MERCK MOLECULAR-FORCE FIELD .4. CONFORMATIONAL ENERGIES AND GEOMETRIES FOR MMFF94

Citation
Ta. Halgren et Rb. Nachbar, MERCK MOLECULAR-FORCE FIELD .4. CONFORMATIONAL ENERGIES AND GEOMETRIES FOR MMFF94, Journal of computational chemistry, 17(5-6), 1996, pp. 587-615
Citations number
76
Categorie Soggetti
Chemistry
ISSN journal
01928651
Volume
17
Issue
5-6
Year of publication
1996
Pages
587 - 615
Database
ISI
SICI code
0192-8651(1996)17:5-6<587:MMF.CE>2.0.ZU;2-Y
Abstract
This article describes the parameterization and performance of MMFF94 for conformational energies, rotational barriers, and equilibrium tors ion angles. It describes the derivation of the torsion parameters from high-quality computational data and characterizes MMFF94's ability to reproduce both computational and experimental data, the latter partic ularly in relation to MM3. The computational data included: (i) simila r to 250 comparisons of conformational energy based on ''MP4SDQ/TZP'' calculations (triple-zeta plus polarization calculations at a defined approximation to the highly correlated MP4SDQ level) at MP2/6-31G geo metries; and (ii) similar to 1200 MP2/TZP comparisons of ''torsion pro file'' structures at geometries derived from MP2/6-31G geometries. Th e torsion parameters were derived in restrained least-squares fits tha t used the complete set of available computational data, thereby ensur ing that a fully optimal set of parameters would be obtained. The fina l parameters reproduce the ''MP4SDQ/TZP'' and MP2/TZP computational da ta with root mean square (rms) deviations of 0.31 and 0.50 kcal/mol, r espectively. In addition, MMFF94 reproduces a set of 37 experimental g as-phase and solution conformational energies, enthalpies, and free en ergies with a rms deviation of 0.38 kcal/mol; for comparison, the ''MP 4SDQ/TZP'' calculations and MM3 each gives a rms deviation of 0.37 kca l/mol. Furthermore, MMFF94 reproduces 28 experimentally determined rot ational barriers with a rms deviation of 0.39 kcal/mol. Given the dive rse nature of the experimental conformational energies and rotational barriers and the clear indications of experimental error in some cases , the MMFF94 results appear excellent. Nevertheless, MMFF94 encounters somewhat greater difficulty in handling multifunctional compounds tha t place highly polar functional groups in close proximity, probably be cause it, like other commonly used force fields, too greatly simplifie s the description of electrostatic interactions. Some suggestions for enhancements to MMFF94's functional form are discussed. (C) 1996 by Jo hn Wiley & Sons, Inc.