The effect of surface charge density on valinomycin-K+ complex formation in model membranes

The model membrane approach was used to investigate the surface charge effect on the ion-antibiotic complexation process. Mixed monolayers of valinomycin and lipids were spread on subphases containing K⁺ or Na⁺. The surface charge density was modified by spreading ionizable valinomycin analogs on aqueous subphases of different pH or by changing the nature of the lipid (neutral, negatively charged) in the mixed film. Surface pressure and surface potential measurements demonstrated that a neutral lipid (phosphatidylcholine) or positively charged valinomycin analogs didn't enhance the antibiotic complexing capacity. However, a maximal complexation is reached for a critical lipid concentration in the valinomycin-phosphatidylserine mixed film. The role of the surface charge on the valinomycin complexing properties was examined in terms of the Gouy-Chapman theory. As a consequence of the negative charge of the lipid monolayer, the K⁺ concentration near the surface is larger than the bulk concentration, by a Boltzmann factor. A good agreement was observed between the experimental results and the theoretical predictions. Conductance measurements of asymmetric bilayers containing a neutral lipid (egg lecithin) on one side and a negatively charged lipid (phosphatidylserine) on the other, confirm the role of the surface charge. Indeed, addition of K⁺ to the neutral side of the bilayer containing valinomycin had no effect on the conductance whereas addition of K⁺ to the charged side of the bilayer caused a 80-fold conductance increase.     

Competitive membrane adsorption of Na+, K+, and Ca2+ in smooth muscle cells

Summary A theory for Na⁺, K⁺ and Ca²⁺ competitive adsorption to a charged membrane is used to explain a number of experimental observations in smooth muscle. Adsorption is described by Langmuir isotherms for mono- and divalent cations which in turn are coupled in a self-consistent way to the bulk solution through the diffuse double layer theory and the Boltzman equations. We found that the dissociation constants for binding of Na⁺, K⁺ and Ca²⁺ in guinea pig taenia coli areca. 0.009, 1.0, and 4×10^–8 m, respectively. Furthermore, the effect of a Ca²⁺ pump that maintains free surface Ca²⁺ concentration constant is investigated. A decrease in intracellular Na⁺ content results in an increased Ca²⁺ uptake; part of this uptake is due to an increase in surface-bound Ca²⁺ in an intracellular compartment which is in contact with the myofilaments. Variations in the amount of charge available to bind Ca²⁺ and the surface charge density are studied and their effect interpreted in terms of different pharmacological agents.     

Surface charge near the cardiac inward-rectifier channel measured from single-channel conductance

Summary The conductance of a channel to permeable ions depends on the number of ions near the mouth of the pore. Surface charge controls the local concentration, and impermeable cations can modify this charge. Correlating channel conductance with the concentration of impermeable cations therefore determines the local charge near the open pore. This paper presents data from cell-attached patches on embryonic chick ventricle cells, and it uses the conductance of inward-rectifier channels in the patch (in 100mm K, with various concentrations of Na, Ca, Ba, and Mg) to estimate the local surface potential. The results indicate the presence of ionized residues near the mouth of the channel. Using the Boltzmann equation and the Gouy-Chapman relation, the surface potential due to these residues (in 100K/33Na/0Ca/0Ba/0Mg) is –40 mV, and the charge density is –0.25e/nm².     

Proton Inhibition of Sodium Channels: Mechanism of Gating Shifts and Reduced Conductance

Extracellular acidosis affects both permeation and gating of the expressed rat skeletal muscle Na⁺ channel (μ1). Reduction of the extracellular pH produced a progressive decrease in the maximal whole-cell conductance and a depolarizing shift in the whole-cell current-voltage relationship. A smaller depolarizing shift in the steady-state inactivation curve was observed. The pK of the reduction of maximal conductance was 6.1 over the pH range studied. An upper limit estimate of the pK of the shift of the half-activation voltage was 6.1. The relative reduction in the maximal whole-cell conductance did not change with higher [Na⁺] _o . The conductance of single fenvalerate-modified Na⁺ channels was reduced by extracellular protons. Although the single-channel conductance increased with higher [Na⁺] _o , the maximal conductances at pH 7.6, 7.0 and 6.0 did not converge at [Na⁺] _o up to 280 mm, inconsistent with a simple electrostatic effect. A model incorporating both Na⁺ and H⁺ binding in the pore and cation binding to a Gouy-Chapman surface charge provided a robust fit to the single-channel conductance data with an estimated surface charge density of 1e⁻/439?². Neither surface charge nor proton block alone suffices to explain the effects of extracellular acidosis on Na⁺ channel permeation; both effects play major roles in mediating the response to extracellular pH. Received: 14 May 1996/Revised: 19 September 1996     

