Effect of Ethanol on the Sodium and Potassium Conductances of the Squid Axon Membrane

The effects of ethanol on squid giant axons were studied by means of the sucrose-gap technique. The membrane action potential height is moderately reduced and the duration sometimes shortened by ethanol in sea water. Voltage clamp experiments showed that ethanol in sea water reduced the maximum membrane conductances for sodium (g'_Na) and potassium (g'_K). In experiments with multiple application of ethyl alcohol to the same spot of membrane, a reduction of g'_Na to 82 per cent and of g'_K to 80 per cent of their value in sea water was brought about by 3 per cent ethanol (by volume) while 6 per cent caused a decrease of g'_Na to 59 per cent and of g'_K to 69 per cent. Ethanol has no significant effect on the steady-state inactivation of g_Na (as a function of conditioning membrane potential) or on such kinetic parameters as τ_h or the time course of turning on gi g_Na and g_K. It is concluded that ethanol mainly reduces g_Na and g_K in the Hodgkin-Huxley terminology.     

Partition of the Hodgkin-Huxley type model parameter space into the regions of qualitatively different solutions

We have examined the problem of obtaining relationships between the type of stable solutions of the Hodgkin-Huxley type system, the values of its parameters and a constant applied current (I). As variable parameters of the system the maximal Na⁺(g_Na),K⁺(g_K) conductances and shifts (Gm, Gh, Gn) of the voltage-dependences have been chosen. To solve this problem it is sufficient to find points belonging to the boundary, partitioning the parameter space of the system into the regions of the qualitatively different types of stable solutions (steady states and stable periodic oscillations). Almost all over the physiological range of I, a type of stable solution is determined by the type of steady state (stable or unstable). Using this fact, the approximate solution of this problem could be obtained by analyzing the spectrum of eigenvalues of the Jacobian matrix for the linearized system. The families of the plane sections of the boundary have been constructed in the three-parameter spaces (I, g_Na,g_K), (I, Gm, Gh), (I, Gm, Gn).     

Sodium Conductance Activation without Inactivation in Pronase-perfused Axons

A controversy of long standing in membrane electrophysio-logy is whether the sodium ion current (I_Na) and potassium ion current (I_K) pass through the membrane in separate channels, or through a single set of channels which conduct first I_Na and then I_K. In support of the latter hypothesis it has been noted that the sodium conductance (g_Na) decline, called inactivation, proceeds with about the same time course as the potassium conductance (g_K) increase. This could mean that Na⁺ selective channels are being converted into K⁺ selective channels. The hypothesis is especially interesting because of the possibility that the carrier postulated in active transport is convertible from Na⁺ to K⁺ selectivity¹. An explicit statement of the single channel hypothesis and the means for disproving it were given by Mullins². Because a single channel could not simultaneously conduct I_Na and I_K, disproof requires that membrane conductance (g_m) be made somehow to exceed the maximum value of g_Na or g_K. We report here that inactivation of g_Na can be destroyed fairly selectively by the action from inside the axon of the unspecific proteolytic enzymes of pronase. In many cases g_m after pronase treatment is greater than maximum g_K before treatment, making untenable the single channel hypothesis.     

A comparison of the subcellular distribution of 5′-nucleotidase, (Na+K+)-ATPase and adenyl cyclase in beef thyroid gland

The validity of 5′-nucleotidase as a plasma membrane marker enzyme in beef thyroid has been tested by comparing the subcellular distribution of its activity to that of (Na⁺K⁺)-activated ATPase and adenyl cyclase. The specific activity and total activity of (Na⁺K⁺)-ATPase and adenyl cyclase were greatest in the 1000 × g (“nuclear”) and 33 000 × g (“mitochondrial and lysosomal”) fractions. In contrast, 5′-nucleotidase activity was concentrated in the 165 000 × g (“microsomal”) pellet and supernatant. Partially purified plasma membranes were separated from the 1000 (N₂), 30 000 (M₂) and 165 000 × g (P₂) pellets by discontinuous sucrose gradient centrifugation. Again a discordant distribution of these enzyme activities was observed. (Na⁺K⁺)-ATPase specific activity was increased approximately 30-fold over the homogenate in Fractions N₂ and M₂. Basal, thyroid-stimulating hormone-and fluoride-stimulated adenyl cyclase activities were concentrated in the same fractions. 5′-Nucleotidase activity was preferentially located in M₂ and P₂. These differences in distribution pattern suggest that 5′-nucleotidase activity is not uniquely located in the plasma membrane in the thyroid.     

