De Weer P, Gadsby D C, Rakowski R F
Marine Biological Laboratory, Woods Hole, Massachusetts 02543, USA.
J Gen Physiol. 2001 Apr;117(4):315-28. doi: 10.1085/jgp.117.4.315.
The steady-state voltage and Na(+) dependence of the electrogenic sodium pump was investigated in voltage-clamped internally dialyzed giant axons of the squid, Loligo pealei, under conditions that promote the backward-running mode (K(+)-free seawater; ATP- and Na(+)-free internal solution containing ADP and orthophosphate). The ratio of pump-mediated (42)K(+) efflux to reverse pump current, I(pump) (both defined by sensitivity to dihydrodigitoxigenin, H(2)DTG), scaled by Faraday's constant, was -1.5 +/- 0.4 (n = 5; expected ratio for 2 K(+)/3 Na(+) stoichiometry is -2.0). Steady-state reverse pump current-voltage (I(pump)-V) relationships were obtained either from the shifts in holding current after repeated exposures of an axon clamped at various V(m) to H(2)DTG or from the difference between membrane I-V relationships obtained by imposing V(m) staircases in the presence or absence of H(2)DTG. With the second method, we also investigated the influence of Na(+) (up to 800 mM, for which hypertonic solutions were used) on the steady-state reverse I(pump)-V relationship. The reverse I(pump)-V relationship is sigmoid, I(pump) saturating at large negative V(m), and each doubling of Na(+) causes a fixed (29 mV) rightward parallel shift along the voltage axis of this Boltzmann partition function (apparent valence z = 0.80). These characteristics mirror those of steady-state (22)Na(+) efflux during electroneutral Na(+)/Na(+) exchange, and follow without additional postulates from the same simple high field access channel model (Gadsby, D.C., R.F. Rakowski, and P. De Weer, 1993. Science. 260:100-103). This model predicts valence z = nlambda, where n (1.33 +/- 0.05) is the Hill coefficient of Na binding, and lambda (0.61 +/- 0.03) is the fraction of the membrane electric field traversed by Na ions reaching their binding site. More elaborate alternative models can accommodate all the steady-state features of the reverse pumping and electroneutral Na(+)/Na(+) exchange modes only with additional assumptions that render them less likely.
在促进反向运转模式的条件下(无钾海水;含二磷酸腺苷和正磷酸盐的无三磷酸腺苷和无钠内部溶液),研究了乌贼(Loligo pealei)电压钳制的内部透析巨轴突中电生钠泵的稳态电压和Na⁺依赖性。泵介导的(⁴²)K⁺外流与反向泵电流I(pump)的比值(两者均由对双氢地高辛配基H₂DTG的敏感性定义),经法拉第常数换算后为-1.5±0.4(n = 5;2K⁺/3Na⁺化学计量比的预期比值为-2.0)。稳态反向泵电流-电压(I(pump)-V)关系可通过将钳制在不同V(m)的轴突反复暴露于H₂DTG后保持电流的变化获得,也可通过在有或无H₂DTG的情况下施加V(m)阶梯得到的膜I-V关系之差获得。采用第二种方法,我们还研究了Na⁺(高达800 mM,为此使用了高渗溶液)对稳态反向I(pump)-V关系的影响。反向I(pump)-V关系呈S形,I(pump)在大的负V(m)时达到饱和,Na⁺每增加一倍,会使该玻尔兹曼分配函数的电压轴向右平行移动固定值(29 mV)(表观价态z = 0.80)。这些特征反映了电中性Na⁺/Na⁺交换过程中稳态(²²)Na⁺外流的特征,并且无需额外假设即可从相同的简单高场通路模型得出(Gadsby, D.C., R.F. Rakowski, and P. De Weer, 1993. Science. 260:100 - 103)。该模型预测价态z = nλ,其中n(1.33±0.05)是Na⁺结合的希尔系数,λ(0.61±0.03)是到达其结合位点的Na⁺离子穿越的膜电场分数。更复杂的替代模型只能通过额外假设来适应反向泵浦和电中性Na⁺/Na⁺交换模式的所有稳态特征,而这些假设使其可能性降低。