Ha. Carlson et al., Method for including the dynamic fluctuations of a protein in computer-aided drug design, J PHYS CH A, 103(49), 1999, pp. 10213-10219
We have recently presented a new pharmacophore design method that allows fo
r the incorporation of the inherent flexibility of a target active site. Th
e flexibility of the enzymatic system is described by collecting many confo
rmations of the uncomplexed protein: this ensemble of conformational states
can come from a molecular dynamics (MD) simulation, multiple crystal struc
tures, or many NMR structures. Binding sites for functional groups that com
plement the active site are determined throu,oh multiple-copy calculations.
These calculations are conducted for each protein conformation, providing
a large collection of potential binding sites. The Cartesian coordinates fr
om each protein conformation are overlaid through RMS fitting of essential
catalytic residues, and the pharmacophore model is described by binding reg
ions that are conserved over many protein conformations. Previously, we dev
eloped a "dynamic" pharmacophore model for HIV-1 integrase using 11 conform
ations of the protein from an MD simulation; the MUSIC procedure was used t
o calculate binding positions for methanol molecules in each configuration
of the active site. Here we present "static" pharmacophore models developed
with a single conformation of the protein from two new crystal structures
(standard protocol for multiple-copy methods). The static models do not per
form as well as the previous dynamic model in fitting known inhibitors of H
IV-1 intergrase. To test the applicability of the dynamic pharmacophore met
hod and the assumption that any reliable source of protein conformations is
applicable, we have now developed a second dynamic pharmacophore model bas
ed on the two crystal structures also used for the development of the stati
c models. Though the dynamic model based on the two crystal structures does
not fit as many known inhibitors as the previous: dynamic model, it is a s
ignificant improvement over the static models. Even better performance is e
xpected with the addition of new crystal structures as they become availabl
e. However, it is notable that using only two structures leads to great imp
rovement in the models.