Formation of large,ion-permeable membrane channels by the matrix protein (porin) of Escherichia coli

One of the major proteins of the outer membrane of Escherichia coli, the matrix protein (porin), has been isolated by detergent solubilisation. When the protein is added in concentrations of the order of 10 ng/cm³ to the outer phases of a planar lipid bilayer membrane, the membrane conductance increases by many orders of magnitude. At lower protein concentrations the conductance increases in a stepwise fashion, the single conductance increment being about 2 nS ($\text{1}\text{nS}\text{= 10}{}^{\mathrm{?9}}\text{siemens}\text{= 10}{}^{\mathrm{?9}}\text{Ω}{}^{\mathrm{?1}}$) in 1 M KCl. The conductance pathway has an ohmic current vs. voltage character and a poor selectivity for chloride and the alkali ions. These findings are consistent with the assumption that the protein forms large aqueous channels in the membrane. From the average value of the single-channel conductance a channel diameter of about 0.9 nm is estimated. This channel size is consistent with the sugar permeability which has been reported for lipid vesicles reconstituted in the presence of the protein.     

Effect of angiotensin II on artificial lipid membranes

(5-Isoleucine)-angiotensin II applied to black lipid membranes produced current fluctuations varying between $\text{Δ>G = 5 · 10}{}^{\mathrm{?11}}\text{Ω}{}^{\mathrm{?}}$ and 3.5 · 10^?10 Ω^?1. These fluctuations depend on the voltage and the hydrostatic pressure. The membrane resistance is lowered by $\text{Δ>R = 6.1 · 10}{}^7\text{Ω · cm}{}^2$. With (5-isoleucine, 8-leucine)-angiotensin II the jumps are of a single amplitude ($\text{Δ>G = 2 · 10}{}^{\mathrm{?10}}\text{Ω}{}^{\mathrm{?1}}$). In both cases water and ions are transported across the membrane.     

Local measurement of lateral motion in erythrocyte membranes by photobleaching technique

The lateral diffusion coefficients ($\text{D}$) of the molecular fluorescence probe 3,3′-dioctadecylindocarbocyanine iodide (DII) in the membrane of discoid erythrocyte ghosts has been measured with the photobleaching technique between 7°C and 40°C. A fluorescence microscope which allows bleaching experiments within small local fields (approx. 1 μm²) at high magnification (X1600) has been used for these measurements. The diffusion coefficient increases from $\text{D = 9 · 10}{}^{\mathrm{?10}}\text{cm}{}^2\text{/s}$ to $\text{D = 7.5 · 10}{}^{\mathrm{?9}}\text{cm}{}^2\text{/s}$ from 7 to 40°C. An increase in membrane fluidity between 12°C and 17°C indicates a conformational change of the lipid bilayer moiety in this temperature region. The diffusion coefficient measured in the regions between the spicules of echinocytes is appreciably smaller than in the untransformed discoid ghosts. In the myelin tubes originating from cells, the lateral diffusion is somewhat larger (about a factor of 2) than in the non-transformed ghosts. With the fluorescence probe technique the rate of growth of myelin tubes of 0.3 μm diameter has been estimated.     

Incorporation into lipid bilayer membranes of a photo-sensitive pigment from the honeybee compound eye

An increase of electrical conductance up to a factor $\text{10}{}^2\text{-5·10}{}^2$ was obtained by adding, in the dark, the honeybee photopigment to a positively charged lipid bilayer. The increase in conductance was made slower by illuminating the system during the incorporation of the protein into the membrane and it was negligible when the photopigment was bleached before the incorporation. The interaction of the photopigment with the membrane is tentatively interpreted in terms of formation of channels.     

