Bukauskas F F, Elfgang C, Willecke K, Weingart R
Physiologisches Institut, Universität Bern, Switzerland.
Biophys J. 1995 Jun;68(6):2289-98. doi: 10.1016/S0006-3495(95)80411-X.
A clone of human HeLa cells stably transfected with mouse connexin40 DNA was used to examine gap junctions. Two separate cells were brought into physical contact with each other ("induced cell pair") to allow insertion of gap junction channels and, hence, formation of a gap junction. The intercellular current flow was measured with a dual voltage-clamp method. This approach enabled us to study the electrical properties of gap junction channels (cell pairs with a single channel) and gap junctions (cell pairs with many channels). We found that single channels exhibited multiple conductances, a main state (gamma j(main state)), several substates (gamma j(substates)), a residual state (gamma j (residual state)), and a closed state (gamma j(closed state)). The gamma j(main state) was 198 pS, and gamma j(residual state) was 36 pS (temperature, 36-37 degrees C; pipette solution, potassium aspartate). Both properties were insensitive to transjunctional voltage, Vj. The transitions between the closed state and an open state (i.e., residual state, substate, or main state) were slow (15-45 ms); those between the residual state and a substate or the main state were fast (1-2 ms). Under steady-state conditions, the open channel probability, Po, decreased in a sigmoidal manner from 1 to 0 (Boltzmann fit: Vj,o = -44 mV; z = 6). The temperature coefficient, Q10, for gamma j(main state) and gamma j(residual state) was 1.2 and 1.3, respectively (p < 0.001; range 15-40 degrees C). This difference suggests interactions between ions and channel structure in case of gamma j(residual state). In cell pairs with many channels, the gap junction conductance at steady state, gj, exhibited a bell-shaped dependency from Vj (Boltzmann fit, negative Vj, Vj,o = -45 mV, gj(min) = 0.24; positive Vj, Vj,o = 49 mV, gj(min) = 0.26; z = 6). We conclude that each channel is controlled by two types of gates, a fast one responsible for Vj gating and involving transitions between open states (i.e., residual state, substates, main state), and a slow one involving transitions between the closed state and an open state.
利用稳定转染了小鼠连接蛋白40 DNA的人HeLa细胞克隆来检测间隙连接。将两个分离的细胞彼此进行物理接触(“诱导细胞对”),以允许间隙连接通道的插入,从而形成间隙连接。采用双电压钳法测量细胞间电流。这种方法使我们能够研究间隙连接通道(具有单个通道的细胞对)和间隙连接(具有多个通道的细胞对)的电学性质。我们发现单个通道表现出多种电导,一个主状态(γj(主状态))、几个亚状态(γj(亚状态))、一个残余状态(γj(残余状态))和一个关闭状态(γj(关闭状态))。γj(主状态)为198 pS,γj(残余状态)为36 pS(温度36 - 37℃;移液管溶液,天冬氨酸钾)。这两种性质对跨连接电压Vj均不敏感。关闭状态与开放状态(即残余状态、亚状态或主状态)之间的转变缓慢(15 - 45毫秒);残余状态与亚状态或主状态之间的转变迅速(1 - 2毫秒)。在稳态条件下,开放通道概率Po呈S形从1降至0(玻尔兹曼拟合:Vj,o = -44 mV;z = 6)。γj(主状态)和γj(残余状态)的温度系数Q10分别为1.2和1.3(p < 0.001;范围15 - 40℃)。这种差异表明在γj(残余状态)情况下离子与通道结构之间存在相互作用。在具有多个通道的细胞对中,稳态下的间隙连接电导gj对Vj呈钟形依赖性(玻尔兹曼拟合,负Vj,Vj,o = -45 mV,gj(min) = 0.24;正Vj,Vj,o = 49 mV,gj(min) = 0.26;z = 6)。我们得出结论,每个通道由两种类型的门控,一种快速门控负责Vj门控,涉及开放状态(即残余状态、亚状态、主状态)之间的转变,另一种缓慢门控涉及关闭状态与开放状态之间的转变。