Hui C S, Chandler W K
Department of Physiology, Indiana University School of Medicine, Indianapolis 46223.
J Gen Physiol. 1990 Aug;96(2):257-97. doi: 10.1085/jgp.96.2.257.
Intramembranous charge movement was measured in cut twitch fibers mounted in a double Vaseline-gap chamber with either a tetraethylammonium chloride (TEA.Cl) or a TEA2.SO4 solution (13-14 degrees C) in the central pool. Charge vs. voltage data were fitted by a single two-state Boltzmann distribution function. The average values of V (the voltage at which steady-state charge is equally distributed between the two Boltzmann states), k (the voltage dependence factor), and qmax/cm (the maximum charge divided by the linear capacitance, both per unit length of fiber) were V = -53.3 mV (SEM, 1.1 mV), k = 6.3 mV (SEM, 0.3 mV), qmax/cm = 18.0 nC/microF (SEM, 1.1 nC/microF) in the TEA.Cl solution; and V = -35.1 mV (SEM, 1.8 mV), k = 10.5 mV (SEM, 0.9 mV), qmax/cm = 36.3 nC/microF (SEM, 3.2 nC/microF) in the TEA2.SO4 solution. These values of k are smaller than those previously reported for cut twitch fibers and are as small as those reported for intact fibers. If a correction is made for the contributions of currents from under the Vaseline seals, V = -51.2 mV (SEM, 1.1 mV), k = 7.2 mV (SEM, 0.4 mV), qmax/cm = 22.9 nC/microF (SEM, 1.4 nC/microF) in the TEA.Cl solution; and V = -34.0 mV (SEM, 1.9 mV), k = 10.1 mV (SEM, 1.1 mV), qmax/cm = 38.8 nC/microF (SEM, 3.2 nC/microF) in the TEA2.SO4 solution. With this correction, however, the fit of the theoretical curve to the data is poor. A good fit with this correction can be obtained with a sum of two Boltzmann distribution functions. The first has average values V = -33.0 mV (SEM, 2.8 mV), k = 11.0 mV (SEM, 0.5 mV), qmax/cm = 10.6 nC/microF (SEM, 1.0 nC/microF) in the TEA.Cl solution; and V = -20.0 mV (SEM, 3.3 mV), k = 17.0 mV (SEM, 2.0 mV), qmax/cm = 36.4 nC/microF (SEM, 2.3 nC/microF) in the TEA2.SO4 solution. The second has average values V = -56.5 mV (SEM, 1.3 mV), k = 2.9 mV (SEM, 0.4 mV), qmax/cm = 13.2 nC/microF (SEM, 1.0 nC/microF) in the TEA.Cl solution; and V = -41.6 mV (SEM, 1.4 mV), k = 2.5 mV (SEM, 0.8 mV), qmax/cm = 11.8 nC/microF (SEM, 1.7 nC/microF) in the TEA2.SO4 solution. When a fiber is depolarized to near V of the second Boltzmann function, a slowly developing "hump" appears in the ON-segment of the current record.(ABSTRACT TRUNCATED AT 400 WORDS)
在置于双凡士林间隙室中的切断的单收缩纤维中测量膜内电荷移动,中央池中装有四乙铵氯化物(TEA.Cl)或硫酸二乙铵(TEA2.SO4)溶液(13 - 14摄氏度)。电荷与电压数据通过单一的双态玻尔兹曼分布函数拟合。在TEA.Cl溶液中,V(稳态电荷在两个玻尔兹曼态之间均匀分布时的电压)、k(电压依赖性因子)和qmax/cm(最大电荷除以线性电容,均为每单位纤维长度)的平均值分别为V = -53.3 mV(标准误,1.1 mV),k = 6.3 mV(标准误,0.3 mV),qmax/cm = 18.0 nC/μF(标准误,1.1 nC/μF);在TEA2.SO4溶液中,V = -35.1 mV(标准误,1.8 mV),k = 10.5 mV(标准误,0.9 mV),qmax/cm = 36.3 nC/μF(标准误,3.2 nC/μF)。这些k值小于先前报道的切断单收缩纤维的值,并且与完整纤维报道的值一样小。如果对凡士林密封下电流的贡献进行校正,在TEA.Cl溶液中,V = -51.2 mV(标准误,1.1 mV),k = 7.2 mV(标准误,0.4 mV),qmax/cm = 22.9 nC/μF(标准误,1.4 nC/μF);在TEA2.SO4溶液中,V = -34.0 mV(标准误,1.9 mV),k = 10.1 mV(标准误,1.1 mV),qmax/cm = 38.8 nC/μF(标准误,3.2 nC/μF)。然而,进行此校正后,理论曲线与数据的拟合较差。使用两个玻尔兹曼分布函数的和可以得到此校正后的良好拟合。第一个在TEA.Cl溶液中的平均值为V = -33.0 mV(标准误,2.8 mV),k = 11.0 mV(标准误,0.5 mV),qmax/cm = 10.6 nC/μF(标准误,1.0 nC/μF);在TEA2.SO4溶液中,V = -20.0 mV(标准误,3.3 mV),k = 17.0 mV(标准误,2.0 mV),qmax/cm = 36.4 nC/μF(标准误,2.3 nC/μF)。第二个在TEA.Cl溶液中的平均值为V = -56.5 mV(标准误,1.3 mV),k = 2.9 mV(标准误,0.4 mV),qmax/cm = 13.2 nC/μF(标准误,1.0 nC/μF);在TEA2.SO4溶液中,V = -41.6 mV(标准误,1.4 mV),k = 2.5 mV(标准误,0.8 mV),qmax/cm = 11.8 nC/μF(标准误,1.7 nC/μF)。当纤维去极化到第二个玻尔兹曼函数附近的V时,电流记录的开启段会出现一个缓慢发展的“驼峰”.(摘要截断于400字)