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Journal of Bacteriology, May 2003, p. 2952-2960, Vol. 185, No. 9
0021-9193/03/$08.00+0 DOI: 10.1128/JB.185.9.2952-2960.2003
Copyright © 2003, American Society for Microbiology. All Rights Reserved.
Lehrstuhl für Biotechnologie, Biozentrum der Universität Würzburg, Am Hubland, D-97074 Würzburg, Germany,1 University of Sunderland, Institute of Pharmacy, Fleming Building, Sunderland SR2 3SD, England2
Received 2 December 2002/ Accepted 12 February 2003
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In both foals and humans, R. equi disease is typically characterized by bronchopneumonia, although extrapulmonary manifestations are also found (13, 33, 52). R. equi is an intracellular pathogen of alveolar macrophages, and the bacterium is known to enter macrophages via complement receptors following deposition of complement component C3 (25). Once within the macrophage, the bacteria resist the host's killing mechanisms and multiply. However, there is currently little information concerning the specific bacterial factors which facilitate entry into or subsequent survival within macrophages. Persistence within macrophages most likely contributes to the in vivo resistance of R. equi to many classes of antibiotics (13). A combination of rifampin and erythromycin remains the treatment of choice for foals, but no optimal drug regimen has been established for human infections and relapse is a significant problem (52). Moreover, rifampin-resistant phenotypes of R. equi have been identified (1, 12, 49), and the use of erythromycin in foals may have side effects (13, 46). There thus remains a need to identify physiological features of R. equi that contribute to the ability of this organism to thrive within macrophages and which might provide targets for the implementation of novel therapeutic strategies.
R. equi is a member of a unique bacterial taxon, the mycolata, within the gram-positive actinomycetes (9). Members of this taxon are distinguished by the presence within their cell envelopes of large 3-hydroxy 2-alkyl branched fatty acids, the mycolic acids (MAs). A large proportion of the MAs are covalently linked to the arabinogalactan cell wall polysaccharide, and in contrast to the typical gram-positive cell envelope, an outer lipid permeability barrier is predicted to be formed by the association of these bound MAs with other cell envelope lipids, such as trehalose mycolates (8, 10, 15, 24, 32, 35, 47, 48). The presence of this asymmetric outer lipid permeability barrier predicates that the cell envelopes of the mycolata must contain permeability pathways accessible to hydrophilic solutes. Consistent with this, cation-selective channel-forming proteins have been identified in the cell walls of C. diphtheriae (35), C. glutamicum (20, 23, 29), Mycobacterium bovis (21), M. chelonae (50), M. phlei (38), M. smegmatis (26, 30, 51), M. tuberculosis (16, 45), Nocardia asteroides (39), N. (Rhodococcus) corynebacteroides (37), N. farcinica (40), and R. erythropolis (22). The selectivity of these channels for cations suggests that the cell walls of these MA-containing actinomycetes also contain complementary channels of distinct specificities. Consistent with this, an anion-selective channel has also been identified in M. bovis (21).
To extend these studies on the channel-forming proteins of the mycolata and to further strengthen our understanding of cell envelope permeability in an important pathogen, we have investigated the presence of channel-forming activities in the cell wall of R. equi. The results suggest that the cell wall of this pathogen contains at least two types of channels: a high-conductance cation-selective channel and a low-conductance anion-selective channel.
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SDS-PAGE. Analytical and preparative sodium dodecyl sulfate-polyacrylamide gel electrophoresis (SDS-PAGE) on Tricine-containing gels was performed according to a method previously described (42). The gels were stained with Coomassie brilliant blue or colloidal Coomassie blue (11).