Divalent cation binding to phospholipids: An EPR study

Summary Divalent cation association to sonicated phospholipid liposomes has been examined with electron paramagnetic spectroscopy. Spectra were obtained suggesting that, in some cases, divalent cations associated with acidic phospholipid head groups are highly mobile.Using the amplitude of its characteristic sextet signal as a measure of free Mn(H₂O) ₆ ⁺⁺ , the apparent affinities of cardiolipin and phosphatidylserine for Mn²⁺ were measured as a function of monovalent electrolyte. Monovalent cations having smaller nonhydrated radii were more effective in displacing Mn from the phospholipids. Under conditions of low divalent cation concentrations, it is shown that the Gouy-Chapman diffuse double layer theory predicts a Mn-affinity (K _A ) inversely proportional to the square of monovalent salt concentration. Although this relationship was closely obeyed for Mn binding to cardiolipin, the fall-off inK _A with added sodium chloride was slower in the cases of Mn binding to phosphatidylserine or phosphatidic acid.When phosphatidylcholine or cholesterol was incorporated into mixed vesicles along with a fixed amount of charged phospholipid, the Mn-binding strength was roughly proportional to the weight fraction of the latter. This result is consistent with: (1) a random dispersal of lipids in the bilayer, and (2) a 1:2 divalent cation-phospholipid interaction.     

Effects of Cd++ on short-circuit current across epithelial membranes

Summary Cadmium ion (Cd⁺⁺) was found not to inhibit active sodium transport across the isolated frog skin when added in 10^–3 m concentration to the basal-lateral surface. The same Cd⁺⁺ concentration similarly had no effect on Na⁺ transport across the isolated epithelial cell layer from the frog skin, although this dose of Cd⁺⁺ did inhibit Na⁺ transport across the frog urinary bladder and large intestine. When 10^–3 m Cd⁺⁺ was added to the apical surface of the isolated frog skin or to the isolated epithelial cells from the frog skin, sodium transport was reversibly stimulated, in contrast to the irreversible inhibition noted above. If equimolar cysteine was added with Cd⁺⁺ to the apical surface of the skin, however, active Na⁺ transport was irreversibly inhibited. In conjunction with the inhibition produced by equimolar Cd⁺⁺ and cysteine, isotopic Cd⁺⁺ permeation into the tissue was three times higher when added with cysteine than in the absence of cysteine. Thus, the effects of Cd⁺⁺ on epithelial Na⁺ transport is variable according to the epithelium studied and the presence of potential carrier molecules.     

Barium modifies the concentration dependence of active potassium transport by insect midgut

Summary The rate of active K⁺ transport by the isolated lepidopteran midgut shows a rectangular hyperbolic relation to [K⁺] over the range 20 to 70mm K⁺ in the absence of any divalent cation. Addition of Ba⁺⁺ to the hemolymph (K⁺ uptake) side introduces a linear component to the concentration dependence, such that active K^– transport is decreased at [K⁺] of 55mm or less, but increased transiently at higher [K⁺]. As [Ba⁺⁺] is increased over the range 2 to 8mm the linear component increases and the saturating component decreases; in 8mm Ba⁺⁺ the concentration dependence is dominated by the linear component. The effect of Ba⁺⁺ cannot easily be accounted for by simple competition with K⁺ for basal membrane uptake sites. Similar effects might be exercised by other alkali earth cations, since the concentration dependence of active K⁺ transport possesses a substantial linear component in solutions containing 5mm Ca⁺⁺ and 5mm Mg⁺⁺ (the alkali earth metal concentrations of standard lepidopteran saline).     

