Shin Yeung-gyo K, Newton Marshall D, Isied Stephan S
Department of Chemistry, Rutgers, the State University of New Jersey, Piscataway 08855, USA.
J Am Chem Soc. 2003 Apr 2;125(13):3722-32. doi: 10.1021/ja020358q.
The charge-transfer transition energies and the electronic-coupling matrix element, |H(DA)|, for electron transfer from aminopyridine (ap) to the 4-carbonyl-2,2'-bipyridine (cbpy) in cbpy-(gly)(n)-ap (gly = glycine, n = 0-6) molecules were calculated using the Zerner's INDO/S, together with the Cave and Newton methods. The oligopeptide linkages used were those of the idealized protein secondary structures, the alpha-helix, 3(10)-helix, beta-strand, and polyproline I- and II-helices. The charge-transfer transition energies are influenced by the magnitude and direction of the dipole generated by the peptide secondary structure. The electronic coupling |H(DA)| between (cbpy) and (ap) is also dependent on the nature of the secondary structure of the peptide. A plot of 2.ln|H(DA)| versus the charge-transfer distance (assumed to be the dipole moment change between the ground state and the charge-transfer states) showed that the polyproline II structure is a more efficient bridge for long-distance electron-transfer reactions (beta = 0.7 A(-1)) than the other secondary structures (beta approximately 1.3 A(-1)). Similar calculations on charged dipeptide derivatives, CH(3)CONHCH(2)CONHCH(3)(-), showed that peptide-peptide interaction is more dependent on conformation in the cationic than in the anionic dipeptides. The alpha-helix and polyproline II-helix both have large peptide-peptide interactions (|H(DA)| > 800 cm(-1)) which arise from the angular dependence of their pi-orbitals. Such an interaction is much weaker than in the beta-strand peptides. These combined results were found to be consistent with electron-transfer rates experimentally observed across short peptide bridges in polyproline II (n = 1-3). These results can also account for directional electron transfer observed in an alpha-helical structure (different ET rates versus the direction of the molecular dipole).
使用泽纳的INDO/S方法以及凯夫和牛顿方法,计算了cbpy-(gly)(n)-ap(gly = 甘氨酸,n = 0 - 6)分子中从氨基吡啶(ap)到4-羰基-2,2'-联吡啶(cbpy)的电荷转移跃迁能量和电子耦合矩阵元|H(DA)|。所使用的寡肽连接是理想化蛋白质二级结构的连接,即α-螺旋、3(10)-螺旋、β-链以及聚脯氨酸I型和II型螺旋。电荷转移跃迁能量受肽二级结构产生的偶极子大小和方向的影响。(cbpy)和(ap)之间的电子耦合|H(DA)|也取决于肽二级结构的性质。2.ln|H(DA)|与电荷转移距离(假定为基态和电荷转移态之间的偶极矩变化)的关系图表明,聚脯氨酸II型结构对于长距离电子转移反应(β = 0.7 Å⁻¹)是比其他二级结构(β约为1.3 Å⁻¹)更有效的桥梁。对带电二肽衍生物CH₃CONHCH₂CONHCH₃的类似计算表明,肽 - 肽相互作用在阳离子二肽中比在阴离子二肽中更依赖于构象。α-螺旋和聚脯氨酸II型螺旋都具有较大的肽 - 肽相互作用(|H(DA)| > 800 cm⁻¹),这源于它们π轨道的角度依赖性。这种相互作用比β-链肽中的要弱得多。发现这些综合结果与在聚脯氨酸II(n = 1 - 3)中短肽桥的实验观察到的电子转移速率一致。这些结果也可以解释在α-螺旋结构中观察到的定向电子转移(不同的电子转移速率与分子偶极子方向有关)。