Lenaz G, Fato R
J Bioenerg Biomembr. 1986 Oct;18(5):369-401. doi: 10.1007/BF00743011.
The different possible dispositions of the electron transfer components in electron transfer chains are discussed: random distribution of complexes and ubiquinone with diffusion-controlled collisions of ubiquinone with the complexes, random distribution as above, but with ubiquinone diffusion not rate-limiting, diffusion and collision of protein complexes carrying bound ubiquinone, and solid-state assembly. Discrimination among these possibilities requires knowledge of the mobility of the electron transfer chain components. The collisional frequency of ubiquinone-10 with the fluorescent probe 12-(9-anthroyl)stearate, investigated by fluorescence quenching, is 2.3 X 10(9) M-1 sec-1 corresponding to a diffusion coefficient in the range of 10(-6) cm2/sec (Fato, R., Battino, M., Degli Esposti, M., Parenti Castelli, G., and Lenaz, G., Biochemistry, 25, 3378-3390, 1986); the long-range diffusion of a short-chain polar Q derivative measured by fluorescence photobleaching recovery (FRAP) (Gupte, S., Wu, E. S., Höchli, L., Höchli, M., Jacobson, K., Sowers, A. E., and Hackenbrock, C. R., Proc. Natl. Acad. Sci. USA 81, 2606-2610, 1984) is 3 X 10(-9) cm2/sec. The discrepancy between these results is carefully scrutinized, and is mainly ascribed to the differences in diffusion ranges measured by the two techniques; it is proposed that short-range diffusion, measured by fluorescence quenching, is more meaningful for electron transfer than long-range diffusion measured by FRAP, or microcollisions, which are not sensed by either method. Calculation of the distances traveled by random walk of ubiquinone in the membrane allows a large excess of collisions per turnover of the respiratory chain. Moreover, the second-order rate constants of NADH-ubiquinone reductase and ubiquinol-cytochrome c reductase are at least three orders of magnitude lower than the second-order collisional constant calculated from the diffusion of ubiquinone. The activation energies of either the above activities or integrated electron transfer (NADH-cytochrome c reductase) are well above that for diffusion (found to be ca. 1 kcal/mol). Cholesterol incorporation in liposomes, increasing bilayer viscosity, lowers the diffusion coefficients of ubiquinone but not ubiquinol-cytochrome c reductase or succinate-cytochrome c reductase activities. The decrease of activity by ubiquinone dilution in the membrane is explained by its concentration falling below the Km of the partner enzymes. It is calculated that ubiquinone diffusion is not rate-limiting, favoring a random model of the respiratory chain organization.(ABSTRACT TRUNCATED AT 400 WORDS)
复合物和泛醌随机分布,泛醌与复合物通过扩散控制碰撞;上述随机分布,但泛醌扩散不是限速步骤;携带结合泛醌的蛋白质复合物的扩散和碰撞;以及固态组装。区分这些可能性需要了解电子传递链成分的流动性。通过荧光猝灭研究发现,泛醌 -10 与荧光探针 12-(9-蒽基)硬脂酸酯的碰撞频率为 2.3×10⁹ M⁻¹ s⁻¹,对应的扩散系数在 10⁻⁶ cm²/sec 范围内(法托,R.,巴蒂诺,M.,德格利·埃斯波西托,M.,帕伦蒂·卡斯泰利,G.,和莱纳兹,G.,《生物化学》,25,3378 - 3390,1986);通过荧光漂白恢复(FRAP)测量的短链极性 Q 衍生物的长程扩散(古普特,S.,吴,E.S.,赫克利,L.,赫克利,M.,雅各布森,K.,索尔斯,A.E.,和哈肯布罗克,C.R.,《美国国家科学院院刊》81,2606 - 2610,1984)为 3×10⁻⁹ cm²/sec。仔细审查了这些结果之间的差异,主要归因于两种技术测量的扩散范围不同;有人提出,通过荧光猝灭测量的短程扩散对于电子传递比通过 FRAP 测量的长程扩散或微碰撞更有意义,而微碰撞两种方法都无法检测到。计算泛醌在膜中随机游走的距离可知,呼吸链每一次周转会发生大量的碰撞。此外,NADH - 泛醌还原酶和泛醇 - 细胞色素 c 还原酶的二级速率常数至少比根据泛醌扩散计算出的二级碰撞常数低三个数量级。上述活性或整合电子传递(NADH - 细胞色素 c 还原酶)的活化能远高于扩散的活化能(发现约为 1 kcal/mol)。将胆固醇掺入脂质体中,增加双层膜粘度,会降低泛醌的扩散系数,但不会降低泛醇 - 细胞色素 c 还原酶或琥珀酸 - 细胞色素 c 还原酶的活性。膜中泛醌稀释导致活性降低是因为其浓度降至伴侣酶的 Km 以下。据计算,泛醌扩散不是限速步骤,这支持了呼吸链组织的随机模型。(摘要截短至 400 字)