Binding and Electrostatic Attraction of Lanthanum (La3+) and Aluminum (Al3+) to Wheat Root Plasma Membranes

A general model for the sorption of trivalent cations to wheat-root (Triticum aestivum L cv. Scout 66) plasma membranes (PM) has been developed and includes the first published coefficients for La³⁺ and Al³⁺ binding to a biological membrane. Both ions are rhizotoxic, and the latter ion is the principal contributor to the toxicity of acidic soils around the world. The model takes into account both the electrostatic attraction and the binding of cations to the negatively charged PM surface. Ion binding is modeled as the reaction P ⁻+I ^Z⇌PI ^{Z −1} in which P ⁻ represents a negatively charged PM ligand, located in an estimated area of 540 ?², and I ^Z represents an ion of charge Z. Binding constants for the reaction were assigned for K⁺ (1 m ⁻¹) and Ca²⁺ (30 m ⁻¹) and evaluated experimentally for La³⁺ (2200 m ⁻¹) and H⁺ (21,500 m ⁻¹). Al sorption is complicated by Al³⁺ hydrolysis that yields hydroxoaluminum species that are also sorbed. Binding constants of 30 and 1 m ⁻¹ were assigned for AlOH²⁺ and Al(OH)⁺ ₂, respectively, then a constant for Al³⁺ (20,000 m ⁻¹) was evaluated experimentally using the previously obtained values for K⁺, Ca²⁺ and H⁺ binding. Electrostatic attraction was modeled according to Gouy-Chapman theory. Evaluation of parameters was based upon the sorption of ions to PM vesicles suspended in solutions containing variable concentrations of H⁺, Ca²⁺ and La³⁺ or Al³⁺. Use of small volumes, and improved assay techniques, allowed the measurement of concentration depletions caused by sorption to vesicles. Some independent confirmation of our model is provided by substantial agreement between our computations and two published reports of La³⁺ effects upon zeta potentials of plant protoplasts. The single published report concerning the electrostatic effects of Al on cell membranes is in essential agreement with the model. Received: 6 January 1997/Revised: 6 June 1997     

Electrical properties of the plasma membrane of microplasmodia ofPhysarum polycephalum

Summary Microplasmodia ofPhysarum polycephalum have been investigated by conventional electrophysiological techniques. In standard medium (30mm K⁺, 4mm Ca⁺⁺, 3mm Mg⁺⁺, 18mm citrate buffer, pH 4.7, 22°C), the transmembrane potential differenceV _m is around –100 mV and the membrane resistance about 0.25 m².V _m is insensitive to light and changes of the Na⁺/K⁺ ratio in the medium. Without bivalent cations in the medium and/or in presence of metabolic inhibitors (CCCP, CN^–, N ₃ ^– ),V _m drops to about 0 mV. Under normal conditions,V _m is very sensitive to external pH (pH _o ), displaying an almost Nernstian slope at pH _o =3. However, when measured during metabolic inhibition,V _m shows no sensitivity to pH _o over the range 3 to 6, only rising (about 50 mV/pH) at pH _o =6. Addition of glucose or sucrose (but not mannitol or sorbitol) causes rapid depolarization, which partially recovers over the next few minutes. Half-maximal peak depolarization (25 mV with glucose) was achieved with 1mm of the sugar. Sugar-induced depolarization was insensitive to pH _o . The results are discussed on the basis of Class-I models of charge transport across biomembranes (Hansen, Gradmann, Sanders and Slayman, 1981,J. Membrane Biol. 63:165–190). Three transport systems are characterized: 1) An electrogenic H⁺ extrusion pump with a stoichiometry of 2 H⁺ per metabolic energy equivalent. The deprotonated form of the pump seems to be negatively charged. 2) In addition to the passive K⁺ pathways, there is a passive H⁺ transport system; here the protonated form seems to be positively charged. 3) A tentative H⁺-sugar cotransport system operates far from thermodynamic equilibrium, carrying negative charge in its deprotonated states.     