Membrane conductances of principal cells in Malpighian tubules of Aedes aegypti

Two-electrode voltage clamp (TEVC) methods were used to explore conductive transport pathways in principal cells, the dominant cell type in Malpighian tubules of the yellow fever mosquito. The basolateral membrane of principal cells had a voltage (V_bl) of -85.1 mV in 49 principal cells under control conditions. Measures of the input resistance R_pc together with membrane fractional resistance yielded estimates of the conductance of the basolateral membrane (g_bl = 1.48 μS) and the apical membrane (g_a = 3.13 μS). K⁺ channels blocked by barium accounted for 0.94 μS of g_bl. Estimates of transference numbers yielded the basolateral membrane Na⁺ conductance of 0.24 μS, leaving 0.30 μS (20%) of g_bl unaccounted. The secretagogue db-cAMP (0.1 mM), a known activator of the basolateral membrane Na⁺ conductance, significantly depolarized V_bl to -65.0 mV and significantly increased g_bl from 1.48 μS to 2.47 μS. The increase was blocked with amiloride (1 mM), a known blocker of epithelial Na⁺ transport. The inhibition of metabolism with di-nitrophenol significantly depolarized V_bl to -9.7 mV and significantly increased R_pc from 391.6 kΩ to 2612.5 kΩ. Similar results were obtained with cyanide, but it remains unclear whether the large increases in R_pc stem from the uncoupling of epithelial cells and/or the shutdown of conductive transport pathways in basolateral and apical membranes. Our results indicate that the apical membrane of principal cells is more than twice as conductive as the basolateral membrane. Partial ionic conductances suggest the rate-limiting step for transepithelial Na⁺ secretion at the basolateral membrane.     

(Na,K)-ATPase activity of embryonic chick heart and skeletal muscles as a function of age

The specific activity of the membrane (Na⁺,K⁺)-ATPase of intact chick embryonic hearts (ventricles) was measured as a function of embryonic age. The membranes were prepared by a NaI extraction method of the 100 000 × g fraction which selectively removes much of the ouabain-insensitive Mg²⁺-ATPase. The specific activity of the myocardial (Na⁺, K⁺)-ATPase increased markedly during embryonic development from mean levels of about 3.0 μmoles P_i per h per mg protein at day 6 to 7.4 at day 16 and 11.0 at day 20 (1 day prior to hatching); the adult level was about the same as that of the 16-day-old chick. The relative activities with respect to that at day 16 (from paired experiments) averaged 43 % (day 6), 56 % (day 9), 73 % (day 13), 140 % (day 20), 115 % (day 23), 126 % (day 30) and 96 % (adult). There was a similar increase in relative activity of the (Na⁺,K⁺)-ATPase from chick skeletal (leg) muscles during development. If the total protein content per unit membrane area and the turnover number remain constant, the data indicate that the surface density of the (Na⁺,K⁺)-ATPase molecules increases during embryonic development; thus, the cation pumping capabilities of the cells should be enhanced if the surface area/volum ratio of the myocardial cells remains unchanged. However, the pumping capabilities of the very young cells must be sufficient to maintain the known high [K⁺]_i and low [Na⁺]_i already present; their internal activities actually change only to a small extent during development. Since there is a known increase in K⁺ permeability during embryonic development, thereby increasing the demand on the cation pump, the observed increase in activity of the (Na⁺,K⁺)-ATPase tends to compensate for this.     

