149 research outputs found
Characteristic, completion or matching timescales? An analysis of temporary boundaries in enzyme kinetics
Scaling analysis exploiting timescale separation has been one of the most
important techniques in the quantitative analysis of nonlinear dynamical
systems in mathematical and theoretical biology. In the case of enzyme
catalyzed reactions, it is often overlooked that the characteristic timescales
used for the scaling the rate equations are not ideal for determining when
concentrations and reaction rates reach their maximum values. In this work, we
first illustrate this point by considering the classic example of the
single-enzyme, single-substrate Michaelis--Menten reaction mechanism. We then
extend this analysis to a more complicated reaction mechanism, the auxiliary
enzyme reaction, in which a substrate is converted to product in two sequential
enzyme-catalyzed reactions. In this case, depending on the ordering of the
relevant timescales, several dynamic regimes can emerge. In addition to the
characteristic timescales for these regimes, we derive matching timescales that
determine (approximately) when the transitions from initial fast transient to
steady-state kinetics occurs. The approach presented here is applicable to a
wide range of singular perturbation problems in nonlinear dynamical systems.Comment: 35 pages, 11 figure
Validity of the MichaelisâMenten equation â steadyâstate or reactant stationary assumption: that is the question
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/102681/1/febs12564.pd
Protein Interactions and Transition Times that Influence the Pathogenesis of Protein Folding Diseases
Designing nanoparticle treatment of autoimmunity with quantitative biology
Peer Reviewedhttps://deepblue.lib.umich.edu/bitstream/2027.42/141246/1/imcb201320.pd
Stochastic enzyme kinetics and the quasi-steady-state reductions: Application of the slow scale linear noise approximation \`a la Fenichel
The linear noise approximation models the random fluctuations from the mean
field model of a chemical reaction that unfolds near the thermodynamic limit.
Specifically, the fluctuations obey a linear Langevin equation up to order
, where is the size of the chemical system (usually the
volume). Under the presence of disparate timescales, the linear noise
approximation admits a quasi-steady-state reduction referred to as the slow
scale linear noise approximation. However, the slow scale linear approximation
has only been derived for fast/slow systems that are in Tikhonov standard form.
In this work, we derive the slow scale linear noise approximation directly from
Fenichel theory, without the need for a priori scaling and dimensional
analysis. In so doing, we can apply for the first time the slow scale linear
noise approximation to fast/slow systems that are not of standard form. This is
important, because often times algorithms are only computationally expensive in
parameter ranges where the system is singularly perturbed, but not in standard
form. We also comment on the breakdown of the slow scale linear noise
approximation near dynamic bifurcation points -- a topic that has remained
absent in the chemical kinetics literature, despite the presence of
bifurcations in simple biochemical reactions, such the Michaelis--Menten
reaction mechanism.Comment: 22 pages, 2 figure
The Quasi-Steady-State Approximations revisited: Timescales, small parameters, singularities, and normal forms in enzyme kinetic
In this work, we revisit the scaling analysis and commonly accepted
conditions for the validity of the standard, reverse and total
quasi-steady-state approximations through the lens of dimensional
Tikhonov-Fenichel parameters and their respective critical manifolds. By
combining Tikhonov-Fenichel parameters with scaling analysis and energy
methods, we derive improved upper bounds on the approximation error for the
standard, reverse and total quasi-steady-state approximations. Furthermore,
previous analyses suggest that the reverse quasi-steady-state approximation is
only valid when initial enzyme concentrations greatly exceed initial substrate
concentrations. However, our results indicate that this approximation can be
valid when initial enzyme and substrate concentrations are of equal magnitude.
Using energy methods, we find that the condition for the validity of the
reverse quasi-steady-state approximation is far less restrictive than was
previously assumed, and we derive a new "small" parameter that determines the
validity of this approximation. In doing so, we extend the established domain
of validity for the reverse quasi-steady-state approximation. Consequently,
this opens up the possibility of utilizing the reverse quasi-steady-state
approximation to model enzyme catalyzed reactions and estimate kinetic
parameters in enzymatic assays at much lower enzyme to substrate ratios than
was previously thought. Moreover, we show for the first time that the critical
manifold of the reverse quasi-steady-state approximation contains a singular
point where normal hyperbolicity is lost. Associated with this singularity is a
transcritical bifurcation, and the corresponding normal form of this
bifurcation is recovered through scaling analysis.Comment: 50 pages, 10 figures, 1 tabl
On the validity of the stochastic quasi-steady-state approximation in open enzyme catalyzed reactions: Timescale separation or singular perturbation?
The quasi-steady-state approximation is widely used to develop simplified
deterministic or stochastic models of enzyme catalyzed reactions. In
deterministic models, the quasi-steady-state approximation can be
mathematically justified from singular perturbation theory. For several closed
enzymatic reactions, the homologous extension of the quasi-steady-state
approximation to the stochastic regime, known as the stochastic
quasi-steady-state approximation, has been shown to be accurate under the
analogous conditions that permit the quasi-steady-state reduction of the
deterministic counterpart. However, it was recently demonstrated that the
extension of the stochastic quasi-steady-state approximation to an open
Michaelis--Menten reaction mechanism is only valid under a condition that is
far more restrictive than the qualifier that ensures the validity of its
corresponding deterministic quasi-steady-state approximation. In this paper, we
suggest a possible explanation for this discrepancy from the lens of geometric
singular perturbation theory. In so doing, we illustrate a misconception in the
application of the quasi-steady-state approximation: timescale separation does
not imply singular perturbation.Comment: 19 pages, 1 Figur
Natural parameter conditions for singular perturbations of chemical and biochemical reaction networks
We consider reaction networks that admit a singular perturbation reduction in
a certain parameter range. The focus of this paper is on deriving "small
parameters" (briefly for small perturbation parameters), to gauge the accuracy
of the reduction, in a manner that is consistent, amenable to computation and
permits an interpretation in chemical or biochemical terms. Our work is based
on local timescale estimates via ratios of the real parts of eigenvalues of the
Jacobian near critical manifolds; this approach is familiar from computational
singular perturbation theory. While parameters derived by this method cannot
provide universal estimates for the accuracy of a reduction, they represent a
critical first step toward this end. Working directly with eigenvalues is
generally unfeasible, and at best cumbersome. Therefore we focus on the
coefficients of the characteristic polynomial to derive parameters, and relate
them to timescales. Thus we obtain distinguished parameters for systems of
arbitrary dimension, with particular emphasis on reduction to dimension one. As
a first application, we discuss the Michaelis--Menten reaction mechanism system
in various settings, with new and perhaps surprising results. We proceed to
investigate more complex enzyme catalyzed reaction mechanisms (uncompetitive,
competitive inhibition and cooperativity) of dimension three, with reductions
to dimension one and two. The distinguished parameters we derive for these
three-dimensional systems are new; in fact no rigorous derivation of small
parameters seems to exist in the literature so far. Numerical simulations are
included to illustrate the efficacy of the parameters obtained, but also to
show that certain limitations must be observed.Comment: 57 pages, 17 figure
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