The potential-dependent K+ channel in molluscan neurones is organized in a cluster of elementary channels

Single potential-dependent K⁺ channels were studied using the patch-voltage-clamp method. Two types of channel with identical, but oppositely directed, potential dependences were found. The channels of the first type (slow channels) are assumed to be responsible for the outward rectification. The properties of the channels of the second type (fast channels) are similar to those of the K⁺ channels in neurone soma which create the fast transient currents. The kinetic characteristics of both types of channel are presented. The conductances of slow and fast K⁺ channels are approx. 30 and 40 pS, respectively, at zero membrane potential and a K⁺ concentration of 50 mmol/l at the inner side of the membrane. The following sequence of channel selectivity with respect to monovalent cations was found: $\text{Tl}{}^{\mathrm{+}}\text{>}\text{K}{}^{\mathrm{+}}\text{>}\text{Rb}{}^{\mathrm{+}}\text{?}\text{Cs}{}^{\mathrm{+}}\text{?}\text{Li}{}^{\mathrm{+}}\text{?}\text{Na}{}^{\mathrm{+}}$. The probability of the channel open state monotonically decreases with free Ca²⁺ concentration at the inside membrane surface for both types of channel. It was found that the channels have discrete and multiple conductance substrates. It is supposed that a unitary K⁺ channel consists of approx. 16 elementary ones with conductances of approx. 2 pS (slow channels) and approx. 2.5 pS (fast channels) at zero potential. At + 100 mV the elementary conductances are equal to approx. 4 and 5.5. pS, respectively. Thus, according to this assumption, the unitary channel is a cluster of elementary channels.     

Effects of insulin on the lipid structure of liver plasma membrane measured with fluorescence and ESR spectroscopic methods

Insulin increased the lipid order of rat and mouse liver plasma membrane domains sampled by the hydrophobic fluorescent probe 1,6-diphenyl-1,3,5-hexatriene in a concentration-dependent saturable manner. The ordering is half maximal at $\text{5.1 · 10}{}^{\mathrm{?11}}\text{M}$ and fully saturated at $\text{1.7 · 10}{}^{\mathrm{?10}}\text{M}$ insulin. Membranes prepared from obese hyperglycemic (ob / ob) mice demonstrated a right-shift in the dose-dependent ordering induced by insulin, such that ordering was half maximal at $\text{1.2 · 10}{}^{\mathrm{?10}}\text{M}$ and fully saturated at $\text{2.0 · 10}{}^{\mathrm{?10}}\text{M}$. Insulin also increased the order of rat liver plasma membranes labeled with the cis- and trans-parinaric acid methyl esters. The ordering caused by insulin as detected with cis methyl parinarate was complete within approx. 15 min. after hormone addition at 37°C, and the ordering was approximately double that observed with the trans isomer. Additional ESR experiments demonstrated that the addition of insulin increased the outer hyperfine splittings of spectra recorded from membranes labeled with the steroid-like spin labels, nitroxide cholestane and nitroxide androstane, but not the fatty acid spin probe, 5-nitroxide stearate. Studies utilizing model membrane systems strongly suggest that the 5-nitroxide stearate samples a cholesterol-poor domain of the membrane, while the steroid-like probes preferentially sample cholesterol-rich regions of the membrane. Finally, insulin-induced membrane ordering was dose-dependently inhibited by cytochalasin B in the range 1–50 μM. From these results, we conclude that (1) the ordering effect of insulin addition to isolated liver plasma membrane fractions occurs within the physiological range of hormone concentration, and the dose-response is right-shifted in membranes from ‘insulin resistant’ animals; (2) the relative responses of the fluorescent and spin probes suggest that the effects of insulin are confined to specific domains within the membrane matrix; and (3) the direct effects of insulin on the membranes may involve protein components having cytochalasin B binding sites.     

Stimulation of respiration-linked proton efflux in Escherichia coli by carbonylcyanide-p-trifluoromethoxyphenylhydrazone (FCCP).

