Abstract

Ordinary differential equation models have become a wide-spread approach to analyze dynamical systems and understand underlying mechanisms. Model parameters are often unknown and have to be estimated from experimental data, e.g., by maximum-likelihood estimation. In particular, models of biological systems contain a large number of parameters. To reduce the dimensionality of the parameter space, steady-state information is incorporated in the parameter estimation process. For non-linear models, analytical steady-state calculation typically leads to higher-order polynomial equations for which no closed-form solutions can be obtained. This can be circumvented by solving the steady-state equations for kinetic parameters, which results in a linear equation system with comparatively simple solutions. At the same time multiplicity of steady-state solutions is avoided, which otherwise is problematic for optimization. When solved for kinetic parameters, however, steady-state constraints tend to become negative for particular model specifications, thus, generating new types of optimization problems. Here, we present an algorithm based on graph theory that derives non-negative, analytical steady-state expressions by stepwise removal of cyclic dependencies between dynamical variables. The algorithm avoids multiple steady-state solutions by construction. We show that our method is applicable to most common classes of biochemical reaction networks containing inhibition terms, mass-action and Hill-type kinetic equations. Comparing the performance of parameter estimation for different analytical and numerical methods of incorporating steady-state information, we show that our approach is especially well-tailored to guarantee a high success rate of optimization.

Highlights

  • Dynamical systems are frequently modeled by systems of ordinary differential equations (ODEs)

  • The kinetic parameters and initial conditions together span the space of model parameters θ = (p, x0)

  • Since solving for state variables often leads to higher-order equations for which solutions are difficult to obtain, one has at least partially to solve for kinetic parameters

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Summary

Introduction

Dynamical systems are frequently modeled by systems of ordinary differential equations (ODEs). Distributed molecules are treated as continuous quantities interacting with each other according to kinetic laws, e.g., mass-action or Michaelis-Menten kinetics. A typical ODE system x = f (x, p, u(t)) , x(0) = x0 (1). Determines the time-evolution of an N-dimensional state vector x(t). P ∈ RM+ denotes the M-dimensional vector of nonnegative kinetic parameters. The vector x0 ∈ RN+,0, where R+,0 = R+ ∪ {0}, gives the set of initial conditions. The kinetic parameters and initial conditions together span the space of model parameters θ = (p, x0). The explicit time-dependency via u(t) corresponds to external driving forces, like drug stimuli in biological dynamic systems

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