Varanda W A, Vieira F L
J Membr Biol. 1978 Mar 20;39(4):369-85. doi: 10.1007/BF01869899.
When the Na electrochemical potential difference across the skin (delta muNa) is altered by perturbing the transmembrane electrical potential difference or the external Na concentration, effects on transport and associated oxygen consumption can be described by the formalism of linear nonequilibrium thermodynamics (Vieira, Caplan & Essig, 1972, J. Gen. Physiol. 59:77; Danisi & Lacaz-Vieira, 1974, J. Gen. Physiol. 64:372; Procópio and Lacaz-Vieira, 1977, J. Membrane Biol. 35:219). We now show that with modifications of delta muNa by substitution of Li or choline for Na in the inner bathing solution, this formalism is no longer applicable. Inner Na by K substitution ((Na X K)i) causes profound alterations in short-circuit current (SCC), JinNa, K efflux (JeffK) and PD. SCC drops transiently after (Na X K)i in Cl and in SO4 media, increasing subsequently. In Cl medium, following the initial transient, there is a late decline in SCC toward a steady state. The rate of SCC decline in Cl medium is more pronounced than that observed in SO4 medium. (Na X K)i causes a transient increase in JinNa with a peak synchronous to the minimum in SCC, both in Cl and in SO4 media. This was interpreted as due to depolarization of the inner membrane. In SO4 medium, following the peak observed after (Na X K)i, JimNa drops, to increase again toward a steady state in which SCC and JinNa are not statistically different, resembling the control condition before (Na X K)i. In Cl medium, however, the JinNa steady state is approximately 100% higher than SCC. This difference is due to an important K efflux (JeffK), which builds up progressively after the substitution. The apparent K permeability [JeffK/(Ki)] is of comparable magnitude in Cl and in SO4 media before (Na X K)i and also in SO4 medium after (Na X K)i. However, in Cl medium, after (Na X K)i, the apparent K permeability increases one order of magnitude as compared to the control condition before the ionic substitution. In Cl medium, the high levels of JinNa and of Jeff(K) observed in the steady state after (Na X K)i were interpreted as being a consequence of cell swelling. SCC and PD follow very different temporal patterns after (Na X K)i which are characterized by transients in SCC and a simple fall in PD. Reasons for these differences are discussed.
当通过改变跨膜电势差或外部钠离子浓度来改变皮肤跨膜的钠电化学势差(δμNa)时,对转运及相关耗氧量的影响可用线性非平衡态热力学形式来描述(维埃拉、卡普兰和埃西格,1972年,《普通生理学杂志》59:77;达尼西和拉卡兹 - 维埃拉,1974年,《普通生理学杂志》64:372;普罗科皮奥和拉卡兹 - 维埃拉,1977年,《膜生物学杂志》35:219)。我们现在表明,在内侧浴液中用锂或胆碱替代钠从而改变δμNa后,这种形式不再适用。用钾替代内侧的钠((Na X K)i)会导致短路电流(SCC)、钠内向电流(JinNa)、钾外流(JeffK)和跨膜电位(PD)发生深刻变化。在Cl和SO4介质中,(Na X K)i后SCC会短暂下降,随后上升。在Cl介质中,初始短暂下降之后,SCC会出现后期下降并趋向稳态。Cl介质中SCC下降速率比在SO4介质中观察到的更明显。在Cl和SO4介质中,(Na X K)i都会使JinNa短暂增加,其峰值与SCC的最小值同步,这被解释为是内膜去极化所致。在SO4介质中,(Na X K)i后观察到峰值之后,JimNa下降,然后再次上升趋向稳态,此时SCC和JinNa在统计学上无差异,类似于(Na X K)i之前的对照条件。然而,在Cl介质中,JinNa稳态比SCC大约高100%。这种差异是由于重要的钾外流(JeffK),它在替代后逐渐增加。在(Na X K)i之前,Cl和SO4介质中以及(Na X K)i之后的SO4介质中,表观钾通透性[JeffK/(Ki)]大小相当。然而,在Cl介质中,(Na X K)i后,表观钾通透性与离子替代前的对照条件相比增加了一个数量级。在Cl介质中,(Na X K)i后稳态下观察到的高JinNa和高Jeff(K)被解释为细胞肿胀的结果。(Na X K)i后SCC和PD遵循非常不同的时间模式,其特征是SCC出现短暂变化,而PD简单下降。讨论了这些差异的原因。