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通过单分子操作探测 F1-ATP 酶抑制态的激活和刚性。

Activation and stiffness of the inhibited states of F1-ATPase probed by single-molecule manipulation.

机构信息

ICORP ATP Synthesis Regulation Project, Japan Science and Technology Corporation, Aomi 2-3-6, Tokyo 135-0064, Japan.

出版信息

J Biol Chem. 2010 Apr 9;285(15):11411-7. doi: 10.1074/jbc.M109.099143. Epub 2010 Feb 12.

Abstract

F(1)-ATPase (F(1)), a soluble portion of F(o)F(1)-ATP synthase (F(o)F(1)), is an ATP-driven motor in which gammaepsilon subunits rotate in the alpha(3)beta(3) cylinder. Activity of F(1) and F(o)F(1) from Bacillus PS3 is attenuated by the epsilon subunit in an inhibitory extended form. In this study we observed ATP-dependent transition of epsilon in single F(1) molecules from extended form to hairpin form by fluorescence resonance energy transfer. The results justify the previous bulk experiments and ensure that fraction of F(1) with hairpin epsilon directly determines the fraction of active F(1) at any ATP concentration. Next, mechanical activation and stiffness of epsilon-inhibited F(1) were examined by the forced rotation of magnetic beads attached to gamma. Compared with ADP inhibition, which is another manner of inhibition, rotation by a larger angle was required for the activation from epsilon inhibition when the beads were forced to rotate to ATP hydrolysis direction, and more torque was required to reach the same rotation angle when beads were forced to rotate to ATP synthesis direction. The results imply that if F(o)F(1) is resting in the epsilon-inhibited state, F(o) motor must transmit to gamma a torque larger than expected from thermodynamic equilibrium to initiate ATP synthesis.

摘要

F(1)-ATP 酶(F(1))是 F(o)F(1)-ATP 合酶(F(o)F(1))的可溶性部分,是一种 ATP 驱动的马达,其中γε亚基在α(3)β(3)圆柱体中旋转。芽孢杆菌 PS3 的 F(1)和 F(o)F(1)的活性被抑制性延伸形式的ε亚基减弱。在这项研究中,我们通过荧光共振能量转移观察到单个 F(1)分子中ε亚基从延伸形式到发夹形式的 ATP 依赖性转变。结果证实了以前的批量实验,并确保具有发夹ε亚基的 F(1)的分数直接决定了任何 ATP 浓度下活性 F(1)的分数。接下来,通过附着在γ上的磁性珠的强制旋转,检查了ε抑制的 F(1)的机械激活和刚度。与 ADP 抑制(另一种抑制方式)相比,当珠粒被迫向 ATP 水解方向旋转以从ε抑制中激活时,需要更大的角度进行旋转,而当珠粒被迫向 ATP 合成方向旋转以达到相同的旋转角度时,则需要更大的扭矩。结果表明,如果 F(o)F(1)处于ε抑制状态,那么 F(o)马达必须向γ传递大于热力学平衡预期的扭矩,才能启动 ATP 合成。

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