Hydrogen bonding and spin density distribution in the Qb semiquinone of bacterial reaction centers and comparison with the Qa site.
Hydrogen bonding and spin density distribution in the Qb semiquinone of bacterial reaction centers and comparison with the Qa site.
复制标题
细菌反应中心Qb半醌的氢键和自旋密度分布以及与Qa位点的比较。
DOI:
10.1021/ja2001538
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发表时间:
2011
影响因子:
15
通讯作者:
Dikanov,SergeiA
中科院分区:
文献类型:
--
作者:
Martin,Erik;Samoilova,RimmaI;Narasimhulu,KupalaV;Lin,Tzu-Jen;O'Malley,PatrickJ;Wraight,ColinA;Dikanov,SergeiA
In the photosynthetic reaction center fromRhodobacter sphaeroides, the primary (QA) and secondary (QB) electron acceptors are both ubiquinone-10, but with very different properties and functions. To investigate the protein environment that imparts these functional differences, we have applied X-band HYSCORE, a 2D pulsed EPR technique, to characterize the exchangeable protons around the semiquinone (SQ) in the QAand QBsites, using samples of15N-labeled reaction centers, with the native high spin Fe2+exchanged for diamagnetic Zn2+, prepared in1H2O and2H2O solvent. The powder HYSCORE method is first validated against the orientation-selected Q-band ENDOR study of the QASQ by Flores et al. (Biophys. J.2007,92, 671−682), with good agreement for two exchangeable protons with anisotropic hyperfine tensor components,T, both in the range 4.6−5.4 MHz. HYSCORE was then applied to the QBSQ where we found proton lines corresponding toT ≈5.2, 3.7 MHz andT≈ 1.9 MHz. Density functional-based quantum mechanics/molecular mechanics (QM/MM) calculations, employing a model of the QBsite, were used to assign the observed couplings to specific hydrogen bonding interactions with the QBSQ. These calculations allow us to assign theT= 5.2 MHz proton to the His-L190 NδH···O4(carbonyl) hydrogen bonding interaction. TheT= 3.7 MHz spectral feature most likely results from hydrogen bonding interactions of O1 (carbonyl) with both Gly-L225 peptide NH and Ser-L223 hydroxyl OH, which possess calculated couplings very close to this value. The smaller 1.9 MHz coupling is assigned to a weakly bound peptide NH proton of Ile-L224. The calculations performed with this structural model of the QBsite show less asymmetric distribution of unpaired spin density over the SQ than seen for the QAsite, consistent with available experimental data for13C and17O carbonyl hyperfine couplings. The implications of these interactions for QBfunction and comparisons with the QAsite are discussed.