Electrogenic and diffusive components of the membrane ofHydrodictyon africanum

Summary In cells of the freshwater algaHydrodictyon africanum, in solutions where [K⁺]₀=0.1mm and pH₀>7.0, the membrane in the light is hyperpolarized. The membrane potential difference {ie179-1} has values from –180 to –275 mV, more negative than any ion diffusion potential difference, and is predominantly a function of pH₀, and independent of [K⁺]₀. The hyperpolarization of the membrane appears to arise from an electrogenic efflux of H⁺, estimated from voltage-clamp data to be about 8 nmol m^–2 sec^–1 when pH₀=8.5. In the light the membrane conductanceg _m is about 0.084 S m^–2. At light-off, {ie179-2} becomes less negative, with a halftime for change of 15 to 30 sec andg _m decreases by about 0.052 S m^–2. After dark periods of up to 300 sec, {ie179-3} is largely independent of pH₀ for values greater than 6.0 and usually behaves as a combined K⁺ and Na⁺ diffusion potential with permeability ratioP _Na/P _K=0.05 to 0.2. The membrane potassium conductanceg _K has either a low value of 2–6×10^–2 Sm^–2, or a high value of up to 18×10^–2 S m^–2 depending on [K⁺]₀, the transition from low to high values occurring when {ie179-4} moves over a threshold value that is more negative than {ie179-5}, the electrochemical equilibrium potential for K⁺. The time for half-change of the transition is about 30 sec. The results are consistent with a model of the membrane in which the pump electromotive force and conductance are in parallel with diffusive electromotive forces and conductances. When the pump is operating its properties determine membrane properties, and when it is inoperative, or running at a diminished rate, the membrane properties are determined more by the diffusive pathways. Changes in both pump rate andg _K can account for a variety of characteristic changes in membrane PD and conductance occurring in response to ligh-dark changes, changes in light intensity, pasage of externally applied electric current across the membrane and changes in ionic constituents of the external medium.     

Model predictions of the ionic mechanisms underlying the beating and bursting pacemaker characteristics of molluscan neurons

The general properties of the excitable membrane on molluscan pacemaker neurons can be described on the basis of a fair amount of experimental evidence available in the literature. The neuronal membrane exhibits under voltage clamp an initial inward current carried by both Na⁺ and Ca²⁺ ions, the time- and voltage-dependent characteristics of which are similar to that of other excitable structures. The conductance mechanism for the two ion species and the transport kinetics appear to be closely similar. The time course and amplitude of the delayed outward current carried by K⁺ ions shows a marked dependence on the membrane potential. Characteristic for the molluscan neurons is the existence of an additional fast transient outward current which is only activated by hyperpolarizing shifts from the membrane potential. A regular beating discharge over a wide range of frequencies can be predicted by making the assumption of a metabolically controlled driving of the Na⁺ conductance. Bursting pacemaker characteristics can be correctly simulated by the model if sinusoidal variations of an additional Na⁺ and Ca²⁺ conductances g _Na and g _Ca, and periodic variations of the K⁺ conductance g _K, governed by the known operation of a metabolic substrate cycle are introduced. The close approximation of experimentally observed impulse bursts requires that the actual inpulse-frequency and the amplitude of the after-spike hyperpolarization are determined by the temporal pattern of g _Na, while the spike amplitude is controlled by g _Na which (although of similar time course) is lagging in phase behing g _Na. The periodic changes in additional K⁺ conductance g _K, are responsible for burst termination and the changes in inter-burst interval, to the effect that spike doublets, triplets and multi-spike bursts can be simulated by a suitable choice for the time characteristics of g _K. The model makes use of the finding that the Ca²⁺ inflow associated with a spike discharge actually activates g _K, so that large postburst hyperpolarizations can be obtained in high-frequency bursts.Supported by the Deutsche Forschungsgemeinschaft (Grant Ch 25/1)     

Ca2+-activated K+ conductance of the human red cell membrane: Voltage-dependent Na+ block of outward-going currents

Summary Human red cells were prepared with various cellular Na⁺ and K⁺ concentrations at a constant sum of 156mm. At maximal activation of the K⁺ conductance,g _K(Ca), the net efflux of K⁺ was determined as a function of the cellular Na⁺ and K⁺ concentrations and the membrane potential,V _m , at a fixed [K⁺]_ex of 3.5mm.V _m was only varied from (V _m –E _K)25 mV and upwards, that is, outside the range of potentials with a steep inward rectifying voltage dependence (Stampe & Vestergaard-Bogind, 1988).g _K(Ca) as a function of cellular Na⁺ and K⁺ concentrations atV _m =–40, 0 and 40 mV indicated a competitive, voltage-dependent block of the outward current conductance by cellular Na⁺. Since the present Ca²⁺-activated K⁺ channels have been shown to be of the multi-ion type, the experimental data from each set of Na⁺ and K⁺ concentrations were fitted separately to a Boltzmann-type equation, assuming that the outward current conductance in the absence of cellular Na⁺ is independent of voltage. The equivalent valence determined in this way was a function of the cellular Na⁺ concentration increasing from 0.5 to 1.5 as this concentration increased from 11 to 101mm. Data from a previous study of voltage dependence as a function of the degree of Ca²⁺ activation of the channel could be accounted for in this way as well. It is therefore suggested that the voltage dependence ofg _K(Ca) for outward currents at (V _m –E _K)>25 25 mV reflects a voltage-dependent Na⁺ block of the Ca²⁺-activated K⁺ channels.     

