Byerly L, Chase P B, Stimers J R
J Physiol. 1984 Mar;348:187-207. doi: 10.1113/jphysiol.1984.sp015105.
Both the activation kinetics and the magnitude of the Ca current in Lymnaea are strongly dependent on temperature. The Q10 for the reciprocal of the activation time constant is 4.9 +/- 0.2 and the Q10 for the maximum current is 2.3 +/- 0.1. By lowering the temperature to 7-10 degrees C, we have been able to resolve the Ca tail currents. The block of Ca current by Cd2+ is voltage dependent, being more effective at more positive potentials. As determined from the magnitude of the tail currents, the Ca permeability is not maximally activated until the membrane potential is greater than +70 mV. The Ca permeability is half activated in the range 30-35 mV. The open-channel current-voltage relation for the Ca current is in rough agreement with the prediction of the constant-field equation. There is no indication of current saturation at negative potentials for potentials down to -60 mV. The Ca tail current decays with at least two time constants, one 200-400 microseconds and the other 2-4 ms. Although these time constants are not strongly voltage dependent, the ratio of the amplitude of the fast component of the tail current to that of the slow component is much larger at -60 mV than at 0 mV. The time course of the Ba tail current is very similar to that of the Ca tail current. The time course of the activation of the Ca current follows m2 kinetics and does not show evidence for a Cole-Moore-type shift for holding potentials between -50 and -110 mV. During a second positive pulse applied 1 ms after the first, the Ca current activates more rapidly, without the delay characteristic of the Ca current of a single positive pulse. The activation of the Ca current can be represented by a linear sequential model. The simplest model that describes both the turn-on and the turn-off of the Ca current must have at least three closed states, followed by a single open state.
椎实螺(Lymnaea)中钙电流的激活动力学和电流大小都强烈依赖于温度。激活时间常数倒数的Q10为4.9±0.2,最大电流的Q10为2.3±0.1。通过将温度降至7 - 10摄氏度,我们得以分辨出钙尾电流。Cd2+对钙电流的阻断具有电压依赖性,在更正的电位下更有效。根据尾电流的大小确定,直到膜电位大于 +70 mV时钙通透性才达到最大激活。钙通透性在30 - 35 mV范围内被激活一半。钙电流的开放通道电流 - 电压关系与恒定场方程的预测大致相符。对于低至 -60 mV的负电位,没有电流饱和的迹象。钙尾电流至少以两个时间常数衰减,一个为200 - 400微秒,另一个为2 - 4毫秒。尽管这些时间常数对电压的依赖性不强,但在 -60 mV时尾电流快速成分的幅度与慢速成分的幅度之比远大于在0 mV时。钡尾电流的时间进程与钙尾电流非常相似。钙电流激活的时间进程遵循m2动力学,并且在 -50至 -110 mV的保持电位下未显示出科尔 - 穆尔(Cole - Moore)型偏移的证据。在第一个正脉冲后1毫秒施加第二个正脉冲时,钙电流激活得更快,没有单个正脉冲钙电流的延迟特征。钙电流的激活可以用线性顺序模型表示。描述钙电流开启和关闭的最简单模型必须至少有三个关闭状态,随后是一个开放状态。