Thompson S, Coombs J
Hopkins Marine Station, Stanford University, Pacific Grove, California 93950.
J Neurosci. 1988 Jun;8(6):1929-39. doi: 10.1523/JNEUROSCI.08-06-01929.1988.
The spatial distribution of Ca current in molluscan neuron cell bodies was studied using a large patch method in combination with 2-microelectrode voltage clamp. The method has a spatial resolution equal to about 0.1% of the cell body area. Ca current is not uniformly distributed. The current density varies between patches, changing by as much as a factor of 2.5 over a distance of 20 micron, and there is evidence that Ca current occurs in "hot spots" involving a few hundred channels. The current density increases in a moderately steep gradient from the soma cap, opposite the axon, toward the axon hillock. Ca currents in patches from different regions of the soma are qualitatively different. Currents near the soma cap do not inactivate or inactivate weakly during depolarization, while currents of equal density nearer the axon hillock exhibit pronounced inactivation. The strength of inactivation increases in parallel with the gradient in current density, but local differences in current density, or in the number of active Ca channels, do not explain the variability in inactivation. Inactivating and noninactivating Ca currents could not be distinguished on the basis of activation or deactivation kinetics, voltage dependence of activation, or sensitivity to hyperpolarizing conditioning pulses. Also, the amplitude of noninactivating current near the soma cap is reduced by intracellular Ca injection showing that, like the whole-cell current, Ca current in this region is subject to Ca-dependent inactivation. The data favor the hypothesis that these cells express only one type of Ca channel. Differences in the strength of inactivation may result from local differences in cytoplasmic Ca buffering, local modification of Ca channels in a way that changes their sensitivity to Ca-dependent inactivation, or local differences in the availability of cytoplasmic factors or enzymes that are necessary for inactivation.
利用大膜片钳方法结合双微电极电压钳,研究了软体动物神经元细胞体中钙电流的空间分布。该方法的空间分辨率约为细胞体面积的0.1%。钙电流分布并不均匀。不同膜片之间的电流密度有所变化,在20微米的距离内变化幅度高达2.5倍,并且有证据表明钙电流出现在涉及数百个通道的“热点”区域。电流密度从与轴突相对的胞体帽向轴丘呈适度陡峭的梯度增加。来自胞体不同区域的膜片上的钙电流在性质上有所不同。胞体帽附近的电流在去极化期间不会失活或失活较弱,而在轴丘附近密度相同的电流则表现出明显的失活。失活的强度与电流密度的梯度平行增加,但电流密度或活性钙通道数量的局部差异并不能解释失活的变异性。失活和非失活的钙电流不能根据激活或失活动力学、激活的电压依赖性或对超极化预处理脉冲的敏感性来区分。此外,胞体帽附近非失活电流的幅度会因细胞内注入钙而降低,这表明与全细胞电流一样,该区域的钙电流也受到钙依赖性失活的影响。这些数据支持了这些细胞只表达一种类型钙通道的假说。失活强度的差异可能源于细胞质钙缓冲的局部差异、钙通道的局部修饰,从而改变其对钙依赖性失活的敏感性,或者失活所需的细胞质因子或酶的可用性的局部差异。