首页> 美国卫生研究院文献>The Journal of Physiology >Estimating the time course of evoked quantal release at the frog neuromuscular junction using end-plate current latencies.
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Estimating the time course of evoked quantal release at the frog neuromuscular junction using end-plate current latencies.

机译:使用终板电流潜伏期估算青蛙神经肌肉接头处诱发的定量释放的时间过程。

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摘要

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+.
机译:在青蛙坐骨神经皮肌的肌肉准备过程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过程。我们还研究了量子释放降低或增强后续量子释放的可能性。将肌肉终板电压钳制在3-4摄氏度。使用不含Ca2 +的EGTA Ringer溶液和充满Ca2 +的微量移液器,将神经释放限制在神经末梢的短区域或局部区域。总计包含0、1、2等量子的e.p.c.s数量,并与使用泊松定理预测的数量进行比较。在研究的十九个交叉口处,实际事件数量与预测事件数量之间的差异并不显着(P小于0.05)。测量了在数百epc中观察到的第一个量子的潜伏期,并将其用于计算与时间相关的概率过程α(t)的估计值α1(t),该估计值控制着所有诱发的量子释放(Barrett&Stevens, 1972b)。在三个实验中,测量了所有的定量延迟,以获得实际的α(t)。在实际和模拟的延迟数据中,alpha 1(t)函数给出了极佳的alpha(t)近似值(P大于0.2)。测量了e.p.c.s中第二个量子的潜伏期,并将其用于提供α(t)的另一个估计值alpha 2(t)。相对于alpha 1(t),在诱发释放期的前几毫秒内,alpha 2(t)的功能降低(降低)。在所有实验中差异均显着(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.s”对我们的测量程序进行了测试。这些测试表明,早期的抑郁症是由于e.p.c.s中第二量子的检测不足所致。使用含有1 M-SrCl2和CaCl2溶液的双管移液管检查Sr2 +对诱发释放的影响。主要结果是相对于Ca2 +,Sr2 +中的alpha 1(t)和alpha 2(t)的持续时间均等延长。

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