The proton efflux from intact, anaerobic $\text{Escherichia}\text{coli}$ cells following a small oxygen pulse is both slow ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>M</mtext><mtext>2</mtext>}}\text{～-10s}$) and inefficient ($\text{H}{}^{\mathrm{+}}\text{O}\text{～-0.5}$. Very low levels (<80 nM) of the proton ionophore carbonylcyanide-$\text{p}$-trifluoromethoxyphenylhydrazone (FCCP), which have no detectable effect upon active transport, cause a 3–5 fold stimulation in the extent of proton efflux without affecting the efflux rate. At slightly higher concentrations of FCCP (80 nM to 0.5 μM), a sharp inhibition of this increased proton efflux occurs, with the $\text{H}{}^{\mathrm{+}}\text{O}$ ratio obtained in the presence of 0.5 μM FCCP approximately equal to that obtained in the absence of FCCP. Still higher concentrations of FCCP (> 1 μM), which inhibit active transport, cause a further gradual decrease in the $\text{H}{}^{\mathrm{+}}\text{O}$ ratio. The unusual increase in the apparent efficiency of H⁺ efflux by <80 nM FCCP is not accompanied by an increase in the rate of membrane deenergization following an O₂ pulse, although such an increase is seen with the higher (uncoupling) FCCP concentrations.     

The characterization of energized and partially de-energized (respiration-independent) β-galactoside transport into escherichia coli

Unidirectional fluxes of [¹⁴C]lactose by whole cells of Escherichia coli under highly energized and partially de-energized (in the presence of CN^?) conditions are analyzed kinetically.When the cells are energized, the value for $\text{V}$ influx is $\text{0.45 ± 0.01}\text{mM}$ internal concentration increment/s and $\text{K}{}_{\mathrm{t}}$ is $\text{0.26 ± 0.03}\text{mM}$. At an external concentration of 0.61 mM the steady-state internal concentration is 0.25 M, reached after about 1h. The maximum steady-state concentration ratio is $\text{2 · 10}{}^3$.The efflux process under these conditions is non-saturable, being linearly dependent upon internal concentration over the range 25–250 mM with a first-order rate constant of $\text{8.8 ± 0.2 · 10}{}^{\mathrm{?4}}\text{s}{}^{\mathrm{?1}}$.The transport in the presence of CN^? is active, with a maximum concentration ratio (internal concentration/external concentration) of 104, and the uptake is mimicked by anoxia (< 70 ppm O₂).The effects of CN^? are to lower the $\text{V}$ for influx and to change the efflux from a non-saturable to a saturable process with a value for $\text{K}{}_{\mathrm{t}}$ (60 mM) intermediate between that for energized efflux ($\text{> 250}\text{mM}$) and influxe (0.3–0.6 mM), the latter value not changing appreciably. Partial de-energization thus affects both the influx and efflux processes.     

Characterization of calcium liberation from a human platelet membrane fraction

Calcium efflux and EGTA-induced calcium release from an internal platelet membrane fraction have been studied after the oxalate-supported calcium uptake had reached steady state. Increasing external calcium concentrations stimulate the calcium efflux velocity, with an apparent half-maximal stimulation at about 5 μM outside calcium concentration and a maximal velocity of calcium efflux of $\text{4.66 ± 2.32}\text{nmol}\text{·}\text{min}{}^{\mathrm{?1}}\text{·}\text{mg}{}^{\mathrm{?1}}$. Moreover, the ratio of the liberated calcium on the loaded calcium seems to be independent of the increasing external calcium concentration. Increasing the calculated internal calcium concentration by varying the oxalate potassium concentration from 10 mM to 1 mM results in an increase of the liberated calcium from the membrane vesicles from 7.4% to 63%, respectively, without changing the calcium efflux velocity. Similar conclusions can be drawn from the observation of results from the calcium efflux and EGTA-induced calcium release methods. Moreover, calcium pump reversal does not seem to be responsible for the calcium efflux or calcium release. All these different points added to the previously described regulation of calcium efflux by the catalytic subunit of cAMP protein kinase suggest us that the mechanism of calcium liberation by the platelet membranes is different from the calcium uptake.     

Inhibition of (Na+ + K+)-ATPase by ouabain: Involvement of calcium and membrane proteins

Treatment of plasma membrane isolated from murine plasmocytoma MOPC 173 with an EDTA-containing buffer resulted in a 300-fold increase in sensitivity of $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-stimulated}$ Mg²⁺-ATPase to ouabain. This phenomenon was associated with the solubilization by EDTA of phospholipid free proteins (approx. 30 000–34 000 daltons) from the cytoplasmic face of the plasma membrane and with removal of about 90% of the membrane bound Ca²⁺. The recovery of the original resistance to ouabain required specifically Ca²⁺ and was associated with a binding of the solubilized proteins to the membrane.     

