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J. Biol. Chem., Vol. 283, Issue 7, 4219-4227, February 15, 2008
Determinants of Anion-Proton Coupling in Mammalian Endosomal CLC Proteins*
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| ABSTRACT |
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or SCN- transport was partially uncoupled from H+ countertransport but still depended on the proton glutamate. Inserting proton glutamates into CLC channels altered their gating but failed to convert them into Cl-/H+ exchangers. Noise analysis indicated that ClC-5 switches between silent and transporting states with an apparent unitary conductance of 0.5 picosiemens. Our results are consistent with the idea that Cl-/H+ exchange of the endosomal ClC-4 and -5 proteins relies on proton delivery from an intracellular titratable residue at position 268 (numbering of ClC-5) and that the strong rectification of currents arises from the voltage-dependent proton transfer from Glu-268 to Glu-211. | INTRODUCTION |
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The linear I/V relationship of ecClC-1 allowed the estimation of a 2:1 stoichiometry of transport from reversal potentials (4). Unlike ecClC-1, ClC-4 and -5 mediate strongly outwardly rectifying currents (7), precluding a precise determination of their coupling ratio from reversal potentials. Comparing Cl- and H+ transport rates yielded estimates for the Cl-/H+ stoichiometry between 1 and 5 (5, 6). The biological consequences of endosomal CLCs being Cl-/H+ antiporters rather than Cl- channels are intriguing (8). These proteins are thought to facilitate endosomal/lysosomal acidification by neutralizing proton pump currents, a process important for endocytotic trafficking and lysosomal function. Indeed, ClC-5 is crucial for renal endocytosis and is mutated in a human disorder associated with proteinuria and kidney stones (9).
It remains unclear whether Cl-/H+ exchange depends on the dimeric structure of CLC proteins. It is known that both pores of the double-barreled ClC-0 Cl- channel can be shut closed simultaneously by a "common gate" that depends on both subunits (10-13). Similarly, it may be that Cl-/H+ flux coupling in CLC transporters is based on a conformational change that involves both subunits.
Although the flux coupling is poorly understood, some amino acids involved in this process have been identified. The crystal structure of ecClC-1 revealed a glutamate that blocks the access of external anions to a central Cl- binding site (14). Neutralizing this glutamate created a new, more external Cl- binding site (15). Equivalent mutations in vertebrate CLC Cl- channels drastically changed their gating (15-17). A loss of rectification was observed with similar mutations in ClC-4 and -5 (7), which are now known to be exchangers. It was suggested (15) that this glutamate is involved in the gating by the permeant anion, a simple model explaining the voltage- and anion-dependent gating of ClC-0 (18). When this "gating glutamate" was neutralized in ecClC-1 (4) or in ClC-4 and -5 (5, 6), proton coupling was lost, and pure anion conductances were observed. Thus, this gating glutamate has a dual role in gating CLC Cl- channels and in coupling Cl- to H+ countertransport in CLC exchangers. Both roles may involve protonation and deprotonation of its side chain.
Mutations in a glutamate ("proton glutamate," Glu-203) close to the cytoplasmic face of ecClC-1 also uncoupled Cl- from H+ fluxes (19), suggesting that H+ and Cl- take different routes to the gating glutamate where both pathways converge. The present work on ClC-4 and -5, although showing a role of the proton glutamate in H+ coupling, reveals important differences from ecClC-1. Whereas neutralizing the proton glutamate converted ecClC-1 into a Cl-conductance, it abolished both Cl- and H+ transport in ClC-4 and -5. Transport of Cl-, but not of H+, was restored by additionally neutralizing the gating glutamate, suggesting a strict coupling of Cl- to H+ transport at the central translocation site. Moreover, Cl-/H+ exchange is carried out independently by each subunit, and noise analysis, usually used to characterize gating events in ensembles of channels, suggests that Cl-/H+ exchange occurs in bursts with an apparent unitary conductance of
0.5 picosiemens.