Changes in membrane properties of chick embryonic hearts during development

The electrophysiological properties of embryonic chick hearts (ventricles) change during development; the largest changes occur between days 2 and 8. Resting potential (E_m) and peak overshoot potential (+E _max) increase, respectively, from -35 mv and +11 mv at day 2 to -70 mv and +28 mv at days 12–21. Action potential duration does not change significantly. Maximum rate of rise of the action potential (+V _max) increases from about 20 v/sec at days 2–3 to 150 v/sec at days 18–21; + V _max of young cells is not greatly increased by applied hyperpolarizing current pulses. In resting E_m vs. log [K⁺]_o curves, the slope at high K⁺ is lower in young hearts (e.g. 30 mv/decade) than the 50–60 mv/decade obtained in old hearts, but the extrapolated [K⁺]_i values (125–140 mM) are almost as high. Input resistance is much higher in young hearts (13 MΩ at day 2 vs. 4.5 MΩ at days 8–21), suggesting that the membrane resistivity (R_m) is higher. The ratio of permeabilities, P _Na/P _K, is high (about 0.2) in young hearts, due to a low P _K, and decreases during ontogeny (to about 0.05). The low K⁺ conductance (g _K) in young hearts accounts for the greater incidence of hyperpolarizing afterpotentials and pacemaker potentials, the lower sensitivity (with respect to loss of excitability) to elevation of [K⁺]_o, and the higher chronaxie. Acetylcholine does not increase g _K of young or old ventricular cells. The increase in (Na⁺, K⁺)-adenosine triphosphatase (ATPase) activity during development tends to compensate for the increase in g _K. +E _max and + V _max are dependent on [Na⁺]_o in both young and old hearts. However, the Na⁺ channels in young hearts (2–4 days) are slow, tetrodotoxin (TTX)-insensitive, and activated-inactivated at lower E_m. In contrast, the Na⁺ channels of cells in older hearts (> 8 days) are fast and TTX-sensitive, but they revert back to slow channels when placed in culture.     

Sodium-dependent Potassium Channels in Leech P Neurons

In leech P neurons the inhibition of the Na⁺-K⁺ pump by ouabain or omission of bath K⁺ leaves the membrane potential unaffected for a prolonged period or even induces a marked membrane hyperpolarization, although the concentration gradients for K⁺ and Na⁺ are attenuated substantially. As shown previously, this stabilization of the membrane potential is caused by an increase in the K⁺ conductance of the plasma membrane, which compensates for the reduction of the K⁺ gradient. The data presented here strongly suggest that the increased K⁺ conductance is due to Na⁺-activated K⁺ (K_Na) channels. Specifically, an increase in the cytosolic Na⁺ concentration ([Na⁺]_i) was paralleled by a membrane hyperpolarization, a decrease in the input resistance (R_in) of the cells, and by the occurrence of an outwardly directed membrane current. The relationship between R_in and [Na⁺]_i followed a simple model in which the R_in decrease was attributed to K⁺ channels that are activated by the binding of three Na⁺ ions, with half-maximal activation at [Na⁺]_i between 45 and 70 mM. At maximum channel activation, R_in was reduced by more than 90%, suggesting a significant contribution of the K_Na channels to the physiological functioning of the cells, although evidence for such a contribution is still lacking. Injection experiments showed that the K_Na channels in leech P neurons are also activated by Li⁺.     