Isolation and purification of the channel-forming proteins from the cell wall. The lyophilized cells were inspected for channel-forming activity by treatment with organic solvents, as this method has successfully been used previously for the identification and purification of the cell wall porins of C. glutamicum (20) and R. erythropolis (22). Lyophilized cells (0.2 g) were extracted with 8 ml of a 1:2 mixture of CHCl3:CH3OH for 24 h at 50°C by stirring in a closed container to avoid the loss of CHCl3. The cell-CHCl3:CH3OH mixture was centrifuged at 10,000 rpm at 4°C for 20 min in a Beckmann J2-21 M/E centrifuge (rotor JA20). The pellet was discarded, and the supernatant extract was mixed with ice-cold diethylether in a ratio of 1 part supernatant to 9 parts diethylether and kept overnight at -20°C. The precipitated protein was dissolved in a solution containing 1% Genapol and 10 mM Tris-HCl (pH 8.0) followed by a second precipitation step with ice-cold diethylether. This second precipitation step reduced the lipid content of the samples. The final pellet contained the channel-forming protein PorBReq (R. equi pore B), as determined by black-lipid bilayer experiments (see below). Treatment of the dissolved protein fraction with 2.5 volumes of ice-cold ethanol for 24 h at -20°C followed by centrifugation yielded a pellet that was dissolved in a solution containing 1% Genapol and 10 mM Tris-HCl (pH 8.0) and was incubated for 2 days at room temperature. Inspection of this preparation for channel-forming activity led to the discovery of the channel-forming protein PorAReq (R. equi pore A).
Lipid bilayer experiments. The method used for the experiments investigating reconstitution by the black lipid bilayer membranes has been described previously (5). The membranes were formed from a 1% (wt/vol) solution of a mixture of diphytanoyl phosphatidylcholine (PC) and phosphatidylserine (PS) (both lipids were obtained from Avanti Polar Lipids, Alabaster, Ala.) in a molar ratio of 4:1 in n-decane. Membranes were also formed from PC-MA (Sigma) or PC-PS-MA mixtures to study the effect of MAs on channel formation. The membrane current was measured with a pair of calomel electrodes switched in series with a voltage source and an electrometer (Keithley 617). For single-channel recordings, the electrometer was replaced by a highly sensitive current amplifier (Keithley 427). Using a high-impedance electrometer (Keithley 617) as described earlier (6), zero-current membrane potentials were measured by establishing a salt gradient across membranes containing 100 to 1,000 channels.
Estimation of the channel diameter using the Renkin correction factor. The calculation of the channel size is possible from single-channel conductance data when the channel is wide and water filled and when only cations or anions can permeate through the channel. Under these conditions, the entry of the ions in the channel and not the diffusion through the channel is the rate-limiting step and the Renkin correction factor (36) times the aqueous diffusion coefficient of the hydrated ions can be used to estimate the channel radius a from the relative permeativities of the different ions through the channel. The relative permeativities of the ions were calculated from their single-channel conductance relative to that of Rb+ and plotted as a function of the hydrated ion radius r (51). It is noteworthy that a similar approach has been used previously to calculate the radii of porin channels from the relative rates of permeation of different solutes in the liposome swelling assay (31).
Channel size estimations from the effect of negatively charged groups at the channel. Negative charges at the opening of an ion channel result in substantial ionic strength-dependent surface potentials at the pore mouth that attract cations and repel anions. Accordingly, they influence both single-channel conductance and zero-current membrane potential. A quantitative description of the effect of the point charges on the single-channel conductance was determined using the treatment proposed previously (28, 50). These reports described the effect of point charges on the conductance of a channel, which is dependent on ion concentration, on the channel diameter, and on the number of negative charges (3). Comparison of the crystal structure of Rhodobacter capsulatus porin with the diameter derived from this theoretical treatment yielded good agreement (34).