Effects of quinine on Ca++-induced K+ efflux from human red blood cells

Summary The Ca⁺⁺-mediated increase in K⁺-permeability of intact red blood cells (Gardos effect) was initiated by exposing cells to known concentrations of Ca⁺⁺ (using EGTA buffers) in the presence of the ionophore A23187. The potency of quinine, an inhibitor of the response, was found to depend on the external K⁺ concentration. In K⁺-free solutions the concentration of quinine to achieve 50% inhibition (K ₅₀) was 5 m, but at 5mm K⁺ the required concentration was increased 20-fold to 100 m. An increase in internal Na⁺ had the opposite effect, allowing a high potency of quinine despite the presence of external K⁺. Alterations in the internal K⁺ level, on the other hand, were without effect on theK ₅₀, suggesting that the membrane potential is not a factor. This conclusion is supported by the lack of effect on quinine inhibition of substitution of Cl^– by NO ₃ ^– , a considerably more permeant anion. The data are consistent with the hypothesis that quinine inhibits by competitively displacing K⁺ from an external binding site, the reported K⁺-activation site for the Ca⁺⁺-mediated K⁺-permeability.     

Calcium entry in rabbit corneal epithelial cells: Evidence for a nonvoltage dependent pathway

We performed experiments to elucidate the calcium influx pathways in freshly dispersed rabbit corneal epithelial cells. Three possible pathways were considered: voltage-gated Ca⁺⁺ channels, Na⁺/Ca⁺⁺ exchange, and nonvoltage-dependent Ca⁺⁺-permeable channels. Whole cell inward currents carrying either Ca⁺⁺ or Ba⁺⁺ were not detected using voltage clamp techniques. We also used imaging technology and the Ca⁺⁺-sensitive ratiometric dye fura 2 to measure changes in intracellular Ca⁺⁺ concentration ([Ca]_i). Bath perfusion with NaCl Ringer's solution containing the calcium channel agonist Bay-K-8644 (1 m), or Ni⁺⁺ (40 m), a blocker of many voltage-dependent calcium channels, did not affect [Ca⁺⁺]_i. Membrane depolarization with a KCl Ringer's bath solution resulted in a decrease in [Ca⁺⁺]_i. These results are inconsistent with the presence of voltage gated Ca⁺⁺ channels. Nonvoltage gated Ca⁺⁺ entry, on the other hand, would be reduced by membrane depolarization and enhanced by membrane hyperpolarization. Agents which hyperpolarize via stimulation of K⁺ current, such as flufenamic acid, resulted in an increase in ratio intensity. The cells were found to be permeable to Mn⁺⁺ and bath perfusion with 5 mm Ni⁺⁺ decreased [Ca⁺⁺]_i suggesting that the Ca⁺⁺ conductance was blocked. These results are most consistent with a nonvoltage gated Ca⁺⁺ influx pathway. Finally, replacing extracellular Na⁺ with Li⁺ resulted in an increase in [Ca⁺⁺]_i if the cells were first Na⁺-loaded using the Na⁺ ionophore monensin and ouabain, a Na⁺-K⁺-ATPase inhibitor. These results suggest that Na⁺/Ca⁺⁺ exchange may also regulate [Ca⁺⁺] in this cell type.The authors are grateful to Chris Bartling for expert technical assistance with the imaging experiments, Helen Hendrickson for cell preparation, and Jonathon Monck for helpful discussions regarding imaging technology. This work was supported by National Institutes of Health grants EYO3282, EYO6005, DK08677, and an unrestricted award from Research to Prevent Blindness.     

Triple helix formation and disulphide bonding during the biosynthesis of glomerular basement membrane collagen.

