BioPHYSICAL chemistry

(singke) #1

58 PARTI THERMODYNAMICS AND KINETICS


differ in how they are regulated. Whereas
inhibitors for kinases have been identified
by random compound screening, few suc-
cessful drugs have been developed using
design principles. In recent design studies
(Noble et al. 2004; Ahn & Resing 2005;
Cohen et al. 2005), the ATP-binding site of
protein kinases has been targeted. At the site
is a gatekeeper residue that flanks a highly
variable hydrophobic portion of the ATP-
binding pocket. Differences in the size of this
residue as well as the surrounding amino acid
residues for different protein kinases have
been used to achieve selectivity. Protein
kinases can exist in inactive forms that are
also attractive for drugs.
Protein dynamics play a role in the affinity and kinetics of drug bind-
ing (Freire 2002; Teague 2003). The drug can be viewed as binding to
the lowest-energy state of the protein, which must undergo structural re-
arrangements in order to accommodate the drug. Due to protein dynamics,
multiple conformations of a protein are seen by a drug prior to binding
(Figure 3.7). In some cases, the drug binding can induce a substantial
conformational change due to the hydrophobic interactions between the
protein and drug. Although the overall energy of one conformation of
the protein may be at a minimum for the unbound complex, it may not
be the most favorable for drug binding, as the conformational changes
associated with drug binding can lead to a more stable complex for the
unbound conformation that has a larger energy.

Gibbs energy for an ideal gas


For an ideal gas, the change in the Gibbs energy can be directly related
to its thermodynamic parameters, such as the change in pressure. An
infinitesimal change in the Gibbs energy,dG, can be related to the enthalpy
and entropy according to dG=dH−TdS(eqn 3.19). Since the change in
enthalpy can be related to the total energy and the product of pressure
and volume (eqn 2.20), an infinitesimal change in the enthalpy,dH, is related
to the change in volume, dV, and the change in pressure, dP:

H=U+PV (3.24)

dH=dU+PdV+VdP

d(f(x)g(x)) =g(x)d(f(x)) +f(x)d(g(x))

PL

P*L

P*

ΔGobs

ΔGconvert

ΔGbarrier

P ΔGintrinsic

Protein energy profile Complex energy profile

Time

Energy

Figure 3.7
Dynamics result
in a protein having
several possible
conformations
(Pand P*) that
each has a different
overall energy. The
binding of a drug
can have different
interactions with
these conformations,
resulting in
significantly
altered energetics
for the drug–protein
complex yielding an
observed energy
change of ΔGobsfor
ligand binding.

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