Chiang Chien-Sung, Anishkin Andriy, Sukharev Sergei
Department of Biology, University of Maryland College Park, Maryland 20742, USA.
Biophys J. 2004 May;86(5):2846-61. doi: 10.1016/S0006-3495(04)74337-4.
Physical expansion associated with the opening of a tension-sensitive channel has the same meaning as gating charge for a voltage-gated channel. Despite increasing evidence for the open-state conformation of MscL, the energetic description of its complex gating remains incomplete. The previously estimated in-plane expansion of MscL is considerably smaller than predicted by molecular models. To resolve this discrepancy, we conducted a systematic study of currents and dose-response curves for wild-type MscL in Escherichia coli giant spheroplasts. Using the all-point histogram method and calibrating tension against the threshold for the small mechanosensitive channel (MscS) in each patch, we found that the distribution of channels among the subconducting states is significantly less dependent on tension than the distribution between the closed and conducting states. At -20 mV, all substates together occupy approximately 30% of the open time and reduce the mean integral current by approximately 6%, essentially independent of tension or P(o). This is consistent with the gating scheme in which the major rate-limiting step is the transition between the closed state and a low-conducting substate, and validates both the use of the integral current as a measure of P(o), and treatment of dose-response curves in the two-state approximation. The apparent energy and area differences between the states deltaE and deltaA, extracted from 29 independent dose-response curves, varied in a linearly correlated manner whereas the midpoint tension stayed at approximately 10.4 mN/m. Statistical modeling suggests slight variability of gating parameters among channels in each patch, causing a strong reduction and correlated spread of apparent deltaE and deltaA. The slope of initial parts of activation curves, with a few channels being active, gave estimates of deltaE = 51 +/- 13 kT and deltaA = 20.4 +/- 4.8 nm(2), the latter being consistent with structural models of MscL, which predict deltaA = 23 nm(2).
与张力敏感通道开放相关的物理扩张与电压门控通道的门控电荷具有相同的意义。尽管有越来越多的证据支持MscL的开放状态构象,但其复杂门控的能量描述仍不完整。先前估计的MscL平面内扩张比分子模型预测的要小得多。为了解决这一差异,我们对大肠杆菌原生质球中野生型MscL的电流和剂量反应曲线进行了系统研究。使用全点直方图方法并根据每个膜片中的小机械敏感通道(MscS)的阈值校准张力,我们发现亚导通状态之间通道的分布对比导通状态和关闭状态之间的分布对张力的依赖性要小得多。在-20 mV时,所有亚状态一起占据开放时间的约30%,并使平均积分电流降低约6%,基本上与张力或P(o)无关。这与门控方案一致,其中主要的限速步骤是关闭状态和低导通亚状态之间的转变,并验证了使用积分电流作为P(o)的度量以及在双态近似中处理剂量反应曲线的方法。从29条独立的剂量反应曲线中提取的状态之间的表观能量和面积差异deltaE和deltaA以线性相关的方式变化,而中点张力保持在约10.4 mN/m。统计建模表明每个膜片中通道之间门控参数存在轻微变化,导致表观deltaE和deltaA大幅降低并相关扩散。激活曲线初始部分的斜率,有少数通道处于活跃状态,得出deltaE = 51 +/- 13 kT和deltaA = 20.4 +/- 4.8 nm(2)的估计值,后者与预测deltaA = 23 nm(2)的MscL结构模型一致。