De Bruijne J, Jongsma H J, van Ginneken A C
J Physiol. 1984 Oct;355:281-93. doi: 10.1113/jphysiol.1984.sp015419.
Membrane specific resistance and capacitance of non-spontaneously active spheroidal aggregates, cultured from collagenase-dissociated neonatal rat heart cells, were calculated from changes in membrane potential due to intracellularly injected rectangular hyper- and depolarizing current pulses during diastole. The relation between steady-state membrane voltage displacement and injected current is linear for current pulses between +10 and -10 nA. No significant fall-off of electrotonic potential is measured in an aggregate at increasing distances from the site of current injection. The aggregate membrane resistance (input resistance) was best fitted by an inverse square function of the aggregate radius. This suggests selective current flow through the outer membranes of the spheroidal aggregate. Taking this into account the membrane specific resistance was calculated to be 753 +/- 38 omega cm2 (S.E. of mean; n = 39). The time course of the change in membrane potential is exponential with a time constant ranging from 5 to 26 ms, depending on the aggregate radius. The aggregate membrane capacitance is calculated from the exponential transients for each aggregate and appears to be a cubic function of the radius, indicating that the membrane area of all cells in the preparation equally contributes to the input capacitance. The membrane specific capacitance is calculated to be 0.97 +/- 0.02 microF/cm2 (S.E. of mean; n = 100). It is concluded that myocytes in aggregates are electrically well coupled and that a resistance in series with the inner membranes, if present, is negligible compared to the membrane resistance of the internal cells. In order to explain the finding that the membrane resistance was not inversely related to the cube of the aggregate radius, it is postulated that the membrane specific resistance might be a function of aggregate radius.
从胶原酶解离的新生大鼠心脏细胞培养的非自发性活动球状聚集体的膜比电阻和电容,是根据舒张期细胞内注入矩形超极化和去极化电流脉冲引起的膜电位变化来计算的。对于+10至-10 nA之间的电流脉冲,稳态膜电压位移与注入电流之间的关系是线性的。在距电流注入部位距离增加时,未在聚集体中测量到电紧张电位的显著衰减。聚集体膜电阻(输入电阻)最适合用聚集体半径的反平方函数来拟合。这表明电流选择性地流过球状聚集体的外膜。考虑到这一点,计算出膜比电阻为753±38Ω·cm²(平均值的标准误;n = 39)。膜电位变化的时间进程是指数性的,时间常数范围为5至26 ms,这取决于聚集体半径。聚集体膜电容是根据每个聚集体的指数瞬变来计算的,并且似乎是半径的立方函数,表明制剂中所有细胞的膜面积对输入电容的贡献相同。计算出膜比电容为0.97±0.02μF/cm²(平均值的标准误;n = 100)。得出的结论是,聚集体中的心肌细胞电耦合良好,并且与内膜串联的电阻(如果存在)与内部细胞的膜电阻相比可忽略不计。为了解释膜电阻与聚集体半径的立方不成反比关系这一发现,推测膜比电阻可能是聚集体半径的函数。