Two substrate sites in the renal Na+-d-glucose cotransporter studied by model analysis of phlorizin binding and-d-glucose transport measurements

Summary Time courses of phlorizin binding to the outside of membrane vesicles from porcine renal outer cortex and outer medulla were measured and the obtained families of binding curves were fitted to different binding models. To fit the experimental data a model with two binding sites was required. Optimal fits were obtained if a ratio of low and high affinity phlorizin binding sites of 1:1 was assumed. Na⁺ increased the affinity of both binding sites. By an inside-negative membrane potential the affinity of the high affinity binding site (measured in the presence of 3 mM Na⁺) and of the low affinity binding site (measured in the presence of 3 or 90 mM Na⁺) was increased. Optimal fits were obtained when the rate constants of dissociation were not changed by the membrane potential. In the presence of 90 mM Na⁺ on both membrane sides and with a clamped membrane potential,K _D values of 0.4 and 7.9 M were calculated for the low and high affinity phlorizin binding sites which were observed in outer cortex and in outer medulla. Apparent low and high affinity transport sites were detected by measuring the substrate dependence ofd-glucose uptake in membrane vesicles from outer cortex and outer medulla which is stimulated by an initial gradient of 90 mM Na⁺(out>in). Low and high affinity transport could be fitted with identicalK _m values in outer cortex and outer medulla. An inside-negative membrane potential decreased the apparentK _m ofhigh affinity transport whereas the apparentK _m of low affinity transport was not changed. The data show that in outer cortex and outer medulla of pighigh and low affinity Na⁺-d-glucose cotransporters are present which containlow and high affinity phlorizin binding sites, respectively. It has to be elucidated from future experiments whether equal amounts of low and high affinity transporters are expressed in both kidney regions or whether the low and high affinity transporter are parts of the same glucose transport moleculc.     

Application of the Hodgkin-Huxley equations to an electric field model for interaction between excitable cells

We previously described a model for the electrical transfer of excitation from one cell to the next which utilized the electric potential generated in the junctional cleft between the cells. Low-resistance connections between the cells were not used in the model, and it was assumed that the junctional membranes were excitable. This model was analyzed for the static case without capacitances and for the dynamic case in which capacitances were part of the circuit elements. For simplicity, the Na⁺ resistance (R_Na), after a threshold potential was exceeded, was allowed to decrease exponentially (to 1% of its initial value) within 0·25–1·0 ms, and possible changes in the K⁺ resistance were ignored. In this paper, we have incorporated the Hodgkin-Huxley equations into the operation of the lumped membrane units for the electrical equivalent circuit of the cell membrane. The parameters varied are the membrane capacitances, resistances, maximum Na⁺ conductance ($\text{g}{}_{\mathrm{<mtext>Na</mtext>}}$), and the radial cleft resistance (R_jc). We demonstrated that our model worked very well, i.e. the successful transfer of action potentials was achieved, with the membrane units following Hodgkin-Huxley dynamics for changes in g_Na and g_K. The calculations indicate that transmission is facilitated when the junctional units have a higher $\text{g}{}_{\mathrm{<mtext>Na</mtext>}}$ and a lower capacitance and when R_jc is elevated. Lowering the resistance of the junctional membrane units several fold, relative to the surface membrane units, also facilitated transmission; however, the absolute resistance of the junctional membrane was still well above the maximum value that would allow sufficient local-circuit current to flow to effect transmission. Thus, the electric field model provides an alternative means of cell-to-cell propagation between myocardial cells which is electrical in nature but does not require the presence of low-resistance connections between cells.     

Mechanism of aldosterone-induced increase of K+ conductance in early distal renal tubule cells of the frog

Summary Isolated early distal tubule cells (EDC) of frog kidney were incubated for 20–28 hr in the presence of aldosterone and then whole-cell K⁺ currents were measured at constant intracellular pH by the whole-cell voltage-clamp technique. Aldosterone increased barium-inhibitable whole-cell K⁺ conductance (gK⁺) threefold. This effect was reduced by amiloride and totally abolished by ouabain. However, aldosterone could still raisegK⁺ in ouabain-treated cells in the presence of furosemide.We tested whether changes in intracellular pH (pH _i ) could be a signal for cells to regulategK⁺. After removal of aldosterone, the increase ingK⁺ was preserved by subsequent incubation for 8 hr at pH 7.6 but abolished at pH 6.6. In the complete absence of aldosterone, incubation of cells at pH 8.0 for 20–28 hr raised pH _i and doubledgK⁺.Using the patch-clamp technique, three types of K⁺-selective channels were identified, which had conductances of 24, 45 and 59 pS.Aldosterone had no effect on the conductance or open probability (P _o) of any of the three types of channels. However, the incidence of observing type II channels was increased from 4 to 22%. Type II channels were also found to be pH sensitive,P _o was increased by raising pH.These results indicate that prolonged aldosterone treatment raises pH _i and increasesgK⁺ by promoting insertion of K⁺ channels into the cell membrane. Channel insertion is itself triggered by raising both pH _i and increasing the activity of the Na⁺/K⁺ pump in early distal cells of frog kidney. Present address: Department of Physiology, The University of Leeds, Leeds, LS2 9NQ, England     

