MINIMIZATION OF POLYPEPTIDE ENERGY .I. PRELIMINARY STRUCTURES OF BOVINE PANCREATIC RIBONUCLEASE S-PEPTIDE
MINIMIZATION OF POLYPEPTIDE ENERGY .I. PRELIMINARY STRUCTURES OF BOVINE PANCREATIC RIBONUCLEASE S-PEPTIDE
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DOI:
10.1073/pnas.58.2.420
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发表时间:
1967-01-01
影响因子:
11.1
通讯作者:
SCHERAGA, HA
中科院分区:
文献类型:
--
作者:
GIBSON, KD;SCHERAGA, HA
UNB= a b UHf () A (1 r 2 r6 r6 The coefficient UH of the attractive term was calculated by sum-ning all the re-maining electrostatic and nonbonded energy contributions of the pair of atoms in-volved in the bond, and requiring that the distance between the hydrogen atom and the acceptor atom be 1.85 A when UNB is a minimum (with f (0) set equal to 1). This procedure appeared to give reasonable values for UNB at the minimum; however, it is difficult to make a valid comparison with experimental results, since the latter always include many interactions between atoms not taken into account in the calculation of UH. Angular dependence was introduced through the function f (0), where0 for 00< 0< 1350 f (0)=(2) cos4 20for 1350< 0< 1800 and 0 is the angle between the vectors AH and B... H, with A being the donor atom and B the acceptor atom. For a linear hydrogenbond, 0= 1800. This function is equal to 1.0 when the bond is linear and falls off rapidly to zero as the bond departs from linearity. No accountwas taken of possible angulardependence involving the orientation around the acceptor atom. The hydrogen bond and 6-12 potentials become negligible at interatomic distances of more than a few angstroms. The electrostatic energies fall off more slowly with distance; but since a sufficiently large separation of the atoms allows solvent molecules (in this case water, with a dielectric constant of about 80) to