Harmaline distribution in single muscle fibres and the inhibition of sodium efflux

Harmaline, a known inhibitor of the ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ in cell membranes, inhibited 50% of the ²²Na efflux from barnacle muscle fibres at an extracellular concentration of 2.4 mM. Injected harmaline inhibited 50% of the efflux at an estimated intracellular concentration of about $\text{8}\text{mM}\text{·}\text{kg}{}^{\mathrm{?1}}$, assuming complete equilibration with no binding. Total fibre harmaline was measured in separate fibres by ultraviolet spectrophotometry. Fibres in 3 mM harmaline saline accumulated harmaline with a half-time of 17 min and a final total fibre concentration of $\text{6–12}\text{mM}\text{·}\text{kg}{}^{\mathrm{?1}}$. In harmaline-free saline this accumulated harmaline was lost exponentially with a half-time of 35 min; injected harmaline was lost exponentially from fibres with a half-time of 50 min. It is proposed that harmaline crosses the fibre membrane as the uncharged base and that its apparent accumulation against a concentration gradient is mainly due to intracellular binding with an additional contribution from a transmembrane pH gradient. It is concluded that, in fibres exposed to harmaline saline, the intracellular concentration can reach a sufficiently high value, as judged from the results of the injection experiments, to inhibit Na⁺ efflux at an interior-facing site on the fibre membrane. In contrast, harmaline appears to inhibit the Na⁺-dependent uptake of l-glutamate at an extracellular site.     

The effects of membrane lipid order and cholesterol on the internal and external cationic sites of the Na+−K+ pump in erythrocytes

Cholesterol depletion alters the apparent affinity of the internal cationic sites and the maximal translocation rate but not the affinity of the external cationic sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump in human erythrocytes. To test whether these effects were mediated by a direct cholesterol-internal site interaction or by a change in membrane lipid order, the effects of five fluidizing amphiphiles (chlorpromazine, imipramine, benzyl alcohol, sodium oleate and sodium benzenesulphonate) on the kinetic parameters of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump were determined. The cholesterol removal and all the agents used induced dose-response decreases in membrane lipid order as measured by fluorescence polarization or ESR. Positive and neutral amphiphiles mimicked the effects of cholesterol removal on the affinity of the internal sites of the pump and to a lesser extent on the maximal translocation rate. Anionic amphiphiles had no effect on internal sites, probably because they distributed preferentially within the outer leaflet on the membrane. These results indicate that cholesterol controls the affinity of the internal sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump by altering the membrane lipid order. In contrast, neither cholesterol depletion nor the agents used altered the affinity of the external sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump. This difference in sensitivity to membrane lipid order suggests that internal and external cationic sites, although borne by the same protein, are in different lipid environments.     

Localization of lysophosphatidylcholine in bovine chromaffin granules

One of the unique features of the chromaffin granule membrane is the presence of about 17 mol% lysophosphatidylcholine. Lysophosphatidylcholine isolated from the granules could be degraded by approx. 94% by lysophospholipase. This result is consistent with chemical analyses data showing that about 9% of this lysophospholipid is 1′-alkenyl glycerophosphocholine.The localization of the acylglycerophosphocholine in the chromaffin granule membrane was studied by using pure bovine liver lysophospholipases. In intact granules only about 10% of the total lysophosphatidylcholine was directly available for enzymic hydrolysis. In contrast, when granule membranes (ghosts) were treated with lysophospholipases approx. 60% of the lysophosphatidylcholine was deacylated. These values did not increase after pre-treatment of intact granules or ghosts with trypsin. Added $\text{1-[1-}{}^{14}\text{C]palmitoyl}\text{-sn-}\text{glycero-3-phosphocholine}$ did not mix with the endogenous lysophosphatidylcholine pool(s) and remained completely accessible to added lysophospholipases.     