| EXPERIMENTAL PROCEDURES |
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Two-electrode Voltage Clamp of Injected Xenopus Oocytes—Oocytes were obtained by dissection and collagenase treatment of ovaries from pigmented and albino Xenopus laevis frogs and injected with 10-50 ng of cRNA transcribed from linearized cDNA with the Ambion mMessage mMachine kit according to the manufacturer's instructions. Currents were measured using a standard two-electrode voltage clamp at room temperature (20-24 °C) employing a Turbo Tec amplifier (npi, Tamm, Germany) and a custom acquisition program (GePulse) or pClamp9 (Molecular Devices). The standard bath solution contained (in mM): 100 NaCl, 4 MgCl2, 10 HEPES, pH 7.3. Alternatively, a solution similar to frog Ringer's was used (ND96, pH 7.5, or buffered with MES to pH 5.5 or 6.5 or with Tris to pH 8.5 as indicated), in which divalent cation and potassium salts were substituted with the corresponding gluconate salts and NaCl with NaSCN, NaNO3, NaBr, NaI, or NaClO4 as indicated. Ag/AgCl electrodes and 3 M KCl agar bridges were used as reference and bath electrodes. For ion substitution experiments we substituted 100 mM NaCl with 100 mM NaSCN or 100 mM NaNO3 and MgCl2 with MgSO4.
Extracellular pH Measurements—H+ transport activity was assessed by monitoring the acidification of the extracellular solution close to the oocyte using a pH-sensitive microelectrode as described previously (5). Briefly, a silanized microelectrode was tip-filled with a proton ionophore (Cocktail B, Fluka), backfilled with a solution containing phosphate-buffered saline, and connected to a custom high-impedance amplifier. The electrodes were routinely checked and responded consistently with a slope of 57-61 mV/pH unit. A pH-sensitive microelectrode was gently pushed onto the vitelline membrane without rupturing the plasma membrane. A microelectrode filled with 3 M KCl was placed close to the oocyte as a reference, and the difference signal was low pass-filtered at 50 Hz before digitization. The oocyte was simultaneously voltage-clamped with two microelectrodes, and acidification was induced by applying a train of voltage clamp pulses to +80 mV, as described previously (5). A pulse protocol rather than continuous depolarization was chosen to avoid the activation of endogenous conductances. ClC-4 and -5 only transport ions during the positive pulse, as they are strongly outwardly rectifying. The pH signal was averaged for the duration of one pulse of the train and plotted versus the time of the application of the pulse (see Fig. 1). For measurements of the extracellular acidification, solutions contained 0.5 mM buffer (HEPES for pH > 6.5, otherwise MES).
Intracellular pH Measurements—We developed a fluorescence-based device, called Fluorocyte, to measure intracellular pH changes based on the pH-sensitive excitation of BCECF (free acid, 23 nl of saturated aqueous solution injected 10-30 min prior to the experiment) at 488 nm, where fluorescence is pH-dependent. Emission was band pass-filtered at 512-565 nm, converted to current by a photodiode, and digitized by a Digidata 1320 interface (Molecular Devices) following I/V conversion at 0.5 V/nA. Fluorocyte allowed simultaneous two-electrode voltage clamp measurements (using an npi TEC10) and fluorescence while perfusing the bath continuously. The oocyte was placed over a hole of 0.8 mm in diameter, through which BCECF fluorescence was measured and which was in contact with a perfusion channel. Thus, solution could be quickly exchanged both at the small membrane portion facing the hole and on the much larger rest of the oocyte. This is important for comparing currents (which reflect the conductance of the entire membrane) with changes in pHi, which was only measured close to the plasma membrane area that faced the hole. The fluorescence response to an ensemble of depolarizing pulses to +90 mV for 400 ms interrupted by 100 ms pulses to -60 mV (to avoid the activation of endogenous currents by prolonged depolarization) was measured and digitally Bessel-filtered at 1 Hz, as in Fig. 5. The method allows a sensitive qualitative measurement of pH changes brought about by voltage clamping or solution exchange, but is not quantitative, as no ratiometric measurements and calibrations are used. We frequently observed a drift in base-line fluorescence, which became more apparent in the higher resolution scaling necessary to resolve the smaller fluorescence changes observed with weakly transporting mutants. This drift could be due to redistribution of the dye within the oocyte or bleaching, or a combination of both. However, as we observed the difference between the rate of the fluorescence change during the pulse protocol and with the oocytes held at their resting membrane potential, Fluorocyte gave a robust semiquantitative measure for H+ transport activity.
