Gardner-Medwin A R
J Physiol. 1983 Feb;335:353-74. doi: 10.1113/jphysiol.1983.sp014539.
The flux of K+ produced by electric current across the pia-arachnoid surface of the neocortex of anaesthetized rats has been studied with K+-selective electrodes in a cup at the surface and with flame photometry. The potential differences developed across three regions of the rat brain (neocortex, cerebellum, hippocampus) have been measured as [K+] was altered in fluid at the surface. The experimental results have been related to those that would be expected (i) if K+ moved principally by diffusion in extracellular space and (ii) if current flow through cells makes a significant contribution to K+ transfer. K movement produced by current across the neocortical surface accounted for 0.06 of the transfer of electric charge with small currents in either direction (ca. 5 microA mm-2) and with larger currents out of the tissue. Large currents (ca. 20 microA mm-2) into the tissue produced less K+ movement, but still more than the fraction 0.012 expected for purely extracellular flux. Alternating current pulses (5 Hz) with zero net transfer of charge produced no flux of K+ across the surface, while alternation with unequal durations produced the same effects as the equivalent steady charge transfer. The K+ flux lagged behind the onset and cessation of current with a time constant ca. 45 sec, approximately as expected from calculations with a model of the tissue. A surface-negative potential shift averaging 2 mV was observed when [K+ ]at the brain surface was increased from 3 to 12 mM. The time for development of half of the full potential change was 20 sec, with the solution changes complete in less than 4 sec. These results are inconsistent with the hypothesis that K+ movement through brain tissue occurs principally through intercellular clefts, except where these movements involve very localized gradients. They are consistent with the conclusion that ca. 5 times as much K+ flux passes through cells (probably largely glial cells) as through extracellular space, with fluxes driven by either extracellular voltage or concentration gradients.
利用置于麻醉大鼠新皮质软脑膜表面杯中的钾离子选择性电极以及火焰光度法,研究了电流通过该表面所产生的钾离子通量。在改变表面液体中钾离子浓度时,测量了大鼠脑三个区域(新皮质、小脑、海马体)产生的电位差。将实验结果与预期结果进行了关联,预期结果如下:(i)钾离子主要通过细胞外空间扩散移动;(ii)电流通过细胞对钾离子转移有显著贡献。电流通过新皮质表面产生的钾离子移动,在小电流双向流动(约5微安/平方毫米)以及较大电流流出组织时,占电荷转移的0.06。流入组织的大电流(约20微安/平方毫米)产生的钾离子移动较少,但仍比纯细胞外通量预期的0.012分数要多。电荷净转移为零的交流脉冲(5赫兹)不会使钾离子穿过表面,而持续时间不等的交替脉冲产生的效果与等效的稳定电荷转移相同。钾离子通量在电流开始和停止后有滞后,时间常数约为45秒,大致与用组织模型计算的结果相符。当脑表面的钾离子浓度从3毫摩尔增加到12毫摩尔时,观察到平均为2毫伏的表面负电位偏移。达到最大电位变化一半所需的时间为约20秒,溶液变化在不到4秒内完成。这些结果与钾离子通过脑组织主要通过细胞间缝隙移动的假设不一致,除非这些移动涉及非常局部的梯度。它们与以下结论一致:通过细胞(可能主要是神经胶质细胞)的钾离子通量大约是通过细胞外空间的5倍,通量由细胞外电压或浓度梯度驱动。