Pyrazole Derivatives
Journal of Medicinal Chemistry, 2005, Vol. 48, No. 23 7121
as receptor models. This was performed with the force field
AMBER* united atom notation and GB/SA water implicit
model of solvation as implemented in MacroModel, version
7.2.25
distance between the ligand centers of mass and the FAD N5
atom. A longer simulation up to 20 ps revealed no significant
changes in this geometrical descriptor after 2 ps in all
complexes.
All calculations were done by a Linux cluster of 5 Intel Xeon
dual processors at 3.2 GHz with 2 Gb of RAM. Graphic
manipulations and analysis of the docking experiments were
performed by the Maestro Graphical User Interface, version
4.1.012, for Linux operating systems.25 Jmol, version 10, was
used for creating Figures 2 and 3.39
The MOLINE computational approach required as receptor
and ligand input data, respectively, the pretreated enzyme
models and the two conformations obtained in the MC search
of the inhibitors. The docking experiments were carried out
with the same AMBER* united atom force field considered in
the simulations above. According to a recently reported22
similar case study, both the MOLINE grid resolution GR and
the van der Waals compression factor ø were systematically
varied. Two different dielectric constants respectively fixed at
4 (to mimic conditions similar to an “average” protein medium)
and 80 (water environment) were tried in the docking experi-
ments.
According to the GLIDE24 approach, both pretreated enzyme
models were submitted to map calculations using a box of
about 110 000 Å3 centered on the FAD N5 atom. Flexible
docking of the four ligands was done by generating a maximum
number of 1000 configurations, saving the 10 lowest energy
ones and submitting them to the multiminimization proce-
dures as follows. We considered the MMFF, AMBER* united
atoms and all-atom force fields. OPLS* did not work for
missing parameters related to the FAD phosphate moiety. For
solvation models, we considered two different dielectric con-
stants and the water implicit GB/SA solvation model.25 Three
different constraint conditions were systematically studied:
full relaxing (no constraints), protein backbone fixed with a
200 kJ mol-1 Å-1 force constant on each atom, and a shell of
free atoms up to 15 Å from the FAD N5 with the remaining
atoms kept constrained as above. The interaction energy of
all complexes was computed according to the MOLINE method23
and converted to average state equations. Globally, 8 × 10 ×
3 × 3 × 3 ) 2160 conformations were energy-minimized at
the above conditions.
Molecular interaction fields required by the GLUE program
were precalculated by GRID using the standard probes OH2
and H. Specific probes related to the chemical structures of 1
and 4 were C3, C1d, N2, N:d, F, CL, and O. This last probe
was used to mimic the thiourea S atom, not available in the
GLUE probe list. In the generation of the GRID maps, a cube
box of 10 000 Å3 was centered on the FAD N5 atom using the
original PDB models without their covalent ligands. The
flexibility of the inhibitors was considered, allowing free
rotations of all rotatable bonds of compounds 1 and 4. The
lowest interaction energy configurations of each complex were
submitted to GROMACS calculations.
The force field considered in the GROMACS calculations
was the ffgmx force field with the SPC explicit model of
solvation.34 GROMACS specific modules editconf and genbox
were used to add water molecules within a box edge of
minimum 10 Å from the enzyme complex. The module genion
allowed the neutralization of the models by adding three Cl-
and four Na+ counterions to the MAO-A and MAO-B com-
plexes, respectively. The PRODRG service tool available on
the Internet was used for a quick setup of the non-protein
section of the eight complexes.35 Preliminary minimization was
done using 500 iterations of the steepest descents algorithm
with an energy convergence criterion fixed at 1000 kJ mol-1
nm-1. The particle mesh Ewald (PME) method was used to
treat the electrostatic term.36 Dynamic conformational assess-
ment of non-protein atoms was carried out by Berendsen’s
temperature and pressure coupling method37 for 2 ps at 300
K with a time step of 2 fs. The linear constraints solver
algorithm (LINCS) was adopted for all atoms, preventing bond
distortions as suggested for time steps larger than 1 fs.38 The
g_lie GROMACS utility was used to estimate the free-binding
interaction energy of each enzyme-inhibitor complex (FBIE)
using final conformations of the 2 ps molecular dynamics run.
Theoretical affinity constants (tKa) were derived according to
the equation RT ln tKa ) FBIE, where R is the gas constant
and T the room temperature set to 300 K. The same conforma-
tions were submitted to geometrical analysis considering the
Acknowledgment. This work was supported by
grants from MURST. We also acknowledge Mr. Anton
Gerada, a professional translator and Fellow of the
Institute of Translation and Interpreting of London and
Member of AIIC (Association Internationale des Inter-
preˆtes de Confe´rences, Geneva), for the revision of the
manuscript.
Supporting Information Available: 1H NMR, IR spec-
tral data, and elemental analysis results of derivatives 1-10.
This material is available free of charge via the Internet at
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