Western blot analysis. In Western blot (immunoblot) experiments, the proteins separated by 10% Tricine-containing SDS-PAGE were transferred onto 0.2-µm-thick nitrocellulose sheets (Protran BA83; Schleicher & Schuell) in a semidry blotting apparatus according to a previously described method (43). This method is a modification of a previously described procedure (17) and takes into account the higher ionic strength of Tricine-containing gels. The reactive sites were blocked with 5% skim milk in Tris-buffered saline (TBS) (1 M Tris-HCl [pH 7.5], 0.01 M NaCl) for 30 min and shortly washed with three different solutions (solution 1, 1% skim milk in TBS [pH 7.5]; solution 2, 1% skim milk, 0.1% Tween in TBS [pH 7.5]; solution 3, TBS [pH 7.5]). The blots were probed for 1 h (or overnight) at room temperature with rabbit polyclonal antibodies (Charles River Wiga GmbH, Sulzfeld, Germany) raised against synthetic peptides corresponding to the N terminus of the R. erythropolis porin (22) in a 1:100 dilution. After the incubation, the membrane was washed with solution at a 1-to-3 ratio. Bound antibodies were detected by using horseradish-peroxidase-coupled rabbit immunoglobulins (DAKO, Glostrup, Denmark) at a 1:1,000 dilution. Color reaction was obtained after 10 min of incubation in 94% TBS-6% chloronaphthol (0.3%)-0.075% hydrogen peroxide.
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FIG. 1. SDS-PAGE of the purified cell wall channel proteins of R. equi. (A) PorAReq (R. equi pore A). Lane 1, molecular mass markers (26.6, 17.0, 14.2, and 6.5 kDa); lane 2, 5 µg of purified PorAReq solubilized at 40°C for 30 min in 20 µl of sample buffer; lane 3, molecular mass markers (94, 67, 43, 30, 20.1, and 14.4 kDa) (Coomassie blue staining). (B) PorBReq (R. equi pore B). Lane 1, molecular mass markers (94, 67, 43, 30, 20.1, and 14.4 kDa); lane 2, molecular mass markers (16.9, 14.4, 10.7, and 8.2 kDa [6.2- and 2.5-kDa molecular mass markers are not visible on the gel]); lane 3, 3 µg of purified PorBReq was solubilized at 40°C for 30 min in 20 µl of sample buffer (Coomassie blue staining).
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Single-channel analyses. The addition of lower concentrations of the cell wall proteins (10 ng/ml) to lipid bilayers made of PC-PS allowed the resolution of stepwise conductance increases. Figure 2 shows the results of single-channel recording in the presence of the cell wall porins PorAReq (panel A) and PorBReq (panel B), which were added 5 min after the membrane had turned black. Shortly after the addition of the protein, the current started to increase in a step-wise fashion. Each step corresponded to the incorporation of one channel-forming unit into the membrane. Under the low-voltage conditions for the experiment whose results are depicted in Fig. 2, all the steps were directed upwards, which indicated that the channels were always in the open state and had a long lifetime (mean lifetime, more than 5 min). Figure 3 represents the histograms of the conductance fluctuations observed under the conditions described for Fig. 2. PorAReq had (on average) a single-channel conductance in 1 M KCl of about 4 nS (more than 45% of all conductance fluctuations) (Fig. 3A). Besides the 4-nS channel, we observed also channels with about 8 nS, as shown in Fig. 3A, which presumably represent dimers of the 4-nS channel which incorporate at the same time into the membrane. At 300 pS in 1 M KCl, the single-channel conductance of PorBReq was substantially smaller (more than 80% of all conductance fluctuations) (Fig. 3B). It is noteworthy that the exchange of PC-PS membranes with membranes made of other lipid mixtures such as PC alone, PC-MA (molar ratio, 4:1), or PC-MA-PS (molar ratio, 4:4:1) did not influence the single-channel conductance of either channel-forming protein.
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FIG. 2. Single-channel recordings of a PC-PS (molar ratio 4:1)-n-decane membrane in the presence of the purified cell wall channels of R. equi. In both cases, the aqueous phase contained 1 M KCl, 10 mM Tris-HCl (pH 8.0), and 10 ng of cell wall protein/ml. The applied membrane potential was 10 mV, and the temperature was 20°C. (A) Recording of PorAReq, the 67-kDa protein from the cell wall of R. equi. (B) Recording of PorBReq, the 11-kDa protein from the cell wall of R. equi.
