzymes in detail. The following values of parameters are used:
The Michaelis-Menten constants for E3, E4, and E5 are not required for analyzing the kinetic constraints. Fig. 2 summarizes the constraints of fluxes J1 and J5 for various network constructions. Initially, if both J1 and J5 are isolated, they are restricted by the maximal reaction rates of E1 and E5, which are 10 and 8, respectively (column A). If there is no regulation, the kinetic constraints are calculated using Eq. 7 (for simplicity, we set
therefore, the constraints due to
are the same; see Fig. 1 for detailed analysis for the case of varying
). Therefore,
(column B). However, when E2 is inhibited by its substrate S2, kinetic constraint becomes
based on Eq. 10. Fig. 2 clearly demonstrates that regulation may impose severe constraints for formation of steady states (column C). As an example, Fig. 3 shows the development of S2 for two neighboring values of J1. In Fig. 3, all Michaelis-Menten constants are set to be unity for numerical simulation. If J1 = 1.32 < 1.33 (Fig. 3 a), a steady state is established. However, if J1 = 1.34 > 1.33 (Fig. 3 b), no steady state is established for S2. In a similar manner, all possibilities for kinetic constraints in Fig. 2 can be numerically analyzed, and they confirm that Eq. 10 displays the constraints for formation of steady states in Network 4 (data not shown). If Network 4 is extended to Network 5, J5 is an input to the lower part. If it is assumed that the lower part in Network 5 is exactly same as the upper part, a further constraint J5 < 1.33 must be satisfied to maintain a steady state for the whole network. The kinetic constraints for Network 5 are also included in Fig. 2 for comparison (column D). It is clear that, as the complexity of network increases, kinetic constraints become more severe.
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following Eq. 10 we have the following constraints: J1 must be <1.33, otherwise Network 4 cannot establish a steady state. Moreover, if J1 < 0.36, a steady state is guaranteed.
Co-regulation and kinetic constraints
It has recently been shown (Ihmels et al., 2004
) that, for some pathways, only a subset of genes displays significant co-expression, and these sets of genes consist mainly of linear arrangements of enzymes. Moreover, it has been shown (Ihmels et al., 2004
) that, at a branching point, co-regulation of incoming reaction and one of the two outgoing reactions is prevalent. Segre (2004)
analyzed a simple kinetic model, showing that co-regulation might lead to indefinite increase in fluxes.
The approach introduced above is able to assess how kinetic constraints restrict formation of steady states in co-regulated networks. For simplicity, in the first instance, we assume that when enzymes are co-regulated, their maximal reaction rates are increased by the same percentage. Analysis of the kinetic constraints for various networks reveals that for most networks, co-regulation linearly enhances the constraints. For example, for Network 1, if the maximal reaction rates of all enzymes except for E2b are upregulated by a factor
, the kinetic constraints become
![]() | (12) |
and Ji versus
(i = 2,...n)) is different, depending on the values of maximal reaction rates.
Interestingly, for cyclic networks, co-regulation may nonlinearly enhance the kinetic constraints. As an example, we analyze Network 4 and revisit analysis for Fig. 2. When the network is co-regulated for all enzymes apart from the enzyme at cyclic point (E5c), the kinetic constraint is
Using the same values of parameters as those for Fig. 2, we know
As
increases, the constraint is enhanced nonlinearly. If E5c is also enhanced by a factor of
, the constraint becomes
Since
is always larger than
for
> 1, the network is able to absorb larger fluctuations in fluxes if E5c is not co-regulated.
Moreover, if the enzymes in a network are co-regulated with different strengths and the strengths can be quantified, the kinetic constraints of co-regulated networks can also be analyzed using the approach introduced. In terms of the analysis of co-regulation with the same strengths, co-regulated networks are able to establish a steady state in less restricted conditions and therefore the networks more possibly absorb large fluctuations in fluxes.