Properties of bilayer membranes in the presence of dipicrylamine. A comparative study by optical absorption and electrical relaxation measurements

In order to test the question if a pool of lipophilic ions may exist in black lipid membranes which cannot be detected by electrical relaxation measurements we have performed simultaneously measurements of the optical absorption of a lipophilic ion. The absorbance of membrane-bound dipicrylamine at 410 nm was measured with a sensitive spectrophotometer which can detect absorbance changes $\text{? 4 · 10}{}^{\mathrm{?5}}$. A minimal concentration of about 6 · 10¹¹ dipicrylamine ions per cm² of the membrane could be detected with this instrument. The dipicrylamine concentration in the membrane obtained with the optical method $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ is compared with the concentrations $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ obtained from simultaneous electrical relaxation measurements. $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ and $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ agreed at low dipicrylamine concentrations (10^?8–10^?7 M in the aqueous phase) and showed saturation at higher concentrations (up to 5 · 10^?6 M). In the saturation range $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ was maximally four times higher than $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$. The significance of this difference is discussed together with general aspects of the saturation phenomenon.     

Author index

The ionic influence and ouabain sensitivity of lymphocyte Mg²⁺-ATPase and $\text{Mg}{}^{\mathrm{2+}}\text{-(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-activated}$ ATPase were studied in intact cells, microsomal fraction and isolated plasma membranes. The active site of 5′-nucleotidase and Mg²⁺-ATPase seemed to be localized on the external side of the plasma membrane whereas the ATP binding site of $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ was located inside the membrane.Concanavalin A induced an early stimulation of Mg²⁺-ATPase and $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ both on intact cells and purified plasma membranes. In contrast, 5′-nucleotidase activity was not affected by the mitogen. Although the thymocyte Mg²⁺-ATPase activity was 3–5 times lower than in spleen lymphocytes, it was much more stimulated in the former cells (about 40 versus 20 %). $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ activity was undetectable in thymocytes. However, in spleen lymphocytes $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ activity can be detected and was 30 % increased by concanavalin A. Several aspects of this enzymic stimulation had also characteristic features of blast transformation induced by concanavalin A, suggesting a possible role of these enzymes, especially Mg²⁺-ATPase, in lymphocyte stimulation.     

A high-affinity (Ca2+ + Mg2+)-ATPase in plasma membranes of rat ascites hepatoma AH109A cells

The activity of calcium-stimulated and magnesium-dependent adenosinetriphosphatase which possesses a high affinity for free calcium (high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$, EC 3.6.1.3) has been detected in rat ascites hepatoma AH109A cell plasma membranes. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ had an apparent half saturation constant of $\text{77 ± 31}\text{nM}$ for free calcium, a maximum reaction velocity of $\text{9.9 ± 3.5}\text{nmol}$ ATP hydrolyzed/mg protein per min, and a Hill number of 0.8. Maximum activity was obtained at 0.2 μM free calcium. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ was absolutely dependent on 3–10 mM magnesium and the pH optimum was within physiological range (pH 7.2–7.5). Among the nucleoside trisphosphates tested, ATP was the best substrate, with an apparent $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 30 μM. The distribution pattern of this enzyme in the subcellular fractions of the ascites hepatoma cell homogenate (as shown by the linear sucrose density gradient ultracentrifugation method) was similar to that of the known plasma membrane marker enzyme alkaline phosphatase (EC 3.1.3.1), indicating that the ATPase was located in the plasma membrane. Various agents, such as K⁺, Na⁺, ouabain, KCN, dicyclohexylcarbodiimide and NaN₃, had no significant effect on the activity of high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$. Orthovanadate inhibited this enzyme activity with an apparent half-maximal inhibition constant of 40 μM. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ was neither inhibited by trifluoperazine, a calmodulin-antagonist, nor stimulated by bovine brain calmodulin, whether the plasma membranes were prepared with or without ethylene glycol $\text{bis}\text{(β-}\text{aminoethyl ether}\text{)-N,N,N′,N′-}\text{tetraacetic acid}$. Since the kinetic properties of the high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ showed a close resemblance to those of erythrocyte plasma membrane $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$, the high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ of rat ascites hepatoma cell plasma membrane is proposed to be a calcium-pumping ATPase of these cells.     