For the anion exchange experiments aimed at a more quantitative comparison of coupling stoichiometry, we performed ratiometric BCECF imaging (excitation at 440 and 480 nm and emission between 515 and 560 nm) using a Zeiss microscope 10-30 min after injection of BCECF into the oocyte. We divided the change in ratio in response to a set of depolarizing pulses through the measured current integrated over time and normalized the data to chloride.
Inside-out Patch Clamp Measurements for Noise Analysis—The extracellular (pipette) solution contained (in mM): 100 N-methyl-D-glucamine Cl, 5 MgCl2, 10 HEPES, pH 7.3. The internal solution contained (in mM): 100 N-methyl-D-glucamine Cl, 2 MgCl2, 10 HEPES, 2 EGTA, pH 7.3. To detect macroscopic currents in excised patches, pipettes were made from aluminum silicate glass capillaries (Hilgenberg, Malsfeld, Germany) to a diameter of about 15-20 µm with a resistance of 300-800 kilohms under our recording conditions. Recordings were performed using an EPC-7 amplifier (HEKA Electronics, Lambrecht, Germany). The voltage protocol consisted of a voltage step to 140 mV for 50 ms, followed by a step to -50 mV. Currents were filtered at 20 kHz and digitized with a sampling rate of 50 kHz. Noise analysis was performed on an ensemble of 70-120 recordings. To estimate apparent "single channel" (unitary) conductances, the variance was plotted versus the mean current, and the points were fitted with the function (Equation 1),
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Data Analysis—Data were analyzed using custom software (Ana), SigmaPlot (SPSS Inc.), Origin (OriginLab Corporation), and pClamp9.
| RESULTS |
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/H+ antiporter that accumulates nitrate in plant vacuoles (24) also displays a proton glutamate. We therefore used ClC-4 and -5 to explore the role of putative proton glutamates in mammalian Cl-/H+ exchangers. As described previously (5, 6, 20), ClC-5 mediates strongly outwardly rectifying currents (Fig. 1B) and extrudes protons upon depolarization, as detected by intracellular alkalinization in Fig. 1C. Replacing the proton glutamate with the similarly acidic aspartate reduced transport activity without abolishing it (Fig. 1, D-F). The voltage dependence and kinetics of currents from the E268D mutant (Fig. 1D) resembled those of WT ClC-5 (Fig. 1B). Likewise, the mutant extruded acid equivalents when activated by trains of depolarizing pulses, as detected by intracellular alkalinization (Fig. 1E) or extracellular acidification (Fig. 1F). Importantly, and again like WT ClC-5, it could extrude protons against an electrochemical gradient (pHo 5) (Fig. 1E), strongly suggesting a directly coupled Cl-/H+ exchange. The weakly basic histidine (Fig. 2A), but not the strongly basic arginine (Fig. 2B), could also functionally substitute for the proton glutamate. Tyrosine also supported Cl-/H+ exchange, albeit with generally lower transport rates (Fig. 2C). By contrast, when the proton glutamate was replaced with alanine, the mutants produced neither measurable currents nor H+ transport in Xenopus oocytes (Fig. 1, G and H, for ClC-5E268A; supplemental Fig. S1 for ClC-4E281A). Likewise, no transport was observed when the proton glutamate was replaced with valine, the residue present in CLC channels, or with cysteine, methionine, or asparagine (data not shown).