Ion Selectivity of the KcsA Channel: A Perspective from Multi-Ion Free Energy Landscapes

Potassium (K⁺) channels are specialized membrane proteins that are able to facilitate and regulate the conduction of K⁺ through cell membranes. Comprising five specific cation binding sites (S₀-S₄) formed by the backbone carbonyl groups of conserved residues common to all K⁺ channels, the narrow selectivity filter allows fast conduction of K⁺ while being highly selective for K⁺ over Na⁺. To extend our knowledge of the microscopic mechanism underlying selectivity in K⁺ channels, we characterize the free energy landscapes governing the entry and translocation of a Na⁺ or a K⁺ from the extracellular side into the selectivity filter of KcsA. The entry process of an extracellular ion is examined in the presence of two additional K⁺ in the pore, and the three-ion potential of mean force is computed using extensive all-atom umbrella sampling molecular dynamics simulations. A comparison of the potentials of mean force yields a number of important results. First, the free energy minima corresponding to configurations with extracellular K⁺ or Na⁺ in binding site S₀ or S₁ are similar in depth, suggesting that the thermodynamic selectivity governed by the free energy minima for those two binding sites is insignificant. Second, the free energy barriers between stable multi-ion configurations are generally higher for Na⁺ than for K⁺, implying that the kinetics of ion conduction is slower when a Na⁺ enters the pore. Third, the region corresponding to binding site S₂ near the center of the narrow pore emerges as the most selective for K⁺ over Na⁺. In particular, while there is a stable minimum for K⁺ in site S₂, Na⁺ faces a steep free energy increase with no local free energy well in this region. Lastly, analysis shows that selectivity is not correlated with the overall coordination number of the ion entering the pore, but is predominantly affected by changes in the type of coordinating ligands (carbonyls versus water molecules). These results further highlight the importance of the central region near binding site S₂ in the selectivity filter of K⁺ channels.     

The Effects of Several Alcohols on the Properties of the Squid Giant Axon

The effects of several alcohols on the resting potential, action potential, and voltage-clamp currents of the squid giant axon have been measured. All the alcohols employed are similar in that they depress maximum sodium conductance much more than maximum potassium conductance. Octyl alcohol differs from the others (C₂ through C₅) in that it has less tendency to depolarize the axon. Depolarization is always accompanied by a decrease of g_K near the resting potential, such that the ratio g_K/g_leak is decreased. Steady-state inactivation of the sodium ion current is unaffected by alcohols, as is membrane capacity. Resting membrane conductance is usually decreased by alcohols. The findings are discussed in relation to work on monomolecular films.     

Interaction of Tetraethylammonium Ion Derivatives with the Potassium Channels of Giant Axons

A number of compounds related to TEA⁺ (tetraethylammoniumion) were injected into squid axons and their effects on g_K (the potassium conductance) were determined. In most of these ions a quaternary nitrogen is surrounded by three ethyl groups and a fourth group that is very hydrophobic. Several of the ions cause inactivation of g_K, a type of ionic gating that is not normally seen in squid axon; i.e., after depolarization g_K increases and then spontaneously decreases to a small fraction of its peak value even though the depolarization is maintained. Observations on the mechanism of this gating show that (a) QA (quaternary ammonium) ions only enter K⁺ channels that have open activation gates (the normal permeability gates). (b) The activation gates of QA-occluded channels do not close readily. (c) Hyperpolarization helps to clear QA ions from the channels. (d) Raising the external K⁺ concentration also helps to clear QA ions from the channels. Observations (c) and (d) strongly suggest that K⁺ ions traverse the membrane by way of pores, and they cannot be explained by the usual type of carrier model. The data suggest that a K⁺ pore has two distinct parts: a wide inner mouth that can accept a hydrated K⁺ ion or a TEA⁺-like ion, and a narrower portion that can accept a dehydrated or partially dehydrated K⁺ ion, but not TEA⁺.     