Kinetic constraints for the network that accumulates sucrose in the sugar cane culm
The approach introduced in this work clearly demonstrates that kinetic constraints are of vital importance to the formation of steady states in biochemical networks. Regulations and co-regulations may have important implications in kinetic constraints. As a first example of the application of this approach, we apply it to the analysis of an actual network that describes sucrose accumulation in the sugar cane culm (Rohwer and Botha, 2001
). The network was analyzed in detail in terms of its kinetic properties (Rohwer and Botha, 2001
). We employ the model as an example, and derive the kinetic constraints for the network. We further employ numerical analysis to confirm the validity of those constraints.
As described in literature (Rohwer and Botha, 2001
), the network includes eight metabolites, two input fluxes, and two output fluxes. The enzymes in the network are regulated in complicated ways, and enzyme kinetics are highly nonlinear. For simplicity, we use the original notations. However, for the consistency with this work, we use symbol J rather than V to represent reaction rates and maximal reaction rates. The two input fluxes are as follows. The value J1 is the flux from external fructose to internal fructose; and J2 is the flux from external glucose to internal glucose. Following the approach developed above and in the Appendix, the kinetic constraints are derived.
The kinetic constraints for glucose and fructose to establish a steady state are
![]() | (13) |
![]() | (14) |
Numerical calculations confirm that Eq. 13 displays the kinetic constraints for glucose and fructose to form a steady state. Fig. 4 a shows that as long as J2 < 0.1576, a steady state is established for glucose. However, if J2 > 0.1576, no steady state is possible for glucose. Fig. 4 b confirms that the kinetic constraints for fructose to establish a steady state are more restricted. As long as J1 > 0.125, fructose cannot settle onto a steady state. The difference of the kinetic constraints for glucose and fructose to establish a steady state is due to the contribution of the second term of the first equation in Eq. 13. In a similar manner, the kinetic constraints for sucrose and hexose phosphate to establish a steady state can be derived, and they are described by Eq. 15, as
![]() | (15) |
numerical calculation confirms that as long as
a steady state can be established for sucrose and hexose phosphate. Otherwise, no steady state is possible for sucrose and hexose phosphate. Finally, the kinetic constraints for sucrose 6-phosphate to establish a steady state can be derived (data not shown); it depends on the steady-state concentrations of many metabolites.
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| CONCLUDING REMARKS |
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In general, biochemical networks comprise a large number of enzymatic reactions, and their structure is complicated. Networks can be unidirectional, reversible, branched, or cyclic. Moreover, enzyme regulations generally exist (Stryer, 1997
). Our analysis shows that for the reactions occurring at system boundary or branching point, their reversibility significantly impacts on kinetic constraints for formation of steady states. Therefore, In addition to their roles in flux control (Koch, 1967
), reversible reactions may play an important role in maintaining steady states in biochemical networks. Moreover, analysis of the kinetic constraints for an actual network that accumulates sucrose in the sugar cane culm clearly shows that naturally occurring networks are indeed restricted by kinetic constraints.
Enzyme catalysis can be regulated by compounds which are themselves reaction substrates and products, and the consequent regulatory networks are the basis of biological functioning in cells. In a pathway, such a process settles onto a stable, though possibly time-dependent, state. Although metabolic networks can be described in terms of flux control (Fell, 1997
), spatiotemporal behavior (Goldbeter, 1996
), and energy utility (Ross and Schell, 1987
), ultimately, their behavior arises from the formation of stable states (Liu et al., 1997
). One of the stable states is a steady state. Based on mass-action kinetics, general theories about reaction networks have been developed, and the properties of reaction networks have been extensively studied (Clarke, 1981
, 1988
; Feinberg, 1989
; Horn and Jackson, 1972
; Heinrich and Schuster, 1996
). Recently, it has been shown that, for receptor-ligand interactions, existence, uniqueness and global stability of positive steady states can be guaranteed under mass-action kinetics (Chaves et al., 2004
). Enzymatic kinetics are usually derived from traditional mass-action kinetics together with simplifying assumptions such as the existence of a quasi-steady state (Segel and Selmrod, 1989
; Stoleriu et al., 2004a
). At the level of enzymatic reactions, the kinetic rate laws exhibit some special features such as saturation and regulation (Heinrich and Schuster, 1996
). Those features are due predominantly to the catalyzing functions of enzymes, and they are captured by Michaelis-Menten-type kinetics. At the level of mass-action kinetics of an enzyme-catalyzed reaction, although the rate laws for all reactions follow mass-action kinetics, the concentration of any form of an enzyme cannot arbitrarily change as it is limited by the total concentration of the enzyme. Therefore, although the saturation and regulation features of enzymatic rate laws cannot be immediately described by mass-action kinetics (Heinrich and Schuster, 1996
), they are the consequences of the mass-action kinetics in which the concentrations of all forms of an enzyme are limited. To copy with those features, generalized mass-action kinetics were suggested (Schauer and Heinrich, 1983
). This work shows that the features of enzymatic reactions may have implications for the formation of steady states in biochemical networks. Once a steady state is established in a network, various approaches can be applied to study the properties of the networks. For example, flux balance analysis may analyze the integrated functions. Steady-state perturbation experiments may reveal the underlying regulatory mechanisms (Andrec et al., 2005
; Torralba et al., 2003
; Vance et al., 2002
).
