MD simulations
the energetic interactions of the two enantiomers of the same
ligand into the receptor, we took only the first three terms of eqn
(1) into account, considering the entropic value as approximately
constant.
All simulations were performed using AMBER 10.39 The five com-
plexes (four (R)-4-A1AR and one (S)-4-A1AR systems) were em-
bedded into a phospholipid bilayer made up of POPC molecules.
The creation of the phospholipid bilayer and the insertion of the
receptor-ligand complexes were carried out using VMD.40 MD
simulations were carried out using the modified parm94 force field
at 300 K. An explicit solvent model of TIP3P water was used. The
system was solvated on the “extracellular” and “intracellular” side
Acknowledgements
National Interest Research Projects (PRIN_2008_5HR5JK) is
gratefully acknowledged.
˚
with a 12 A water cap. Chlorine ions were added as counterions
to neutralize the system. Prior to MD simulations, three steps of
energy minimization were carried out. In the first stage, we kept
References
1 K. A. Jacobson, P. J. van Galen and M. Williams, J. Med. Chem., 1992,
35, 407–422.
the protein and phospholipids fixed with a position restraint of
-2
100 kcal mol-1
and we just energy minimized the positions
˚
A
2 J. W. Daly, J. Med. Chem., 1982, 25, 197–207.
of the water molecules. In the second stage, we energy minimized
the phospholipid–water system, applying a position restraint of
3 S. A. Poulsen and R. J. Quinn, Bioorg. Med. Chem., 1998, 6, 619–641.
4 S. Schenone, C. Brullo, F. Musumeci, O. Bruno and M. Botta, Curr.
Top. Med. Chem., 2010, 10, 878–901.
5 P. S. Modlinger and W. J. Welch, Curr. Opin. Nephrol. Hypertens., 2003,
12, 497–502.
-2
100 kcal mol-1
A
on the protein. Finally, we applied a restraint
only on the a carbons of the receptor. The
˚
of 30 kcal mol-1
-2
˚
A
three energy minimization stages consisted of 10 000 steps. The
first 1000 steps were Steepest Descent, and the last 9000 were
Conjugate Gradient. Molecular dynamics trajectories were run
using the energy minimized structure as the input, and particle
mesh Ewald electrostatics41 and periodic boundary conditions
were used in the simulation. The time step of the simulations
6 R. H. Shah and W. H. Frishman, Cardiol. Rev., 2009, 17, 125–131.
7 C. N. Wilson, A. Nadeem, D. Spina, R. Brown, C. P. Page and S. J.
Mustafa, Handb. Exp. Pharmacol., 2009, 193, 329–362.
8 T. Maemoto, M. Tada, T. Mihara, N. Ueyama, H. Matsuoka, K.
Harada, T. Yamaji, K. Shirakawa, S. Kuroda, A. Akahane, A. Iwashita,
N. Matsuoka and S. Mutoh, J. Pharmacol. Sci., 2004, 96, 42–52.
9 J. Trevitt, C. Vallance, A. Harris and T. Goode, Pharmacol., Biochem.
Behav., 2009, 92, 521–527.
10 F. Manetti, S. Schenone, F. Bondavalli, C. Brullo, O. Bruno, A. Ranise,
L. Mosti, G. Menozzi, P. Fossa, M. L. Trincavelli, C. Martini, A.
Martinelli, C. Tintori and M. Botta, J. Med. Chem., 2005, 48, 7172–
7185.
˚
was 2.0 fs with a cutoff of 12 A for the non-bonded interaction.
SHAKE was employed to keep all bonds involving hydrogen
atoms rigid. A constant-volume was carried out for 200 ps, during
which time the temperature was raised from 0 to 300 K (using the
Langevin dynamics method). Then, 4800 ps of constant-pressure
MD were carried out at 300 K. In the first 400 ps, all of the
a carbons of the receptor were blocked with a harmonic force
11 T. Tuccinardi, S. Schenone, F. Bondavalli, C. Brullo, O. Bruno, L. Mosti,
A. T. Zizzari, C. Tintori, F. Manetti, O. Ciampi, M. L. Trincavelli, C.
Martini, A. Martinelli and M. Botta, ChemMedChem, 2008, 3, 898–
913.