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FIG. 3. Histograms of the probability P(G) for the occurrence of a given conductivity unit observed with membranes formed of PC-PS (molar ratio 4:1)-n-decane in the presence of the cell wall channels of R. equi. P(G) is the probability that a given conductance increment G is observed in the single-channel experiments. It was calculated by dividing the number of fluctuations with a given conductance increment by the total number of conductance fluctuations. The aqueous phase contained 1 M KCl and 10 mM Tris-HCl (pH 8.0). The applied membrane potential was 10 mV, and the temperature was 20°C. (A) Histogram after addition of PorAReq. The average single-channel conductance for 109 single-channel events was 4 nS. (B) Histogram after addition of PorBReq. The average single-channel conductance for 121 single-channel events was 300 pS.
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Rb+
Cs+ > Na+ > Li+ > Tris+, which means that the permeability of the cations through the channels approximately followed their mobility sequence in the aqueous phase. This result suggests that PorAReq forms a wide and water-filled channel. In contrast, the single-channel conductance of PorBReq was much less dependent on the type of cation present in the aqueous solution than that of PorAReq. This result indicated that PorBReq is anion selective, a reasonable assumption in that a second cation-selective channel of small permeability would be unnecessary given the presence of the highly conductive PorAReq. |
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TABLE 1. Average single-channel conductance G of the cell wall channels PorAReq and PorBReq of R. equi in different salt solutionsa
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Selectivity of the cell wall channels of R. equi. We performed zero-current membrane potential measurements to obtain further information on the molecular structure of the cell wall channels of R. equi. After incorporation of 100 to 1,000 channels into the PC-PS membranes, the salt concentration on one side of the membranes was raised fivefold (beginning at 100 mM), and the zero-current potential was measured 5 min after every increase of the salt gradient across the membrane. For PorAReq, with all three salts employed in these experiments (KCl, LiCl, and KCH3COO), the more dilute side of the membrane (100 mM) always became positive (Table 2), which indicated preferential movement of the cations through the channel; i.e., this cell wall channel is cation selective, as was already suggested from the single-channel recordings (Table 1). Using the Goldman-Hodgkin-Katz equation (6), analysis of the zero-current potentials suggested that anions also might have limited permeability through the channel, because the ratios of permeability of Pcation and Panion were 8.2 (LiCl), 9.00 (KCl), and 8.5 (potassium acetate). On the other hand, the permeability ratios are close to one another, which is unexpected for moderately selective channels such as the general diffusion pores of gram-negative bacteria because of the different mobilities of anions and cations in a wide water-filled channel (4).
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TABLE 2. Zero-current membrane potentials Vm of PC-PS (molar ratio, 4:1)-n-decane membranes in the presence of the cell wall channels PorAReq and PorBReq of R. equi measured for a fivefold gradient of different saltsa
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The two cell wall channels have different voltage dependences. In single-channel recordings, the cell wall porin PorAReq exhibited some flickering at higher voltages; i.e., it showed rapid transitions between open and closed configurations. This might have been caused by voltage-dependent closing of PorAReq; therefore, we measured the voltage dependence of the channel in multichannel experiments. Figure 4 shows an example of these measurement for voltages between ±10 and ±30 mV. For positive and negative applied voltages, the potential decreased in an exponential fashion (Fig. 4), similar to previous observations for the cell wall channels of N. corynebacteroides, R. erythropolis, and C. glutamicum (20, 22, 37). Interestingly, we observed a symmetric response for voltages between ±10 mV and ±120 mV independently of whether we added the porin at the cis side, at the trans side, or at both sides of the membrane (Fig. 5). These results indicated either a random orientation of the porin PorAReq or a symmetric response to the applied voltage. In contrast, PorBReq was found not to be voltage gated (at least up to about ±100 mV) when the channel-forming protein was added to one or both sides of black PC-PS-n-decane membranes (Fig. 5). This means that the two cell wall channels responded differently to applied voltage.