White erythrocyte membranes, or ghosts, were monoconcave discocytes when incubated in 50mM N-tris (hydroxymethyl) methyl-2-aminoethane sulfonic acid titrated to pH 7.4 with triethanolamine. If 3mM MgCl₂ was included in the incubation medium, the ghosts were predominantly echinocytes. The echinocytic form could also be induced by Co⁺⁺, Ni⁺⁺, Li⁺, Na⁺, K⁺, $\text{NH}{}_4{}^{\mathrm{+}}$ and tetramethylammonium ion, all as chloride salts. The concentration of cation necessary for 50% of the ghosts to be echinocytes was correlated with the hydrated charge density of the cation with the most highly charged cations being the most effective. The cations Ca⁺⁺, Sr⁺⁺, Ba⁺⁺ and La⁺⁺⁺, (also as chloride salts) did not induce the normal echinocytic form, but at high levels induced a few misshapen forms with some resemblance to echinocytes. Instead Ca⁺⁺, Sr⁺⁺, Ba⁺⁺ and La⁺⁺⁺ suppressed the formation of echinocytes in the presence of Mg⁺⁺ and other ions. This suggests the presence of a specific Ca⁺⁺ binding site important to shape control in the erythrocyte membrane.     

Donnan membrane equilibrium is not directly applicable to distributions of ions and water in gels or cells

Equilibration of ions and water with a charged gel does not follow the simple equations of the classical Gibbs-Donnan membrane equilibrium. Partition of ions between the gel and the external solution show specific effects, which require that activity coefficients are different in the two compartments. Highly hydrated ions, such as Na⁺ and H⁺ are accumulated into the gel water, whereas less highly hydrated ions, such as K⁺ and NH₄⁺ accumulate in the external water. This selectivity is the obverse of that found for gels containing low-density, expanded water. Water in a charged gel equilibrated with solutions of MgCl₂ was found to be more dense than bulk water at the same temperature. It is proposed that gels imbibe water to maximize the entropy of the system. Ions and water then equilibrate under those constraints. The chemical potential of water in the two compartments equalizes by an increase in density in the compartment of higher osmolality (the charged gel) and a decrease in density in the compartment of lower osmolality (the external solution). Electrolytes equilibrate so that macroscopic electroneutrality is conserved, and the chemical potential of an electrolyte is the same in each compartment. Because activity coefficients are different in the two compartments this results in asymmetric distributions of ions.Because real gels usually contain both charged and hydrophobic regions of surface, populations of water molecules of different density coexist even in very small pores. This accounts for the common failure to detect this phenomenon experimentally.     

The influence of surface charges on quaternary ammonium block of shaker K+ channels

Block of K⁺ channels can be influenced by the ability of charged residues on the protein surface to accumulate cationic blocking ions to concentrations greater than those in bulk solution. We examined the ionic strength dependence of extracellular block of Shaker K⁺ channels by tetraethylammonium ions (TEA⁺) and by a trivalent quaternary ammonium ion, gallamine³⁺. Wild-type and mutant channels were expressed in Xenopus oocytes and currents recorded with the cut-open oocyte technique. Channel block by both compounds was substantially increased when the bathing electrolyte ionic strength was lowered, but with a much larger effect for trivalent gallamine. These data were quantitatively well described by a simple electrostatic model, accounting for accumulation of blocking ions near the pore of the channel by surface charges. The surface charge density of the wild-type channel consistent with the results was −0.1 e nm⁻². Shaker channels with T449Y mutations have an increased affinity for both TEA and gallamine but the ionic strength dependence of block was described with the same surface charge density as wild-type channels. Much of the increased sensitivity of Shaker K⁺ channels to gallamine may be due to a larger local accumulation of the trivalent ion. The negative charge at position 431 contributes to the sensitivity of channels to TEA (MacKinnon & Yellen, 1990). A charge reversal mutation at this location had little effect on the ionic strength dependence of quaternary ammonium ion block, suggesting that the charge on this amino acid may directly affect binding affinity but not local ion accumulation. Received: 7 December 2000/Revised: 27 April 2001     