Cyclic AMP transport in human erythrocyte ghosts

10^?5 M cyclic AMP has high permeability in human erythrocyte ghosts ($\text{p = 0.061 · 10}{}^{\mathrm{?6}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$). Saturation of influx and efflux occurs. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>oi</mtext>}}\text{= 4.43}\text{mM}$. $\text{V}{}_{\mathrm{zt}}{}^{\mathrm{oi}}\text{= 259.6 μ}\text{M · min}{}^{\mathrm{?1}}$. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 0.475 μ}\text{M}$. $\text{V}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 28.3 μ}\text{M · min}{}^{\mathrm{?1}}$ at 30°C. Equilibrium exchange entry of cyclic AMP has similar kinetics to zero trans influx, though the system does show counterflow. Cythochalasin B is an apparent competitive inhibitor of cyclic AMP exit. ($\text{K}{}_{\mathrm{<mtext>i</mtext>}}\text{= 3.9 · 10}{}^{\mathrm{?7}}\text{M}$).Control experiments indicated that cyclic AMP remains intact during incubation with red blood cell ghosts and is contained within the intravesicular space during the transport experiments.     

The permeability of the lysosomal membrane to small ions

The permeability of the lysosomal membrane to small anions and cations was studied at 37°C and pH 7.0 in a lysosomal-mitochondrial fraction isolated from the liver of untreated rats. The extent of osmotic lysis following ion influx was used as a measure of ion permeancy. In order to preserve electroneutrality, anion influx was coupled to an influx of K⁺ in the presence of valinomycin, and cation influx was coupled to an efflux of H⁺ using the protonophore $\text{3-tert-}\text{butyl-5,2′-dichloro-4′-nitrosalicilylanilide}$. Lysosomal lysis was monitored by observing the loss of latency of two lysosomal hydrolases.The order of permeability of the lysosomal membrane to anions was found to be $\text{SCN}{}^{\mathrm{?}}\text{> I}{}^{\mathrm{?}}\text{> CH}{}_3\text{COO}{}^{\mathrm{?}}\text{> Cl}{}^{\mathrm{?}}\text{≈ HCO}{}^{\mathrm{?}}{}_3\text{≈ P}{}_{\mathrm{i}}\text{> SO}{}_4{}^{\mathrm{2?}}$ and that to cations $\text{Cs}{}^{\mathrm{+}}\text{> K}{}^{\mathrm{+}}\text{> Na}{}^{\mathrm{+}}\text{> H}{}^{\mathrm{+}}$. These orders are largely in agreement with the lyotropic series of anions and cations.The implications of these findings for the mechanism by means of which a low intralysosomal pH is produced and maintained are discussed.     

Characterization of the (Na+ + K+)-ATPase in a membranous preparation from the optic ganglion of the squid (Loligo pealei)

(1) A membrane fraction enriched in $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ (EC 3.6.1.3) was obtained from optic ganglia of the squid (Loligo pealei) by density gradient fractionation of membranes followed by treatment with either SDS or Brij-58. The resulting membrane had an $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ specific activity of approx. 2 units/mg and was $\text{>95\%}$ ouabain-sensitive. (2) The $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ had a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for ATP of $\text{0.42 ± 0.04}\text{mM}$ and a pH optimum of 7.0. It was inhibited by ouabain with a $\text{K}{}_{\mathrm{<mtext>i</mtext>}}$ of $\text{0.32 ± 0.04 μ}\text{M}$. (3) Optimum monovalent cation concentrations were: 240 mM NaCl, 60 mM KCl, tested with $\text{NaCl + KCl}\text{= 300}\text{mM}$. (4) The Mg²⁺ dependence of hydrolysis varied with the absolute ATP concentration. At 3 mM ATP, the$\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for Mg²⁺ was $\text{0.86 ± 0.10}\text{mM}$, and at 6 mM ATP, the $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ was $\text{1.86 ± 0.44}\text{mM}$. High levels of Mg²⁺ caused inhibition of hydrolysis. (5) The interactions of Na⁺ and K⁺ were examined over a range of conditions. K⁺ levels caused modulations in the Na⁺ dependence in the range of 1–150 mM. (6) The $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ prepared from squid optic ganglion displays properties similar to those of the sodium pump in injected nerves.