When enzymes are regulated, a network of enzymatic reactions is capable of generating various steady- and time-dependent states. Our analysis shows that substrate inhibition, a typical type of regulation, may impose severe constraints for formation of steady states. Therefore, in addition to the capabilities in generating spatiotemporal behavior (Shen and Larter, 1994
), regulations may have significance in restricting formation of possible stable states. When time-dependent states emerge, formation of stable states can be analyzed in terms of the balance of average fluxes (Liu, 1999a
,b
, 2001
; Liu and Crawford, 2000
). Moreover, the relationship between a stable state and the nature of environmental fluctuations can be established (Liu and Crawford, 2000
).
It is clearly demonstrated that co-regulations can dramatically enhance capability for a network to form a stable state. Co-regulation patterns based on the evidence of experimental observations can be readily analyzed in terms of their effects on kinetic constraints. It is expected that the analysis can be extended to include how co-regulated networks are able to accommodate various environmental fluctuations, following the methods previously introduced for an extracted small model system with product activation (Liu and Crawford, 2000
).
Clearly, an essential assumption for constraint-based analysis is that a steady state is established. Searching for possible functions beyond the constraints for which a steady state is established is unrealistic for constraint-based analysis. In this sense, kinetic constraints are of vital importance when constraint-based analysis is applied. Combination of stoichiometric, thermodynamic, and kinetic constraints will appropriately restrict the search for biological phenotypes.
| APPENDIX: PRINCIPLE FOR DERIVING KINETIC CONSTRAINTS AND RELEVANT TOPICSA BRANCHED NETWORK AS AN EXAMPLE |
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Flux balance at a steady state
The mass balance of Network 1 is described by
![]() | (A1) |
Principle for deriving kinetic constraints: irreversible Michaelis-Menten kinetics for all reactions as an example
For this case, the steady state of Eq. A1 becomes Eq. A2:
![]() | (A2) |
and ki are the maximal reaction rate and Michaelis-Menten constant of Ei (i = 2,..n), respectively. The values
and k2b are the maximal reaction rate and Michaelis-Menten constant for enzyme E2b, respectively. The value Si (i = 1,...n) is the metabolite concentration.
The kinetic constraints can be derived as follows. The first expression in Eq. A2 contains only one variable, S2. Therefore, it can be directly solved as
![]() | (A3) |
![]() | (A4) |
Therefore, S2 has no positive solution. Therefore, the kinetic constraints for S2 to reach a steady state is a < 0, which leads to
![]() | (A5) |
when S2
. Therefore, Eq. A5 implies that S2 is able to establish a steady state that is finite. For a sequential network,
Therefore, Eq. A5 can be readily generalized to
![]() | (A6) |
![]() | (A7) |
![]() | (A8) |
![]() | (A9) |
![]() | (A10) |
![]() | (A11) |
![]() | (A12) |
Effects of reversible reactions on kinetic constraints
If an enzymatic reaction is reversible, we assume that its rate law follows the uni-uni mechanism of Michaelis-Menten kinetics (Heinrich and Schuster, 1996
), as
![]() | (A13) |
and
denote the maximal reaction rates of the forward and reverse reactions, respectively. The values kS and kP are the Michaelis-Menten constants of substrate, S, and product, P, respectively. For Network 1, we will show that, for the reactions that do not occur at the boundary of the network or branching point, reversibility of reactions do not affect kinetic constraints. However, for the reactions at boundary of the network and branching point, introduction of reversibility of reactions may have significant effects on kinetic constraints.