An L-type Calcium Channel in Renal Epithelial Cells

A voltage-activated Ca⁺⁺ channel has been identified in the apical membranes of cultured rabbit proximal tubule cells using the patch-clamp technique. With 105 mm CaCl₂ solution in the pipette and 180 NaAsp in the bath, the channel had a conductance of 10.4 ± 1.0 pS (n= 8) in on-cell patches, and 9.8 ± 1.1 pS (n= 8) in inside-out patches. In both on-cell and inside-out patches, the channel is active by membrane depolarization. For this channel, the permeation to Ba⁺⁺ and Ca⁺⁺ is highly selective over Na⁺ and K⁺ (P_Ca(Ba):P_Na(K) >200:1). The sensitivity to dihydropyridines is similar to that for L-type channels where the channel was blocked by nifedipine (10 μm), and activated by Bay K 8644 (5 μm). When activated by Bay K 8644, the channel showed subconductance levels. Treatment with forskolin (12.5 μm), phorbol ester (1 μm), or stretching (40 cm water) did not activate this channel. These results indicate that this Ca⁺⁺ channel is mostly regulated by membrane voltage, and appears to be an epithelial class of L-type Ca⁺⁺ channel. As such, it may participate in calcium reabsorption during periods of enhanced sodium reabsorption, or calcium signaling in volume regulation, where membrane depolarization occurs for prolonged periods. Received: 1 April 1996/Revised: 5 August 1996     

Electrokinetic Properties of the Sarcoplasmic Reticulum Membrane Obtained from Reconstitution Studies

Electrophoretic mobility data of SR vesicles reconstituted with uncharged and two mixtures of charged and uncharged lipids (Brethes, D., Dulon, D., Johannin, G., Arrio, B., Gulik-Krzywicki, T., Chevallier, J. 1986. Study of the electrokinetic properties of reconstituted sarcoplasmic reticulum vesicles. Arch. Biochem. Biophys. 246:355–356) were analyzed in terms of four models of the membrane-water interface: (I) a smooth, negatively charged surface; (II) a negatively charged surface of lipid bilayer covered with an electrically neutral surface frictional layer; (III) an electrically neutral lipid bilayer covered with a neutral frictional layer containing a sheet of negative charge at some distance above the surface of the bilayer; (IV) an electrically neutral lipid bilayer covered with a homogeneously charged frictional layer. The electrophoretic mobility was predicted from the numerical integration of Poisson-Boltzmann and Navier-Stokes equations. Experimental results were consistent only with predictions based on Model-III with charged sheet about 4 nm above the bilayer and frictional layer about 10 nm thick. Assuming that the charge of the SR membrane is solely due to that on Ca⁺⁺-ATPase pumps, the dominant SR protein, the mobility data of SR and reconstituted SR vesicles are consistent with 12 electron charges/ATPase. This value compares well to the net charge of the cytoplasmic portion of ATPase estimated from the amino acid sequence (-11e). The position of the charged sheet suggests that the charge on the ATPase is concentrated in the middle of the cytoplasmic portion. The frictional layer of SR can be also assigned to the cytoplasmic portion of Ca⁺⁺-ATPase. The layer has been characterized with hydrodynamic shielding length of 1.1 nm. Its thickness is comparable to the height of the cytoplasmic portion of Ca⁺⁺-ATPase. Received: 15 June 1998/Revised: 8 October 1998     

Counterion exchange reactions on DNA: Monte Carlo and Poisson-Boltzmann analysis

In solutions containing DNA and cations of more than one type, the competitive interactions of these cations with DNA can be modeled as an ion exchange process that can be described quantitatively by means of the theoretical approach reported in this paper. Under conditions of experimental interest the radial distribution function of each type of counterion is calculated from the results of canonical Monte Carlo (MC) simulations using the primitive model for DNA (having a helical charge distribution) and for the electrolyte ions. These ions consist of monovalent coions, monovalent counterions intended to represent Na⁺, and counterions of a second type designated M^z+, having variable size and charge (z ≥ 1). The competitive association of these counterions with DNA is described in terms of D, a parameter analogous to an ion exchange equilibrium quotient. Values of D are calculated from the results of our MC simulations and compared with corresponding predictions of the Poisson–Boltzmann (PB) cell model and with results inferred from analyses of previously published nmr measurements. Over typical experimental concentration ranges (0.02M < [Na⁺] < 0.20M, 0.001 < [M^z+] < 0.160M), D^MC and D^PB both are predicted to be relatively independent of the bulk ion concentrations. For various specifications of the size and charge of the competing cation (M^z+), D^MC and D^PB exhibit similar trends, although the MC simulations consistently predict that the cations bearing a higher charge density than that of Na⁺ are somewhat stronger competitors than indicated by the PB calculations. For monovalent and divalent competitors of varying radii, theoretical predictions of D are compared with values obtained by fitting nmr measurements. If the hard-sphere radii specified in the simulations are the (hydrated) ionic radii determined from conductance measurements, then the MC predictions and the corresponding nmr results are in reasonable agreement for various monovalent competitors and for a divalent polyamine, but not for Ca²⁺ and Mg²⁺.     

