Purnick P E, Oh S, Abrams C K, Verselis V K, Bargiello T A
Department of Neuroscience, Albert Einstein College of Medicine, Bronx, New York 10461, USA.
Biophys J. 2000 Nov;79(5):2403-15. doi: 10.1016/S0006-3495(00)76485-X.
Intercellular channels formed by connexins (gap junctions) are sensitive to the application of transjunctional voltage (V(j)), to which they gate by the separate actions of their serially arranged hemichannels (Harris, A. L., D. C. Spray, and M. V. L. Bennett. 1981. J. Gen. Physiol. 77:95-117). Single channel studies of both intercellular and conductive hemichannels have demonstrated the existence of two separate gating mechanisms, termed "V(j)-gating" and "loop gating" (Trexler, E. B., M. V. L. Bennett, T. A. Bargiello, and V. K. Verselis. 1996. Proc. Natl. Acad. Sci. U.S.A. 93:5836-5841). In Cx32 hemichannels, V(j)-gating occurs at negative V(j) (Oh, S., J. B. Rubin, M. V. L. Bennett, V. K. Verselis, and T. A. Bargiello. 1999. J. Gen. Physiol. 114:339-364; Oh, S., C. K. Abrams, V. K. Verselis, and T. A. Bargiello. 2000. J. Gen. Physiol. 116:13-31). A negative charge substitution at the second amino acid position in the N-terminus reverses the polarity of V(j)-gating of Cx32 hemichannels (Verselis, V. K., C. S. Ginter, and T. A. Bargiello. 1994. Nature. 368:348-351;. J. Gen. Physiol. 116:13-31). We report that placement of a negative charge at the 5th, 8th, 9th, or 10th position can reverse the polarity of Cx32 hemichannel V(j)-gating. We conclude that the 1st through 10th amino acid residues lie within the transjunctional electric field and within the channel pore, as in this position they could sense changes in V(j) and be largely insensitive to changes in absolute membrane potential (V(m)). Conductive hemichannels formed by Cx32Cx43E1 containing a negatively charged residue at either the 8th or 10th position display bi-polar V(j)-gating; that is, the open probability of hemichannels formed by these connexins is reduced at both positive and negative potentials and is maximal at intermediate voltages. In contrast, Cx32Cx43E1 hemichannels with negative charges at either the 2nd or 5th positions are uni-polar, closing only at positive V(j). The simplest interpretation of these data is that the Cx32 hemichannel can adopt at least two different open conformations. The 1st-5th residues are located within the electric field in all open channel conformations, while the 8th and 10th residues lie within the electric field in one conformation and outside the electric field in the other conformation.
由连接蛋白形成的细胞间通道(间隙连接)对跨连接电压(V(j))的施加敏感,它们通过其串联排列的半通道的单独作用对其进行门控(哈里斯,A. L.,D. C. 斯普雷,和 M. V. L. 贝内特。1981 年。《普通生理学杂志》77:95 - 117)。对细胞间和传导性半通道的单通道研究已经证明存在两种独立的门控机制,称为“V(j) - 门控”和“环门控”(特雷克斯勒,E. B.,M. V. L. 贝内特,T. A. 巴尔吉洛,和 V. K. 韦尔塞利斯。1996 年。《美国国家科学院院刊》93:5836 - 5841)。在 Cx32 半通道中,V(j) - 门控发生在负的 V(j) 时(吴,S.,J. B. 鲁宾,M. V. L. 贝内特,V. K. 韦尔塞利斯,和 T. A. 巴尔吉洛。1999 年。《普通生理学杂志》114:339 - 364;吴,S.,C. K. 艾布拉姆斯,V. K. 韦尔塞利斯,和 T. A. 巴尔吉洛。2000 年。《普通生理学杂志》116:13 - 31)。在 N 端第二个氨基酸位置的负电荷取代会反转 Cx32 半通道 V(j) - 门控的极性(韦尔塞利斯,V. K.,C. S. 金特,和 T. A. 巴尔吉洛。1994 年。《自然》。368:348 - 351;《普通生理学杂志》116:13 - 31)。我们报告在第 5、8、9 或 10 位放置负电荷可以反转 Cx32 半通道 V(j) - 门控的极性。我们得出结论,第 1 至 10 个氨基酸残基位于跨连接电场内和通道孔内,因为在这个位置它们可以感知 V(j) 的变化并且对绝对膜电位(V(m))的变化基本不敏感。由在第 8 或 10 位含有负电荷残基的 Cx32Cx43E1 形成的传导性半通道表现出双极 V(j) - 门控;也就是说,由这些连接蛋白形成的半通道的开放概率在正电位和负电位时都会降低,而在中间电压时最大。相比之下,在第 2 或 5 位带有负电荷的 Cx32Cx43E1 半通道是单极的,仅在正的 V(j) 时关闭。对这些数据最简单的解释是 Cx32 半通道可以采用至少两种不同的开放构象。在所有开放通道构象中,第 1 - 5 个残基位于电场内,而第 8 和 10 个残基在一种构象中位于电场内,在另一种构象中位于电场外。