When the reaction catalyzed by E3 in Network 1 is reversible, the steady state of Network 1 is described by
![]() | (A14) |
![]() | (A15) |
When the reaction catalyzed by E2 is reversible, the steady state of Network 1 is described by
![]() | (A16) |
![]() | (A17) |
![]() | (A18) |
![]() | (A19) |
0), the reaction catalyzed by E2 becomes irreversible and Eq. A19 becomes Eq. A10. As S3 increases, Eq. A19 becomes less restricted. The effects of reversibility of the reaction catalyzed by E2 on kinetic constraints can be understood as follows. With the increase of S3, the reverse reaction is enhanced. Therefore, the flux entering the branch catalyzed by E2 becomes smaller for a specific J1. In other words, for specific
(i = 3,...n), Si (i = 3,...n) may reach a steady state for a wider range of J1 as far as the branch catalyzed by E2 is concerned. If S3 reaches such a value that the reaction catalyzed by E2 is at its equilibrium (i.e.,
), Eq. A19 becomes J1 <
. Once this happens, the flux entering the branch catalyzed by E2 is zero. As far as this branch is concerned, there is no constraint for J1. Clearly, for this case, Network 1 becomes a sequential network to the branch catalyzed by E2b whose constraints are analyzed in Principle for Deriving Kinetic Constraints: Irreversible Michaelis-Menten Kinetics for All Reactions as an Example, above. In summary, when the reaction catalyzed by E2 is reversible, the kinetic constraints for formation of a steady state are in the form of
![]() | (A20) |
Incorporation of experimentally measurable data into kinetic constraints
In principle, kinetic constraints can always be derived based on the approaches introduced. However, when a network becomes complicated, analysis of kinetic constraints may become a difficult task. Introduction of some experimentally measurable data may significantly simplify the analysis of kinetic constraints. For example, S2 in Eq. A12 should be in the form of Eqs. A3 and A4. However, for experimentally measurable S2, kinetic constraints can be directly calculated using Eq. A12. In a similar manner, if both S2 and S3 are known, the kinetic constraints for the case for which the reaction catalyzed by E2 is reversible, can be calculated using Eq. A20. No further efforts are required to link S2 and S3 with kinetic parameters.
More generally, the approach introduced can be extended to include the formation of any finite stable state that can be either a steady state or a time-dependent state (Liu and Crawford, 2000
). For a metabolite concentration, S, we know that, as long as
when S
, S cannot increase infinitely. For this case, S is bounded and emergence of finite stable states becomes possible. Therefore, we may derive kinetic constraints for formation of a finite stable state by analyzing the conditions under which
when S
. If a network is subject to environmental fluctuations, appropriate temporal average should be introduced to describe the effects of the fluctuations on flux distribution (Liu and Crawford, 2000
).
Kinetic constraints and level of networks
Following the conventional practice, when the kinetics of an enzymatic reaction are described, concentrations of metabolites are considered to be variables, and concentrations of enzymes are assumed to be parameters that do not change with time. This implies that the derived kinetic constraints are directly applicable to the level of enzymatic reactions. If the synthesis and degradation of enzymes are considered, the concentrations of enzymes become variables. For this case, kinetic constraints for formation of steady states should be examined for the conditions in which concentrations of enzymes are also variables.
| ACKNOWLEDGEMENTS |
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The author acknowledges the Scottish Executive Environment and Rural Affairs Department for support.
Submitted on November 11, 2004; accepted for publication February 14, 2005.
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