 |
Chapter 5
Writing Rate Laws for Binding Processes
Binding is ubiquitous in biological systems. We define binding
to be any non-covalent linking of one chemical species to
another. Examples of binding are 1) hormone - receptor binding,
2) neurotransmitter - receptor binding, 3) cytokine - receptor
binding, 4) protein (hetero- or homo-) dimerization, 5) enzyme -
substrate interactions, 6) ion - protein binding, 7) allosteric
binding of a cellular metabolite to a regulated enzyme, 8)
transcription factor binding to regulatory elements of DNA, and
many others. Often, we are concerned with binding of a small
molecule or ion to a protein. In such cases, the small molecule
can be considered the ligand and the protein can be considered
the receptor. If we let L be the concentration of ligand, and R
be the concentration of receptor, then the simplest form of the
fundamental rate law for the binding process is

where k1 is a second order rate constant. Both
sides would be multiplied by V, the volume in which the binding
takes place, if the flux was to be written in mol/sec. If we
denote the ligand-receptor complex as C, then the flux for the
unbinding process is first order, and has the form

We examined the equilibrium behavior of a binding reaction a
few pages ago, so now we can extend this paradigm to see why the
phenomenon of binding results in saturation behavior in many
biological processes. And this is exactly what we will do in the
next chapter when we develop the rate law for an enzymatic
process. There are, however, several important features of
binding processes that are frequently encountered in modeling
projects. The first of these is cooperativity.
Cooperativity is the word used to describe a response that is
out of proportion to its stimulus. To understand this, recall the
binding equation from the previous chapter, or if you prefer, the
Michaelis-Menten equation for the catalytic flux of a simple
enzyme.

If h is a hormone, and r is its receptor, then the cellular
response to this hormone will be proportional to [hr]. This means
that for a three fold change in [h], you will get a three-fold
change in response, at least as long as [h] is less than or equal
to KD. At concentrations greater than the KD,
a 3-fold change will result in less than a 3-fold change in [hr],
and consequently, less than a 3-fold change in the response. This
is just another way of saying that the response saturates.
For many hormonal stimuli, however, the cellular response is
many fold greater than the factor by which [h] changes. For
example, the production of InsP3 increases 5 to
10-fold in response to a doubling of norepinephrine concentration
outside a vascular smooth muscle cell. Clearly, the simple
binding equation is incapable of this behavior. It could produce
no more than a two-fold change in response for a doubling of the
hormone concentration.
In a classic study of the kinetics of oxygen binding to
hemoglobin, A.V. Hill formulated a modification of the usual
binding equation that permits it to account for cooperative
behavior. He introduced an exponent that has come to be known as
the Hill coefficient. We recommend that you use the following
expression for these situations:

Of course, when n = 1, the equation reverts to the classical
form. For n>1 the response will display what is called
positive cooperativity, and for n<1, the response is
negatively cooperative. This has the useful consequence that
3-fold changes in [h] are no longer limited to 3-fold changes in
[hr] or 3-fold changes in response. In fact, as shown in figure
5-1, the response to a doubling of [h] can be huge.

To understand the significance of figure 5-1, notice that the
quantity plotted on the vertical axis, the "Hill
Fraction", is equal to

where C is the hormone concentration, and KD is the
dissociation constant. This ratio, just like the corresponding
fraction without the Hill coefficient, always falls in the range
from zero to one, and represents the fraction of receptors
occupied by hormone. On the horizontal axis, we've plotted the
ratio of hormone concentration to its dissociation constant.
Consequently, this axis reveals whether the current concentration
is greater or less than the concentration at half-maximal
binding, and a value of 0.1 on the horizontal axis means simply
that the current concentration is ten times less than the KD.
Figure 5-1 is plotted log-log to emphasize the ability of
cooperative mechanisms to produce more than 2-fold changes in
response for only a 2-fold change in the stimulus. To see this,
recognize that the stimulus is the hormone concentration on the
horizontal axis, and the response will be proportional to the
fraction of receptors bound to hormone, as plotted on the
vertical axis. As a specific example, notice that for a Hill
coefficient of 2, a doubling of stimulus (from 0.2 to 0.4) yields
a 10-fold increase in response (from 0.01 to 0.1).
Cooperativity of this magnitude is commonplace in biological
systems.
|  |