Ptushenko Vasily V, Cherepanov Dmitry A, Krishtalik Lev I, Semenov Alexey Yu
A.N.Belozersky Institute of Physical-Chemical Biology, Moscow State University, Moscow, Russia.
Photosynth Res. 2008 Jul;97(1):55-74. doi: 10.1007/s11120-008-9309-y. Epub 2008 May 16.
The midpoint redox potentials (E(m)) of all cofactors in photosystem I from Synechococcus elongatus as well as of the iron-sulfur (Fe(4)S(4)) clusters in two soluble ferredoxins from Azotobacter vinelandii and Clostridium acidiurici were calculated within the framework of a semi-continuum dielectric approach. The widely used treatment of proteins as uniform media with single dielectric permittivity is oversimplified, particularly, because permanent charges are considered both as a source for intraprotein electric field and as a part of dielectric polarizability. Our approach overcomes this inconsistency by using two dielectric constants: optical epsilon(o)=2.5 for permanent charges pre-existing in crystal structure, and static epsilon(s) for newly formed charges. We also take into account a substantial dielectric heterogeneity of photosystem I revealed by photoelectric measurements and a liquid junction potential correction for E(m) values of relevant redox cofactors measured in aprotic solvents. We show that calculations based on a single permittivity have the discrepancy with experimental data larger than 0.7 V, whereas E(m) values calculated within our approach fall in the range of experimental estimates. The electrostatic analysis combined with quantum chemistry calculations shows that (i) the energy decrease upon chlorophyll dimerization is essential for the downhill mode of primary charge separation between the special pair P(700) and the primary acceptor A(0); (ii) the primary donor is apparently P(700) but not a pair of accessory chlorophylls; (iii) the electron transfer from the A branch quinone Q(A) to the iron-sulfur cluster F(X) is most probably downhill, whereas that from the B branch quinone Q(B) to F(X) is essentially downhill.
在半连续介质方法的框架内,计算了来自聚球藻的光系统I中所有辅因子的中点氧化还原电位(E(m)),以及来自维涅兰德固氮菌和嗜酸梭菌的两种可溶性铁氧化还原蛋白中的铁硫(Fe(4)S(4))簇的中点氧化还原电位。将蛋白质视为具有单一介电常数的均匀介质的广泛使用的处理方法过于简化,特别是因为永久电荷既被视为蛋白质内电场的来源,又被视为介电极化率的一部分。我们的方法通过使用两个介电常数来克服这种不一致性:对于晶体结构中预先存在的永久电荷,光学介电常数ε(o)=2.5,对于新形成的电荷,静态介电常数ε(s)。我们还考虑了通过光电测量揭示的光系统I的显著介电不均匀性,以及对在非质子溶剂中测量的相关氧化还原辅因子的E(m)值的液接电位校正。我们表明,基于单一介电常数的计算与实验数据的差异大于0.7V,而在我们的方法中计算的E(m)值落在实验估计范围内。静电分析与量子化学计算相结合表明:(i)叶绿素二聚化时的能量降低对于特殊对P(700)和初级受体A(0)之间的初级电荷分离的下坡模式至关重要;(ii)初级供体显然是P(700)而不是一对辅助叶绿素;(iii)从A分支醌Q(A)到铁硫簇F(X)的电子转移很可能是下坡的,而从B分支醌Q(B)到F(X)的电子转移基本上是下坡的。