9-Aminoacridine fluorescence changes as a measure of surface charge density of the thylakoid membrane

1. When suspended in a low cation-containing medium, chloroplast thylakoid membranes and carboxymethyl-cellulose particles quench the fluorescence from 9-aminoacridine (Searle, G.F.W. and Barber, J. (1978) Biochim. Biophys. Acta 502, 309–320).2. Relief of this quenching is achieved by adding cations to the suspension medium with the order of effectiveness being C³⁺ > C²⁺ > C⁺, indicating that the fluorescence acts as an indicator of the surface electrical potential.3. Using the Gouy-Chapman theory, the differential effect of divalent (methyl viologen) and monovalent (K⁺) cations has been used to calculate surface charge densities.4. The calculations indicate that the surface charge density on the thylakoids significantly increases when cations are added to the low cation-containing medium. Under the same conditions the surface charge density of glutaralde-hyde-fixed thylakoids and carboxymethyl-cellulose particles remained essentially constant.5. It is argued that the 9-aminoacridine technique is able to probe localized areas on the membrane surface and that the variability of the surface charge density of untreated thylakoids may be due to redistribution of charges associated with membrane stacking as suggested by Barber and Chow (Barber, J. and Chow, W.S. (1979) FEBS Lett. 105, 5–10).     

Electrical effects of potassium and bicarbonate on proximal tubule cells ofNecturus

Summary The effects of stepwise concentration changes of K⁺ and HCO ₃ ^– in the basolateral solution on the basolateral membrane potential (V _bl) of proximal tubule cells of the doubly-perfusedNecturus kidney were examined using conventional microelectrodes. Apparent transference numbers were calculated from changes inV _bl after alterations in external K⁺ concentration from 1.0 to 2.5mm (t _{K, 1.0–2.5}), 2.5 to 10, and in external HCO ₃ ^– concentration (at constant pH) from 5 to 10mm (t _{HCO3, 5–10}), 10 to 20, or 10 to 50.t _{K, 2.5–10} was 0.38±0.02 under control conditions but was sharply reduced to 0.08±0.03 (P>0.001) by 4mm Ba⁺⁺. This concentration of Ba⁺⁺ reducedV _bl by 9±1 mV (at 2.5 external K⁺). Perfusion with SITS (5×10^–4 m) for 1 hr hyperpolarizedV _bl by 10±3 mV and increasedt _{K, 2.5–10} significantly to 0.52±0.01 (P<0.001). Ba⁺⁺ application in the presence of SITS depolarizedV _bl by 22±3 mV. In control conditionst _{HCO3, 10–50} was 0.63±0.05 and was increased to 0.89±0.07 (P<0.01) by Ba⁺⁺ but was decreased to 0.14±0.02 (P<0.001) by SITS. In the absence of apical and basolateral chloride, the response ofV _bl to bicarbonate was diminished but still present (t _{HCO3, 10–20} was 0.35±0.03). Intracellular pH, measured with liquid ion-exchange microelectrodes, increased from 7.42±0.19 to 7.57±0.17 (P<0.02) when basolateral bicarbonate was increased from 10 to 20mm at constant pH. These data show that the effects of bicarbonate onV _bl are largely independent of effects on the K⁺ conductance and that there is a significant current-carrying bicarbonate pathway in the basolateral membrane. Hence, both K⁺ and HCO ₃ ^– gradients are important in the generation ofV _bl, and their relative effects vary reciprocally.