Importance of Dispersion and Electron Correlation in ab Initio Protein Folding

被引:70
作者
He, Xiao
Fusti-Molnar, Laszlo
Cui, Guanglei
Merz, Kenneth M., Jr. [1 ]
机构
[1] Univ Florida, Dept Chem, Gainesville, FL 32611 USA
关键词
DENSITY-FUNCTIONAL CALCULATIONS; MOLECULAR-ORBITAL METHOD; POLARIZABLE CONTINUUM MODEL; TRANSFORM COULOMB METHOD; SOLVATION FREE-ENERGIES; ACID BASE-PAIRS; MECHANICAL METHODS; QUANTUM-CHEMISTRY; HYDROPHOBIC CORE; TRANSITION-STATE;
D O I
10.1021/jp8106952
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Dispersion is well-known to be important in biological systems, but the effect of electron correlation in such systems remains unclear. In order to assess the relationship between the structure of a protein and its electron correlation energy, we employed both full system Hartree-Fock (HF) and second-order Moller-Plesset perturbation (MP2) calculations in conjunction with the Polarizable Continuum Model (PCM) on the native structures of two proteins and their corresponding computer-generated decoy sets. Because of the expense of the MP2 calculation, we have utilized the fragment molecular orbital method (FMO) in this study. We show that the sum of the Hartree-Fock (HF) energy and force field (LJ6)-derived dispersion energy (HF + LJ6) is well correlated with the energies obtained using second-order Moller-Plesset perturbation (MP2) theory. In one of the two examples studied, the correlation energy as well as the empirical dispersive energy term was able to discriminate between native and decoy structures. On the other hand, for the second protein we studied, neither the correlation energy nor dispersion energy showed discrimination capabilities; however, the ab initio MP2 energy and the HF+LJ6 both ranked the native structure correctly. Furthermore, when we randomly scrambled the Lennard-Jones parameters, the correlation between the MP2 energy and the sum of the HF energy and dispersive energy (HF+LJ6) significantly drops, which indicates that the choice of Lennard-Jones parameters is important.
引用
收藏
页码:5290 / 5300
页数:11
相关论文
共 78 条
[1]   SPECIFIC NUCLEUS AS THE TRANSITION-STATE FOR PROTEIN-FOLDING - EVIDENCE FROM THE LATTICE MODEL [J].
ABKEVICH, VI ;
GUTIN, AM ;
SHAKHNOVICH, EI .
BIOCHEMISTRY, 1994, 33 (33) :10026-10036
[2]   INTERMOLECULAR FORCES IN SIMPLE SYSTEMS [J].
AHLRICHS, R ;
PENCO, R ;
SCOLES, G .
CHEMICAL PHYSICS, 1977, 19 (02) :119-130
[3]   A new definition of cavities for the computation of solvation free energies by the polarizable continuum model [J].
Barone, V ;
Cossi, M ;
Tomasi, J .
JOURNAL OF CHEMICAL PHYSICS, 1997, 107 (08) :3210-3221
[4]   Exchange-hole dipole moment and the dispersion interaction: High-order dispersion coefficients [J].
Becke, AD ;
Johnson, ER .
JOURNAL OF CHEMICAL PHYSICS, 2006, 124 (01)
[5]   A density-functional model of the dispersion interaction [J].
Becke, AD ;
Johnson, ER .
JOURNAL OF CHEMICAL PHYSICS, 2005, 123 (15)
[6]   ATOMIC CHARGES DERIVED FROM SEMIEMPIRICAL METHODS [J].
BESLER, BH ;
MERZ, KM ;
KOLLMAN, PA .
JOURNAL OF COMPUTATIONAL CHEMISTRY, 1990, 11 (04) :431-439
[7]   De novo prediction of three-dimensional structures for major protein families [J].
Bonneau, R ;
Strauss, CEM ;
Rohl, CA ;
Chivian, D ;
Bradley, P ;
Malmström, L ;
Robertson, T ;
Baker, D .
JOURNAL OF MOLECULAR BIOLOGY, 2002, 322 (01) :65-78
[8]   CALCULATION OF SMALL MOLECULAR INTERACTIONS BY DIFFERENCES OF SEPARATE TOTAL ENERGIES - SOME PROCEDURES WITH REDUCED ERRORS [J].
BOYS, SF ;
BERNARDI, F .
MOLECULAR PHYSICS, 1970, 19 (04) :553-&
[9]  
Branden C., 1999, INTRO PROTEIN STRUCT
[10]   The Amber biomolecular simulation programs [J].
Case, DA ;
Cheatham, TE ;
Darden, T ;
Gohlke, H ;
Luo, R ;
Merz, KM ;
Onufriev, A ;
Simmerling, C ;
Wang, B ;
Woods, RJ .
JOURNAL OF COMPUTATIONAL CHEMISTRY, 2005, 26 (16) :1668-1688