Yuji. Kato, T. Fujiwara, Y. Komeiji, T. Nakano, H. Mori, Yoshio Okiyama, Y. Mochizuki
{"title":"Fragment molecular orbital−based molecular dynamics (FMO-MD) simulations on hydrated Cu(II) ion","authors":"Yuji. Kato, T. Fujiwara, Y. Komeiji, T. Nakano, H. Mori, Yoshio Okiyama, Y. Mochizuki","doi":"10.1273/CBIJ.14.1","DOIUrl":null,"url":null,"abstract":"A simulation protocol based on fragment molecular orbital−based molecular dynamics (FMO-MD) was applied to a droplet model consisting of a divalent copper ion and 64 water molecules. The total energy and forces were evaluated at the unrestricted Hartree-Fock (UHF) level with three-body fragment correction (FMO3). Two MD runs were performed: one with a six-coordination setting and the other with a five-coordination setting in the first hydration shell. Both runs resulted in the main peak position of the Cu-O radial distribution function at 2.02 Å, in reasonable agreement with the experimental data. The O-Cu-O angular distribution function showed different characteristics between the two cases.","PeriodicalId":40659,"journal":{"name":"Chem-Bio Informatics Journal","volume":"2021 1","pages":"1-13"},"PeriodicalIF":0.4000,"publicationDate":"2014-07-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Chem-Bio Informatics Journal","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1273/CBIJ.14.1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"BIOCHEMISTRY & MOLECULAR BIOLOGY","Score":null,"Total":0}
引用次数: 4
Abstract
A simulation protocol based on fragment molecular orbital−based molecular dynamics (FMO-MD) was applied to a droplet model consisting of a divalent copper ion and 64 water molecules. The total energy and forces were evaluated at the unrestricted Hartree-Fock (UHF) level with three-body fragment correction (FMO3). Two MD runs were performed: one with a six-coordination setting and the other with a five-coordination setting in the first hydration shell. Both runs resulted in the main peak position of the Cu-O radial distribution function at 2.02 Å, in reasonable agreement with the experimental data. The O-Cu-O angular distribution function showed different characteristics between the two cases.