To exclude that the lower transport rates exhibited by these mutants are due to a reduced abundance in the plasma membrane, we inserted an extracellular HA tag into some of these constructs and measured the protein expression on the membrane surface as described under "Experimental Procedures." Fig. 3 shows that these mutants were present in the plasma membrane to a comparable degree. Thus the lack of transport activity of ClC-5 mutants E268A and E268R cannot be ascribed to a reduced surface expression. Western blots of total oocytes indicated similar overall expression as well (supplemental Fig. S2).
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Replacing external Cl- with
or SCN- increased ClC-4 and -5 currents (7, 25, 26). Anion flux through ecClC-1 is partially or totally uncoupled from H+ with transport of
or SCN-, respectively (27). Likewise, ClC-4 and -5 show less H+ countertransport with
or SCN- (Fig. 5, A and B), with an almost complete loss of H+ transport in SCN-. However, uncoupling with SCN- has to be viewed with caution, as SCN- also induces rather large currents in uninjected oocytes (supplemental Fig. S4A) and in mock-transfected mammalian cells (data not shown). Quantitatively comparing pHi changes with the transferred charge confirmed partial uncoupling by
and SCN- (Fig. 5C). The partial uncoupling of
or SCN- fluxes from H+ transport suggested that these anions might permeate ClC-4 or -5 even when their proton glutamates are replaced with nondissociable residues. However, also with a replacement of extracellular Cl- with
or SCN-, ClC-5E268A failed to give currents differing from uninjected controls (supplemental Fig. S4, A and B), in contrast to the E268D mutant (supplemental Fig. S4C), which still supports Cl-/H+ exchange. We did not observe significant currents with the E268A mutant when applying solutions in the pH range from 5.5 to 8.5, even in the presence of
(data not shown).
We next inserted proton glutamates into ClC-0 and -1. These mutations affected gating, but did not transform those Cl- channels into Cl-/H+ exchangers, as H+ transport was undetectable. Reversal potential measurements confirmed this conclusion (supplemental Fig. S5 and Table 1).
To explore whether the coupled Cl-/H+ exchange depends on the presence of two fully functional subunits of the CLC, we analyzed concatemers. Currents and pHo changes of control WT-WT dimers (Fig. 6A) resembled those of WT ClC-5, as did those of concatemers linking a E268A with a WT subunit (Fig. 6B). A concatemer linking a WT subunit to the uncoupled gating glutamate mutant E211A also transported H+ (Fig. 6C). It mediated significant currents at negative voltages (Fig. 6, C and D), demonstrating that the E211A subunit is functional and not qualitatively altered by the WT subunit. These results suggest that a single subunit is able to perform ion exchange independently from the other subunit.
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= 1/(2
f), the lower frequencies correspond to time constants of 10.6 and 0.7 ms, respectively, consistent with the time constants of the macroscopic current relaxation. Also the lorentzian appearance of the power spectrum is a priori expected for an ion channel but not for a transporter (28). | DISCUSSION |
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Polyatomic anions like SCN-,
, and
permeate ecClC-1 with only partial or no coupling to H+ (27, 29). We observed similar uncoupling in ClC-4 and -5. If these polyatomic anions can permeate without coupling to H+, they also might yield currents when the supply of H+ is blocked by proton glutamate mutations. Because this was not observed, mutations in the proton glutamate may affect anion transport not just by preventing anion/H+ exchange. Because either glutamate or histidine promoted Cl-/H+ exchange, electrostatic effects seem unlikely. Probably protonation (or neutralization) of the gating glutamate is essential also for the uncoupled SCN- transport.