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FIG. 4. Study of the voltage gating of the cation-selective cell wall channel PorAReq. Cell wall channel protein (500 ng/ml) was added to the cis side of a black PC-PS (molar ratio, 4:1)-n-decane membrane, and the reconstitution of the channels was monitored for about 30 min. When about 100 channels were reconstituted into the membrane, increasing positive (upper traces) and negative voltages (lower traces) were applied to the cis side of the membrane and the membrane current was measured as a function of time. The aqueous phase contained 1 M KCl and 10 mM Tris-HCl (pH 8.0), and the temperature was 20°C.
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FIG. 5. Ratio of the conductance G at a given membrane potential (Vm) divided by the conductance Go at 10-mV membrane potential as a function of membrane potential Vm measured for PorAReq and PorBReq. The circles indicate measurements determined when PorAReq was added to the cis side of the membranes, and the squares indicate measurements determined when PorBReq was added to the same side of the membranes. The aqueous phase contained 1 M KCl, 10 mM Tris-HCl (pH 8.0), and 100 ng of protein/ml. The membranes were formed from PC-PS (molar ratio, 4:1) dissolved in n-decane. The temperature was 20°C. Mean values for at least four experiments are shown.
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FIG. 6. Western blot analysis (using polyclonal antibody to the R. erythropolis porin) of the cell wall porins of R. erythropolis and R. equi. Positions of size markers are shown on the right. The channel-forming protein PorAReq was extracted as described in Materials and Methods, and the cell wall channel of R. erythropolis was determined as described previously (22). Lane 1, cation-selective channel-forming protein of R. equi (PorAReq); lane 2, channel-forming protein of R. erythropolis.
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The cation-selective channel PorAReq had a single-channel conductance of 4 nS in 1 M KCl and was voltage gated. Experiments with higher membrane potentials suggested that its voltage gating is symmetric and that the symmetry is independent of whether we added the channel-forming protein to one side of the membrane or to both sides. Starting at about ±20 mV, the channels closed, and the application of ±40 mV led to a closure of 50% of all channels in the membrane. These results indicated either that the protein was reconstituted in a random conformation in the membrane or that the channels reacted symmetrically to the applied membrane voltage. It is noteworthy that voltage dependence has been found for many cell wall channels. Some of them showed asymmetric voltage-dependent gating; the channels closed only when the cis side (the side with the addition of the protein) had negative voltage, as observed for channels from C. glutamicum (20), N. corynebacteroides (37), and R. erythropolis (22). Moreover, a proportion of these channels seemed to close irreversibly after the application of ±50 mV and higher voltages, which means that the potential at the inner side of the cell wall might influence their permeability properties. The potential might come from a Donnan potential across the cell wall, as has been observed in Escherichia coli cells (44). However, it is also possible that the function of PorAReq in vivo is unaffected by the potential difference across the MA permeability barrier. It is noteworthy that PorBReq was not voltage gated. PorAReq has an apparent molecular mass of 67 kDa by SDS-PAGE and we did not observe dissociation of the 67-kDa protein after boiling. The calculated pore diameter (1.8 to 2.0 nm) of PorAReq is somewhat smaller than those calculated for the porins of R. erythropolis (22), N. corynebacteroides (37), and C. glutamicum (20), consistent with the observation that the conductance of the R. equi channel is lower than those of the other cell wall porins in the same salt solutions (Table 3).
