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球形红杆菌光合反应中心二级醌受体的还原与质子化:基于野生型载色体与L亚基207和217位点携带精氨酸到异亮氨酸取代突变体比较的动力学模型

Reduction and protonation of the secondary quinone acceptor of Rhodobacter sphaeroides photosynthetic reaction center: kinetic model based on a comparison of wild-type chromatophores with mutants carrying Arg-->Ile substitution at sites 207 and 217 in the L-subunit.

作者信息

Cherepanov D A, Bibikov S I, Bibikova M V, Bloch D A, Drachev L A, Gopta O A, Oesterhelt D, Semenov A Y, Mulkidjanian A Y

机构信息

Institute of Electrochemistry, Russian Academy of Sciences, Moscow.

出版信息

Biochim Biophys Acta. 2000 Jul 20;1459(1):10-34. doi: 10.1016/s0005-2728(00)00110-9.

Abstract

After the light-induced charge separation in the photosynthetic reaction center (RC) of Rhodobacter sphaeroides, the electron reaches, via the tightly bound ubiquinone QA, the loosely bound ubiquinone Q(B) After two subsequent flashes of light, Q(B) is reduced to ubiquinol Q(B)H2, with a semiquinone anion Q-(B) formed as an intermediate after the first flash. We studied Q(B)H2 formation in chromatophores from Rb. sphaeroides mutants that carried Arg-->Ile substitution at sites 207 and 217 in the L-subunit. While Arg-L207 is 17 A away from Q(B), Arg-L217 is closer (9 A) and contacts the Q(B)-binding pocket. From the pH dependence of the charge recombination in the RC after the first flash, we estimated deltaG(AB), the free energy difference between the Q-(A)Q(B) and Q(A)Q-(B) states, and pK212, the apparent pK of Glu-L212, a residue that is only 4 A away from Q(B). As expected, the replacement of positively charged arginines by neutral isoleucines destabilized the Q-(B) state in the L217RI mutant to a larger extent than in the L207RI one. Also as expected, pK212 increased by approximately 0.4 pH units in the L207RI mutant. The value of pK212 in the L217RI mutant decreased by 0.3 pH units, contrary to expectations. The rate of the Q-(A)Q-(B)-->Q(A)Q(B)H2 transition upon the second flash, as monitored by electrometry via the accompanying changes in the membrane potential, was two times faster in the L207RI mutant than in the wild-type, but remained essentially unchanged in the L217RI mutant. To rationalize these findings, we developed and analyzed a kinetic model of the Q-(A)Q-(B)-->Q(A)Q(B)H2 transition. The model properly described the available experimental data and provided a set of quantitative kinetic and thermodynamic parameters of the Q(B) turnover. The non-electrostatic, 'chemical' affinity of the QB site to protons proved to be as important for the attracting protons from the bulk, as the appropriate electrostatic potential. The mutation-caused changes in the chemical proton affinity could be estimated from the difference between the experimentally established pK2J2 shifts and the expected changes in the electrostatic potential at Glu-L212, calculable from the X-ray structure of the RC. Based on functional studies, structural data and kinetic modeling, we suggest a mechanistic scheme of the QB turnover. The detachment of the formed ubiquinol from its proximal position next to Glu-L212 is considered as the rate-limiting step of the reaction cycle.

摘要

在球形红细菌光合反应中心(RC)发生光诱导电荷分离后,电子通过紧密结合的泛醌QA到达松散结合的泛醌QB。在随后的两次闪光后,QB被还原为泛醇QBH2,第一次闪光后会形成半醌阴离子Q-(B)作为中间体。我们研究了球形红细菌L亚基中207和217位点发生精氨酸→异亮氨酸取代的突变体的类囊体中QBH2的形成。虽然精氨酸-L207距离QB为17 Å,但精氨酸-L217更近(9 Å)并与QB结合口袋接触。根据第一次闪光后RC中电荷复合的pH依赖性,我们估算了ΔG(AB),即Q-(A)Q(B)和Q(A)Q-(B)状态之间的自由能差,以及pK212,即谷氨酸-L212的表观pK值,该残基距离QB仅4 Å。正如预期的那样,L217RI突变体中带正电的精氨酸被中性异亮氨酸取代比L207RI突变体更大程度地使Q-(B)状态不稳定。同样如预期的那样,L207RI突变体中pK212增加了约0.4个pH单位。与预期相反,L217RI突变体中pK212的值下降了0.3个pH单位。通过膜电位的伴随变化用电位法监测,第二次闪光时Q-(A)Q-(B)→Q(A)Q(B)H2转变的速率在L207RI突变体中比野生型快两倍,但在L217RI突变体中基本保持不变。为了解释这些发现,我们开发并分析了Q-(A)Q-(B)→Q(A)Q(B)H2转变的动力学模型。该模型恰当地描述了可用的实验数据,并提供了一组QB周转的定量动力学和热力学参数。事实证明,QB位点对质子的非静电“化学”亲和力对于从本体吸引质子与适当的静电势同样重要。化学质子亲和力的突变引起的变化可以从实验确定的pK2J2位移与RC的X射线结构计算出的谷氨酸-L212处静电势的预期变化之间的差异来估算。基于功能研究、结构数据和动力学建模,我们提出了QB周转的机制方案。形成的泛醇从其紧邻谷氨酸-L212的近端位置脱离被认为是反应循环的限速步骤。

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