CLC proteins function as (homo)dimers with two pores (13, 14, 30). Conduction properties of CLC channels are determined by their monomers (31), but certain gates can close both pores simultaneously. In a similar manner there might be a link between Cl-/H+ exchange and the dimeric structure. However, our studies of concatemers showed that each subunit can mediate Cl-/H+ exchange independently of the transport activity of the second subunit.
We report the first estimate for an apparent unitary conductance of ClC-5. The value of 0.45 ± 0.06 picosiemens is similar to results for ClC-4 (26). Nonstationary noise analysis is usually applied only to ion channels, but has also revealed gating events in the Na+/Ca2+ exchanger (32). In analogy to the model of Hilgemann (32), we interpret the results of the noise analysis in the following manner. Electrogenic Cl-/H+ exchange, which occurs at a very high rate, is switched on and off by a gating process. Each burst of transport activity is associated with an electrical conductance of 0.45 picosiemens, as the elementary electrogenic exchange processes cannot be temporally resolved. Such a behavior is qualitatively illustrated in Fig. 8A. The recording bandwidth is not sufficient to resolve individual transport events. The noise at the frequencies that can be measured is thus dominated by the gating of the bursts. Assuming that the unitary current reflects the charge transport rate of a single transporter and assuming a transport stoichiometry of 2Cl-/1H+ as for ecClC-1 (4, 27), a transport turnover rate (at 100 mV) of about 105 s-1 can be estimated. The turnover rate of ecClC-1 was estimated to 4000 s-1 at 0 mV (33). If the strong rectification of ClC-5 reflects a voltage dependence of the turnover rate, ClC-5 turnover at less positive voltages may resemble that of ecClC-1.
As with CLC channels, neutralizing the gating glutamate of ClC-4 or -5 abolished rectification and current relaxations after voltage jumps, possibly suggesting that rectification results from voltage-dependent gating. However, >80% of the current increase upon depolarization is instantaneous. Hence, in a re-interpretation of the results of Hebeisen et al. (26), we propose that the major part of rectification stems from an intrinsic voltage dependence of "turned on" Cl-/H+ exchange. The gating glutamate may need to be protonated to allow anion permeation (15). If protons can reach this glutamate in ClC-4 and -5 only from the intracellular side along a path involving the proton glutamate and must be driven there against an energy barrier by voltage, outward rectification ensues. Fig. 8B schematically illustrates this scenario. As expected from this model, currents increased exponentially with voltage, in contrast to a gating process, which finally saturates at the maximal open probability of 1. The exponential current increase also implies that neither the supply of H+ from the cytoplasmic solution to the proton glutamate nor the delivery of H+ to the extracellular solution is rate-limiting.
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| FOOTNOTES |
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The on-line version of this article (available at http://www.jbc.org) contains supplemental Figs. S1-S5 and Table 1. ![]()
1 Both authors contributed equally to this work. ![]()
2 Present address: London Epithelial Group, Royal Free Hospital, UCL, London NW 3 2PF, United Kingdom. ![]()
3 Fellow of the Leibniz Graduate School of Biophysics. ![]()
4 To whom correspondence may be addressed: MDC/FMP, Robert-Rössle-Str. 10, D-13125 Berlin, Germany. E-mail: jentsch{at}fmp-berlin.de.
5 To whom correspondence may be addressed: Istituto di Biofisica, CNR, Via de Marini 6, I-16149 Genova, Italy. E-mail: pusch{at}ge.ibf.cnr.it.
6 The abbreviations used are: CLC, a gene family of Cl- channels and transporters first identified by the cloning of ClC-0 from Torpedo; BCECF, 2',7'-bis(carboxyethyl)-5(6)-carboxyfluorescein; MES, 2-(N-morpholino)ethane-sulfonic acid; ecClC-1, one of the two CLC isoforms in E. coli, also known as ClC-ec1; pHi, intracellular pH; pHo, extracellular pH; WT, wild type; HA, hemagglutinin. ![]()
| ACKNOWLEDGMENTS |
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| REFERENCES |
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