Characteristics of antibody inhibition of rat kidney (Na+−K+)-ATPase

Summary Antibodies which were raised against highly purified membrane-bound (Na⁺–K⁺)-ATPase from the outer medulla of rat kidneys inhibit the (Na⁺–K⁺)-ATPase activity up to 95%. The antibody inhibition is reversible. The time course of enzyme inhibition and reactivation is biphasic in semilogarithmic plots.In the purified membrane-bound (Na⁺–K⁺)-ATPase negative cooperativity was observed (a) for the ATP dependence of the (Na⁺–K⁺)-ATPase activity (n=0.86), (b) for the ATP binding to the enzyme (n=0.58), and (c) for the ouabain inhibition of the (Na⁺–K⁺)-ATPase activity (n=0.77). By measuring the Na⁺ dependence of the (Na⁺–K⁺-ATPase reaction, a positive homotropic cooperativity (n=1.67) was found.As reactivation of the antibody-inhibited enzyme proceeds very slowly (t _0.5=5.2hr), it was possible to measure characteristics of the antibody-(Na⁺–K⁺)-ATPase complex: The antibodies exerted similar effects on the ATP dependence of the (Na⁺–K⁺)-ATPase reaction and on the ATP binding of the enzyme.V _max of the (Na⁺–K⁺)-ATPase reaction and the number of ATP binding sites were reduced whileK _{0.5 ATP} for the (Na⁺–K⁺)-ATPase activity and for the ATP binding were increased by the antibodies. The Hill coefficients for the ATP binding and for the ATP dependence of the enzyme activity were not significantly altered by the antibodies. The antibodies increased theK _0.5 value for the Na⁺ stimulation of the (Na⁺–K⁺)-ATPase activity, but they did not alter the homotropic interactions between the Na⁺-binding sites. The negative cooperativity which was observed for the ouabain inhibition of the (Na⁺–K⁺)-ATPase activity was abolished by the antibodies.The data are tentatively explained by the following model: The antibodies bind to the (Na⁺–K⁺)-ATPase from the inner membrane side, reduce the ATP binding symmetrically at the ATP binding sites and reduce thereby also the (Na⁺–K⁺)-ATPase activity of the enzyme. The antibodies may inhibit the ATP binding by a direct interaction or by means of a conformational change at the ATP binding sites. This may possibly also lead to the alteration of the Na⁺ dependence of the (Na⁺–K⁺)-ATPase activity and to the observed alteration of the dose response to the ouabain inhibition.     

Overexpression of Na+/K+-ATPase Parallels the Increase in Sodium Transport and Potassium Recycling in an In Vitro Model of Proximal Tubule Cellular Ageing

Na⁺/K⁺-ATPase plays a key role in the transport of Na⁺ throughout the nephron, but ageing appears to be accompanied by changes in the regulation and localization of the pump. In the present study, we examined the effect of in vitro cell ageing on the transport of Na⁺ and K⁺ ions in opossum kidney (OK) cells in culture. Cells were aged by repeated passing, and Na⁺/K⁺-ATPase activity and K⁺ conductance were evaluated using electrophysiological methods. Na⁺K⁺-ATPase α₁– and β₁-subunit expression was quantified by Western blot techniques. Na⁺/H⁺ exchanger activity, changes in membrane potential, cell viability, hydrogen peroxide production and cellular proliferation were determined using fluorimetric assays. In vitro cell ageing is accompanied by an increase in transepithelial Na⁺ transport, which results from an increase in the number of Na⁺/K⁺-ATPase α₁- and β₁-subunits, in the membrane. Increases in Na⁺/K⁺-ATPase activity were accompanied by increases in K⁺ conductance as a result of functional coupling between Na⁺/K⁺-ATPase and basolateral K⁺ channels. Cell depolarization induced by both KCl and ouabain was more pronounced in aged cells. No changes in Na⁺/H⁺ exchanger activity were observed. H₂O₂ production was increased in aged cells, but exposure for 5 days to 1 and 10 μM of H₂O₂ had no effect on Na⁺/K⁺-ATPase expression. Ouabain (100 nM) increased α₁-subunit, but not β₁-subunit, Na⁺/K⁺-ATPase expression in aged cells only. These cells constitute an interesting model for the study of renal epithelial cell ageing.