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TABLE 3. Comparison of the cell wall channel properties of R. equi, R. erythropolis, C. glutamicum, N. farcinica, N. corynebacteroides (R. corynebacteroides) and M. bovis BCG
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Gram-negative bacteria contain four classes of outer membrane channels reflecting different strategies for the passage of hydrophilic compounds through their outer membranes. General diffusion porins form water-filled channels for the nonspecific diffusion of hydrophilic compounds, whereas specific porins contain binding sites for classes of particular solutes. In addition, receptors and efflux channels may also be present (4). The properties of the cell wall channels PorAReq and PorBReq are similar to those found in the cell walls of closely related MA-containing actinomycetes (Table 3). Thus, in species representing four major genera of the mycolata, we have identified so far only specialized (i.e., channels containing point-negative net charges) but nonspecific pore-forming proteins. Common to this class of porins is that they are wide and water filled and that they contain charges at the channel mouth. Most cell wall channels contain negative point charges. However, it is noteworthy that one other anion-selective channel has been found previously in M. bovis besides a high-conductance cation-selective pore (21), similar to the situation described here for R. equi. The evolution of two protein channels with distinctive features may be a conserved and general principle in the cell wall channels of MA-containing actinomycetes. We presume that the distribution of anion-selective channels in the mycolata will match that of the cation-selective channels to facilitate the uptake of both kinds of solutes. Cation-selective channels may be more abundant in the cell envelope, making them easier to detect and isolate. However, it is noted that anion-selective pore-forming proteins appear to be less frequent than cation-selective pore-forming proteins in gram-negative bacteria (7). In addition to those described above, channel-forming proteins have recently been identified in the more distantly related actinomycetes that lack MAs but presumably present some kind of as-yet-undescribed cell wall permeability barrier (18, 19). However, the wall channel of Streptomyces griseus is distinctive in that it contains a binding site for the antibiotic streptomycin, which is produced by that organism (18), while that of Micromonospora purpurea is apparently a substantially larger, 200-kDa protein with unusually high (14 nS) single-channel conductance (19).
The diameter of the PorAReq channel of R. equi was estimated on the basis of its single-channel conductance (51). The estimation used the relative permeability of the different cations through the channel, as calculated from the single-channel conductance. This means that it was based on the same assumptions which have been used previously for the derivation of the Renkin equation (36) for the diffusion of neutral molecules through porous membranes (see Experimental Procedures in that report). Figure 7 shows the fit of the relative permeability of the PorAReq channel for cations with the Renkin equation (equation 6 of reference 51) times the aqueous diffusion coefficient of the ions as a function of the hydrated radii calculated from the limiting molar conductivity of the cations by using Stoke's equation (taken from reference 51). The data points are given relative to the data for Rb+, the cation with the smallest hydrated ion radius, whose value was set to unity, and the best fit of the relative permeability was obtained with r = 0.9 nm (Fig. 7; diameter, 1.8 nm). A diameter of 1.8 nm is very similar to those of cell wall channels from other mycolata despite a different molecular mass of the channel-forming proteins (Table 3). The data of PorBReq could not be analyzed using the Renkin formula, because the anions seem to interact with the channel and because the relative permeability of the channel differed only little for the different anions.
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FIG. 7. Fit of the single-channel conductance data of the cell wall channel PorAReq as determined by multiplying the Renkin correction factor by the aqueous diffusion coefficients of the different cations. The product of the two numbers was normalized to 1 for a = 0.105 nm (Rb+). Single-channel conductances were normalized to the ones of Rb+ and plotted versus the hydrated ion radii taken from reference 50. The closed points correspond to Li+, Na+, K+, NH4+, Cs+, N(CH3)4+, N(C2H5)4+ and Tris+, which were all used for the pore-diameter estimation (see Discussion). The fit (solid lines) is shown for r = 1.4 nm (upper line) and r = 0.6 nm (lower line). The best fit was achieved with r = 0.9 nm (diameter = 1.8 nm), which corresponds to the broken line.
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FIG. 8. Single-channel conductance of the cell wall channels of R. equi as a function of the KCl concentration in the aqueous phase. Conductances are shown as circles (PorAReq) and squares (PorBReq). The solid lines represent the fit of the single-channel conductance data with the Nelson and McQuarrie formula (equations 1 to 6 of reference 49), assuming the presence of negative and positive point charges (1.5 positive charges) at the channel mouth and assuming channel diameters of 2 nm (PorAReq) and 1.4 nm (PorBReq). c, molar concentration of the KCl solution; G, average single-channel conductance in pS (10-12 S). The broken (straight) lines show the single-channel conductances of the two cell wall channels when no point charges are present and correspond to linear functions between channel conductance and bulk aqueous salt concentration.
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This investigation was supported by grants from the Deutsche Forschungsgemeinschaft (Be 865/9) and the Fonds der Chemischen Industrie.
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