Baldo G J, Cohen I S, Van der Kloot W
J Physiol. 1986 May;374:503-13. doi: 10.1113/jphysiol.1986.sp016094.
The use of end-plate current (e.p.c.) latency measurements to estimate the time course of the stochastic probabilistic process governing evoked release was investigated in the sciatic nerve-sartorius muscle preparation of the frog, Rana pipiens. We also examined the possibility that the release of a quantum depresses or enhances the subsequent release of additional quanta. Muscle end-plates were voltage clamped at 3-4 degrees C. Quantal release was restricted to a short, or localized, region of the nerve terminal using Ca2+-free, EGTA Ringer solution and a Ca2+-filled micropipette. The number of e.p.c.s containing 0, 1, 2, etc. quanta were totalled and compared to numbers predicted using Poisson's theorem. The differences between the actual and predicted numbers of events were not significant at the nineteen junctions studied (P less than 0.05). The latency of the first quantum observed in several hundred e.p.c.s was measured and used to calculate an estimate, alpha 1(t), of the time-dependent, probabilistic process, alpha (t), governing all evoked quantal release (Barrett & Stevens, 1972b). In three experiments, all quantal latencies were measured to obtain the actual alpha (t). The alpha 1(t) function gave an excellent approximation of alpha (t) (P greater than 0.2), in real and simulated latency data. The latency of the second quantum in the e.p.c.s was measured and used to provide another estimate, alpha 2(t), of alpha (t). The alpha 2(t) function was lower (depressed) during the first few milliseconds of the evoked release period, relative to alpha 1(t). The difference was significant (P greater than 0.01) in all experiments. Our measurement procedures were tested using computer-generated 'e.p.c.s' containing randomly occurring 'quanta'. These tests showed that the early depression was due to inadequate detection of the second quantum in the e.p.c.s. The effect of Sr2+ on evoked release was examined using double-barrelled pipettes containing 1 M-SrCl2 and CaCl2 solutions. The major result was that the durations of alpha 1(t) and alpha 2(t) were equally lengthened in Sr2+, relative to Ca2+.
在牛蛙(Rana pipiens)的坐骨神经 - 缝匠肌标本中,研究了使用终板电流(e.p.c.)潜伏期测量来估计控制诱发释放的随机概率过程的时间进程。我们还研究了一个量子的释放是否会抑制或增强随后额外量子的释放。肌肉终板在3 - 4摄氏度下进行电压钳制。使用无钙、含乙二醇双乙酸盐(EGTA)的林格氏液和一个充满钙离子的微吸管,将量子释放限制在神经末梢的一个短的或局部的区域。对含有0、1、2等量子的e.p.c.数量进行总计,并与使用泊松定理预测的数量进行比较。在所研究的19个接头处,实际事件数与预测数之间的差异不显著(P小于0.05)。测量了几百个e.p.c.中观察到的第一个量子的潜伏期,并用于计算一个估计值α1(t),它是关于控制所有诱发量子释放的随时间变化的概率过程α(t)的估计值(Barrett和Stevens,1972b)。在三个实验中,测量了所有量子的潜伏期以获得实际的α(t)。在真实和模拟的潜伏期数据中,α1(t)函数对α(t)给出了极好的近似(P大于0.2)。测量了e.p.c.中第二个量子的潜伏期,并用于提供另一个关于α(t)的估计值α2(t)。相对于α1(t),α2(t)函数在诱发释放期的最初几毫秒内较低(被抑制)。在所有实验中,这种差异都是显著的(P大于0.01)。我们使用包含随机出现的“量子”的计算机生成的“e.p.c.”对测量程序进行了测试。这些测试表明,早期的抑制是由于在e.p.c.中对第二个量子的检测不足所致。使用含有1 M - SrCl2和CaCl2溶液的双管吸管研究了Sr2+对诱发释放的影响。主要结果是,相对于Ca2+,在Sr2+中α1(t)和α2(t)的持续时间同样延长。