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- Markov (state) models (1)
- Markov models (1)
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Protein-ligand interactions are essential for nearly all biological processes, and yet the bio-
physical mechanism that enables potential binding partners to associate before specific binding
occurs remains poorly understood. Fundamental questions include which factors influence the
formation of protein-ligand encounter complexes, and whether designated association path-
ways exist. In this article we introduce a computational approach to systematically analyze
the complete ensemble of association pathways and to thus investigate these questions. This
approach is employed here to study the binding of a phosphate ion to the Escherichia coli
Phosphate Binding Protein. Various mutants of the protein are considered and their effects
on binding free energy profiles, association rates and association pathway distributions are
quantified. The results reveal the existence of two anion attractors, i.e. regions that initially
attract negatively charged particles and allow them to be efficiently screened for phosphate
which is specifically bound subsequently. Point mutations that affect the charge on these
attractors modulate their attraction strength and speed up association to a factor of 10 of
the diffusion limit and thus change the association pathways of the phosphate ligand. It is
demonstrated that a phosphate that pre-binds to such an attractor neutralizes its attraction
effect to the environment, making the simultaneous association of a second phosphate ion
unlikely. Our study suggests ways how structural properties can be used to tune molecular
association kinetics so as to optimize the efficiency of binding, and highlights the importance
of kinetic properties.
Dynamical fingerprints of macromolecules obtained from experiments often seem to indicate two- or
three state kinetics while simulations typically reveal a more complex picture. Markov state models of
molecular conformational dynamics can be used to predict these dynamical fingerprints and to reconcile
experiment with simulation. This is illustrated on two model systems: a one-dimensional energy surface
and a four-state model of a protein folding equilibrium. We show that (i) there might be no process
which corresponds to our notion of folding, (ii) often the experiment will be insensitive to some of the
processes present in the system, (iii) with a suitable combination the observable and initial conditions in
a relaxation experiment one can selectively measure specific processes. Furthermore, our method can be
used to design experiments such that specific processes appear with large amplitudes. We demonstrate
that for a fluorescence quenching experiment of the MR121-G9-W peptide.
Dynamical averages based on functionals of dynamical trajectories, such as time-correlation func-
tions, play an important role in determining kinetic or transport properties of matter. At temperatures
of interest, the expectations of these quantities are often dominated by contributions from rare events,
making the precise calculation of these quantities by molecular dynamics simulation difficult. Here,
we present a reweighting method for combining simulations from multiple temperatures (or from
simulated or parallel tempering simulations) to compute an optimal estimate of the dynamical prop-
erties at the temperature of interest without the need to invoke an approximate kinetic model (such as
the Arrhenius law). Continuous and differentiable estimates of these expectations at any temperature
in the sampled range can also be computed, along with an assessment of the associated statistical
uncertainty. For rare events, aggregating data from multiple temperatures can produce an estimate
of the desired precision at greatly reduced computational cost compared with simulations conducted
at a single temperature. Here, we describe use of the method for the canonical (NVT) ensemble us-
ing four common models of dynamics (canonical distribution of Hamiltonian trajectories, Andersen
thermostatting, Langevin, and overdamped Langevin or Brownian dynamics), but it can be applied to
any thermodynamic ensemble provided the ratio of path probabilities at different temperatures can be
computed. To illustrate the method, we compute a time-correlation function for solvated terminally-
blocked alanine peptide across a range of temperatures using trajectories harvested using a modified
parallel tempering protocol.
Markov state models of molecular kinetics (MSMs), in which the long-time statistical dynamics
of a molecule is approximated by a Markov chain on a discrete partition of configuration space, have
seen widespread use in recent years. This approach has many appealing characteristics compared
to straightforward molecular dynamics simulation and analysis, including the potential to mitigate
the sampling problem by extracting long-time kinetic information from short trajectories and the
ability to straightforwardly calculate expectation values and statistical uncertainties of various
stationary and dynamical molecular observables. In this article, we summarize the current state of
the art in generation and validation of MSMs and give some important new results. We describe
an upper bound for the approximation error made by modeling molecular dynamics with an MSM
and we show that this error can be made arbitrarily small with surprisingly little effort. In contrast
to previous practice, it becomes clear that the best MSM is not obtained by the most metastable
discretization, but the MSM can be much improved if non-metastable states are introduced near
the transition states. Moreover, we show that it is not necessary to resolve all slow processes
by the state space partitioning, but individual dynamical processes of interest can be resolved
separately. We also present an efficient estimator for reversible transition matrices and a robust
test to validate that an MSM reproduces the kinetics of the molecular dynamics data.
Resolving the apparent gap in complexity between
simulated and measured kinetics of biomolecules
(2012)
Molecular simulations of biomolecules often reveal a complex picture of the their kinetics,
whereas kinetic experiments typically seem to indicate considerably simpler two- or three-state
kinetics. Markov state models (MSM) provide a tool to link between simulation and experi-
ment, and to resolve this apparent contradiction.
In many fields of physics, chemistry and biology the characterization of dynamical processes
between states or species is of fundamental interest. The central mathematical function in such sit-
uations is the committor probability - a generalized reaction coordinate that measures the progress
of the process of interest as the probability of proceeding towards the target state rather than re-
lapsing to the source state. Here, we present methodology for the efficient computation of com-
mittor probabilities for large-scale systems, such as, for example simuations of biomolecular fold-
ing. A method is derived for computing the committor for discrete state spaces using eigenvectors
with expressions for the sensitivity and a Bayesian error model for the committor. The concepts
are illustrated on two examples of diffusive dynamics with a very large number of states: a two-
dimensional model potential with three minima, and a three-dimensional model representing
protein-ligand binding. The method can finally be used to compute committor probabilities in-
cluding error estimations for medium and large system sizes allowing access to the apparatus of
transition path theory and its applications.
Markov (state) models (MSMs) have attracted a lot of interest recently as they (1) can probe
long-term molecular kinetics based on short-time simulations, (2) offer a way to analyze great
amounts of simulation data with relatively little subjectivity of the analyst, (3) provide insight into
microscopic quantities such as the ensemble of transition pathways, and (4) allow simulation data
to be reconciled with measurement data in a rigorous and explicit way. Here we sketch our current
perspective of Markov models and explain in short their theoretical basis and assumptions. We
describe transition path theory which allows the entire ensemble of protein folding pathways to be
investigated and that combines naturally with Markov models. Experimental observations can be
naturally linked to Markov models with the dynamical fingerprint theory, by which experimentally
observable timescales can be equipped with an understanding of the structural rearrangement
processes that take place at these timescales. The concepts of this paper are illustrated by a
simple kinetic model of protein folding.
While seemingly straightforward in principle, the reliable estimation of rate constants is seldom easy in practice. Numerous issues, such as the complication of poor reaction coordinates, cause obvious approaches to yield unreliable estimates. When a reliable order parameter is available, the reactive flux theory of Chandler allows the rate constant to be extracted from the plateau region of an appropriate reactive flux correlation function. However, when applied to real data from single- molecule experiments or molecular dynamics simulations, the reactive flux correlation function requires the numerical differentiation of a noisy empirical correlation function, which can result in an unacceptably poor estimate of the rate and pathological dependence on the sampling interval. We present a modified version of this theory which does not require numerical derivatives, allowing rate constants to be robustly estimated from the time-correlation function directly. We illustrate the approach using single-molecule passive force spectroscopy measurements of an RNA hairpin.