204 6.1 Introduction
in Chapters 3 and 4. However, an important point to note here about single-molecule methods
concerns the ergodic hypothesis of statistical thermodynamics. The ergodic hypothesis
maintains that there is an equivalence between ensemble and single-molecule properties. In
essence, over long periods of time, all accessible microstates are equally probable. This means
that an ensemble average measurement (e.g., obtained from the mean average from many
thousands of molecules) will be the same as the time-averaged measurement taken from one
single molecule over a long period of time. The key difference with a single-molecule experi
ment is that one can sample the whole probability distribution of all microstates as opposed
to just determining the mean value from all microstates as is the case from a bulk ensemble
average experiment, though the caveat is that in practice this often involves generating sig
nificant amounts of data from single-molecule experiments to properly sample the under
lying probability distribution.
KEY POINT 6.1
The ergodic hypothesis, that all accessible microstates with the same energy are equally
probable over a long time, is relevant to single-molecule methods since it implies that
the population mean measurement from a bulk ensemble experiment, involving typ
ically several thousand molecules or more, will be the same as the mean of several
measurements made on a single molecule sampled over a long period of time.
Statistical thermodynamics implicitly assumes ensemble average parameters. That is, a
system with many, many particles. For example, a single microliter of water contains ~1019
molecules. To apply the same concepts to a single molecule requires the ergodic hypothesis.
Intuitively, one might think that the mean average property of thousands upon thousands
of molecules is an adequate description for any given single molecule. In some very simple,
or exceptional, molecular systems, this is, in fact, the case. However, in general, this is not
strictly true. The reason is that single biomolecules often exist in multiple microstates,
which is in general intrinsically related to their biological function. A microstate here is
essentially a measure of the free energy locked into that molecule, which is a combination
of mainly chemical binding energy, the so-called enthalpy, and energy associated with how
disordered the molecule is, or entropy. There are many molecules that, for example, exist in
several different spatial conformations; a good illustration of which are molecular machines,
whose theory of translocation is discussed later in Chapter 8. In other words, the prime
reason for studying biology at the level of single molecules is the prevalence of molecular
heterogeneity.
In the case of molecular machines, although there may be one single conformation that
has a lower free energy microstate than the others, and thus is the most stable, several other
shorter-lived conformations exist that are utilized in different stages of force and motion
generation. The mean ensemble average usually looks similar to the most stable of these
different conformations, but this single average parameter tells us very little of the behavior
of the other shorter lived but functionally essential conformational states. What cannot be
done with bulk ensemble average analysis is to probe such multistate molecular systems. The
power of single-molecule experiments is that these subpopulations of molecular microstates
can be explored directly and individually. Such subpopulations of states are a vital feature of
the proper functioning of natural molecular machines.
As discussed in Chapter 2, there is a fundamental energetic instability in molecular
machines, which allows them to switch between multiple states as part of their underlying
physiological function. There are, however, many experimental biophysical methods that can
be employed in bulk ensemble investigations to synchronize a molecular population. For
example, these include thermal and chemical jumps such as stopped-flow reactions, electric
and optical methods to align molecules, as well as freezing and/or crystallizing a population.
A risk with such approaches is that the normal physiological functioning may be different.
Some biological tissues, for example, muscles and cell membranes, are naturally ordered on a