Chapter 8 – Theoretical Biophysics 333
The value of γ/m = 1/τ is a measure of the collision frequency between the biomolecule
atoms and water molecules, where τ is the mean time between collisions. For example, for
individual atoms in a protein, τ is in the range 25–50 ps, whereas for water molecules, τ is
~80 ps. The limit of high γ values is an overdamped regime in which viscous forces dominate
over inertial forces. Here τ can for some biomolecule systems in water be as low as ~1 ps,
which is a diffusion (as opposed to stochastic) dominated limit called Brownian dynamics.
The equation of motion in this regime then reduces to the Smoluchowski diffusion equation,
which we will discuss later in this chapter in the section on reaction–diffusion analysis.
One effect of applying a stochastic frictional drag term in LD is that this can be used to
slow down the motions of fast-moving particles in the simulation and thus act as feedback
mechanism to clamp the particle speed range within certain limits. Since the system tem
perature depends on particle speeds, this method thus equates to a Langevin thermostat (or
equivalently a barostat to maintain the pressure of the system). Similarly, other nonstochastic
thermostat algorithms can also be used, which all in effect include additional weak frictional
coupling constants in the equation of motion, including the Anderson, isokinetic/Gaussian,
Nosé–Hoover, and Berendsen thermostats.
8.2.8 COARSE-GRAINED SIMULATION TOOLS
There are a range of coarse-grained (CG) simulation approaches that, instead of probing the
exact coordinates of every single atom in the system independently, will pool together groups
of atoms as a rigid, or semirigid, structure, for example, as connected atoms of a single amino
acid residue in a protein, or coarser still of groups of residues in a single structural motif
in a protein. The forces experienced by the components of biological matter in these CG
simulations can also be significantly simplified versions that only approximate the underlying
QM potential energy. These reductions in model complexity are a compromise to achieving
computational tractability in the simulations and ultimately enable larger length and time
scales to be simulated at the expense of loss of fine detail in the structural makeup of the
simulated biological matter.
This coarse-graining costs less computational time and enables longer simulation times to
be achieved, for example, time scales up to ~10−5 s can be simulated. However, again there is a
time scale gap since large molecular conformational changes under experimental conditions
can be much slower than this, perhaps lasting hundreds to thousands of microseconds.
Further coarse-graining can allow access into these longer time scales, for example, by
pooling together atoms into functional structural motifs and modeling the connection
between the motifs with, in effect, simple springs, resulting in a simple harmonic potential
energy function.
Mesoscale models are at a higher length scale of coarse-graining, which can be applied
to larger macromolecular structures. These, in effect, pool several atoms together to create
relatively large soft-matter units characterized by relatively few material parameters, such
as mechanical stiffness, Young’s modulus, and the Poisson ratio. Mesoscale simulations can
model the behavior of macromolecular systems potentially over a time scale of seconds, but
clearly what they lack is the fine detail of information as to what happens at the level of specific
single molecules or atoms. However, in the same vein of hybrid QM/MM simulations, hybrid
mesoscale/CG approaches can combine elements of mesoscale simulations with smaller
length scale CG simulations, and similarly hybrid CG/MM simulations can be performed,
with the strategy for all these hybrid methods that the finer length scale simulation tools
focus on just highly localized regions of a biomolecule, while the longer length scale simula
tion tool generates peripheral information about the surrounding structures.
Hybrid QM/MM approaches are particularly popular for investigating molecular docking
processes. that is, how well or not a small ligand molecule binds to a region of another larger
molecule. This process often utilizes relative simple scoring functions to generate rapid
estimates for the goodness of fit for a docked molecule to a putative binding site to facilitate
fast computational screening and is of specific interest in in silico drug design, that is, using
computational molecular simulations to develop new pharmaceutical chemicals.