Smirnov S V, Aaronson P I
Department of Pharmacology, United Medical School, Guy's Hospital, London, UK.
J Gen Physiol. 1994 Aug;104(2):241-64. doi: 10.1085/jgp.104.2.241.
The properties of the tail current associated with the delayed rectifier K+ current (IK) in isolated rat pulmonary artery smooth muscle cells were examined using the whole cell patch clamp technique. The tail currents observed upon repolarization to -60 mV after brief (e.g., 20 ms) or small (i.e. to potentials negative of 0 mV) depolarizations were outwardly directed, as expected given the calculated K+ reversal potential of -83 mV. The tail currents seen upon repolarization after longer (e.g., 500 ms) and larger (e.g., to +60 mV) depolarizations tended to be inwardly directed. Depolarizations of intermediate strength and/or duration were followed by biphasic tail currents, which were inwardly directed immediately upon repolarization, but changed direction and became outwardly directed before deactivation was complete. When cells were depolarized to +60 mV for 500 ms both IK and the subsequent inward tail current at -60 mV were similarly blocked by phencyclidine. Both IK and the inward tail current were also blocked by 4-aminopyridine. Application of progressively more depolarized 30 s preconditioning potentials inactivated IK, and reduced the inward tail current amplitude with a similar potential dependency. These results indicated that the inward tail current was mediated by IK. The reversal potential of the tail current became progressively more positive with longer depolarizations to +60 mV, shifting from -76.1 +/- 2.2 mV (n = 10) after a 20-ms step to -57.7 +/- 3.5 mV (n = 9) after a 500-ms step. Similar effects occurred when extracellular K+ and Na+ were replaced by choline. When extracellular K+ was raised to 50 mM, the tail current was always inwardly directed at -60 mV, but showed little change in amplitude as the duration of depolarization was increased. These observations are best explained if the dependencies of tail current direction and kinetics upon the duration of the preceding depolarization result from an accumulation of K+ at the external face of the membrane, possibly in membrane invaginations. A mathematical model which simulates the reversal potential shift and the biphasic kinetics of the tail current on this basis is presented.
采用全细胞膜片钳技术,研究了分离的大鼠肺动脉平滑肌细胞中与延迟整流钾电流(IK)相关的尾电流特性。短暂(如20毫秒)或小幅度(即去极化到0毫伏以下电位)去极化后复极化到-60毫伏时观察到的尾电流向外,鉴于计算得出的钾离子反转电位为-83毫伏,这是预期的结果。较长时间(如500毫秒)和较大幅度(如去极化到+60毫伏)去极化后复极化时观察到的尾电流倾向于向内。中等强度和/或持续时间的去极化之后是双相尾电流,复极化时立即向内,但在失活完成前改变方向并变为向外。当细胞去极化到+60毫伏持续500毫秒时,IK和随后在-60毫伏的内向尾电流都被苯环利定类似地阻断。IK和内向尾电流也被4-氨基吡啶阻断。施加逐渐去极化程度更高的30秒预处理电位使IK失活,并以类似的电位依赖性降低内向尾电流幅度。这些结果表明内向尾电流由IK介导。随着去极化到+60毫伏的时间延长,尾电流的反转电位逐渐更正,从20毫秒阶跃后的-76.1±2.2毫伏(n = 10)变为500毫秒阶跃后的-57.7±3.5毫伏(n = 9)。当细胞外钾离子和钠离子被胆碱替代时,也出现类似效应。当细胞外钾离子升高到50毫摩尔时,在-60毫伏时尾电流总是向内,但随着去极化持续时间增加,幅度变化不大。如果尾电流方向和动力学对先前去极化持续时间的依赖性是由于钾离子在膜外表面(可能在膜内陷处)的积累导致的,那么这些观察结果就能得到最好的解释。在此基础上,提出了一个模拟尾电流反转电位变化和双相动力学的数学模型。