Simon B J, Beam K G
J Gen Physiol. 1985 Jan;85(1):1-19. doi: 10.1085/jgp.85.1.1.
Voltage-dependent charge movements were measured in the rat omohyoid muscle with the three-microelectrode voltage-clamp technique. Contraction was abolished with hypertonic sucrose. The standard (ON-OFF) protocol for eliciting charge movements was to depolarize the fiber from -90 mV to a variable test potential (V) and then repolarize the fiber to -90 mV. The quantity of charge moved saturated at test potentials of approximately 0 mV. The steady state dependence of the amount of charge that moves as a function of test potential could be well fitted by the Boltzmann relation: Q = Qmax/(1 + exp[-(V - V)/k]), where Qmax is the maximum charge that can be moved, V is the potential at which half the charge moves, and k is a constant. At 15 degrees C, these values were Qmax = 28.5 nC/microF, V = -34.2 mV, and k = 8.7 mV. Qmax, k, and V exhibited little temperature dependence over the range 7-25 degrees C. "Stepped OFF" charge movements were elicited by depolarizing the fiber from -90 mV to a fixed conditioning level that moved nearly all the mobile charge (0 mV), and then repolarizing the fiber to varying test potentials. The sum of the charge that moved when the fiber was depolarized directly from -90 mV to a given test potential and the stepped OFF charge that moved when the fiber was repolarized to the same test potential had at all test potentials a value close to Qmax for that fiber. In nearly all cases, the decay phase of ON, OFF, and stepped OFF charge movements could be well fitted with a single exponential. The time constant, tau decay, for an ON charge movement at a given test potential was comparable to tau decay for a stepped OFF charge movement at the same test potential. Tau decay had a bell-shaped dependence on membrane potential: it was slowest at a potential near V (the midpoint of the steady state charge distribution) and became symmetrically faster on either side of this potential. Raising the temperature from 7 to 15 degrees C caused tau decay to become faster by about the same proportion at all potentials, with a Q10 averaging 2.16. Raising the temperature from 15 to 25 degrees C caused tau decay to become faster at potentials near V, but not at potentials farther away.(ABSTRACT TRUNCATED AT 400 WORDS)
采用三微电极电压钳技术在大鼠肩胛舌骨肌中测量电压依赖性电荷移动。用高渗蔗糖使收缩消失。引发电荷移动的标准(开 - 关)方案是将纤维从 -90 mV 去极化至可变测试电位(V),然后再将纤维复极化至 -90 mV。在约 0 mV 的测试电位下,移动的电荷量达到饱和。移动的电荷量作为测试电位函数的稳态依赖性可用玻尔兹曼关系式很好地拟合:Q = Qmax/(1 + exp[-(V - V)/k]),其中 Qmax 是可移动的最大电荷量,V 是移动一半电荷量时的电位,k 是一个常数。在 15℃时,这些值为 Qmax = 28.5 nC/μF,V = -34.2 mV,k = 8.7 mV。在 7 - 25℃范围内,Qmax、k 和 V 对温度的依赖性很小。“阶梯式关断”电荷移动是通过将纤维从 -90 mV 去极化至固定的预处理水平(该水平使几乎所有可移动电荷移动,即 0 mV),然后再将纤维复极化至不同的测试电位来引发的。当纤维直接从 -90 mV 去极化至给定测试电位时移动的电荷量与当纤维复极化至相同测试电位时移动的阶梯式关断电荷量之和,在所有测试电位下对于该纤维的值都接近 Qmax。几乎在所有情况下,开、关和阶梯式关断电荷移动的衰减相都可用单一指数很好地拟合。在给定测试电位下,开电荷移动的时间常数 τdecay 与相同测试电位下阶梯式关断电荷移动的 τdecay 相当。τdecay 对膜电位呈钟形依赖性:在接近 V(稳态电荷分布的中点)的电位处最慢,在该电位两侧对称地变快。将温度从 7℃升高到 15℃导致 τdecay 在所有电位下按大致相同的比例变快,Q10 平均为 2.16。将温度从 15℃升高到 25℃导致 τdecay 在接近 V 的电位处变快,但在更远的电位处不变。(摘要截断于 400 字)