12 F. Da Settimo, G. Primofiore, C. La Motta, S. Taliani, F. Simorini, A.
M. Marini, L. Mugnaini, A. Lavecchia, E. Novellino, D. Tuscano and
C. Martini, J. Med. Chem., 2005, 48, 5162–5174.
constant. This was decreased during the 400 ps from 10 to 1 kcal
-1
mol-1 A . In the last 4400 ps, there were no constraints. The final
˚
structure was obtained as the average of the last 4400 ps of MD
13 R. K. Kondru, P. Wipf and D. N. Beratan, Science, 1998, 282, 2247–
2250.
energy minimized with the CG method until a convergence of 0.05
14 R. K. Kondru, P. Wipf and D. N. Beratan, J. Phys. Chem. A, 1999, 103,
6603–6611.
-1
˚
A
kcal mol-1
was reached. The backbone conformation of the
resulting receptor structure was evaluated by inspection of the y/f
Ramachandran plot obtained from PROCHECK analysis.23 The
General Amber Force Field (GAFF) parameters were assigned to
POPC molecules. The partial charges were calculated using the
AM1-BCC method, as implemented in the Antechamber suite of
AMBER 10.
15 P. L. Polavarapu, Chirality, 2002, 14, 768–781.
16 V. P. Jaakola, M. T. Griffith, M. A. Hanson, V. Cherezov, E. Y. Chien,
J. R. Lane, A. P. Ijzerman and R. C. Stevens, Science, 2008, 322, 1211–
1217.
17 R. E. Stenkamp, Acta Crystallogr., Sect. D: Biol. Crystallogr., 2008,
D64, 902–904.
18 V. Cherezov, D. M. Rosenbaum, M. A. Hanson, S. G. Rasmussen, F.
S. Thian, T. S. Kobilka, H. J. Choi, P. Kuhn, W. I. Weis, B. K. Kobilka
and R. C. Stevens, Science, 2007, 318, 1258–1265.
19 T. Warne, M. J. Serrano-Vega, J. G. Baker, R. Moukhametzianov, P. C.
Edwards, R. Henderson, A. G. Leslie, C. G. Tate and G. F. Schertler,
Nature, 2008, 454, 486–491.
Energy evaluation
We extracted from the last 4400 ps of MD of the ligand–receptor
complexes, 88 snapshots (at time intervals of 50 ps) for each species
(complex, receptor and ligand). The various MM-PBSA energy
terms in equation 1 were computed as follows.
20 H. M. Berman, J. Westbrook, Z. Feng, G. Gilliland, T. N. Bhat, H.
Weissig, I. N. Shindyalov and P. E. Bourne, Nucleic Acids Res., 2000,
28, 235–242.
21 A. Martinelli and T. Tuccinardi, Expert Opin. Drug Discovery, 2006, 1,
459–476.
22 A. Fiser, R. K. Do and A. Sali, Protein Sci., 2000, 9, 1753–1773.
23 R. A. Laskowski, M. W. Macarthur, D. S. Moss and J. M. Thornton,
J. Appl. Crystallogr., 1993, 26, 283–291.
(1)
G = Gpolar + Gnonpolar + Emm - TS
Electrostatic, van der Waals and internal energies (Emm) were
obtained using the SANDER module in AMBER 10. Polar
energies (Gpolar) were obtained from the PBSA module of the
AMBER 10 program (using the Poisson–Boltzman method)
applying dielectric constants of 1 and 80 to represent the gas
and water phases, respectively. Nonpolar energies (Gnonpolar) were
determined using the MOLSURF program. In order to compare
24 M. L. Verdonk, J. C. Cole, M. J. Hartshorn, C. W. Murray and R. D.
Taylor, Proteins: Struct., Funct., Bioinf., 2003, 52, 609–623.
25 P. A. Kollman, I. Massova, C. Reyes, B. Kuhn, S. Huo, L. Chong, M.
Lee, T. Lee, Y. Duan, W. Wang, O. Donini, P. Cieplak, J. Srinivasan, D.
A. Case and T. E. Cheatham, 3rd, Acc. Chem. Res., 2000, 33, 889–897.
26 T. Tuccinardi, S. Bertini, A. Martinelli, F. Minutolo, G. Ortore, G. Pla-
canica, G. Prota, S. Rapposelli, K. E. Carlson, J. A. Katzenellenbogen
and M. Macchia, J. Med. Chem., 2006, 49, 5001–5012.
4454 | Org. Biomol. Chem., 2011, 9, 4448–4455
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