Exterior site occupancy infers chloride-induced proton gating in a prokaryotic homolog of the ClC chloride channel

The ClC family of anion channels mediates the efficient, selective permeation of Cl(-) across the biological membranes of living cells under the driving force of an electrochemical gradient. In some eukaryotes, these channels are known to exhibit a unique gating mechanism, which appears to be triggered by the permeant Cl(-) anion. We infer details of this gating mechanism by studying the free energetics of Cl(-) occupancy in the pore of a prokaryotic ClC homolog. These free energetics were gleaned from 30 ns of molecular dynamics simulation on an approximately 133,000-atom system consisting of a hydrated membrane embedded StClC transporter. The binding sites for Cl(-) in the transporter were determined for the cases where the putative gating residue, Glu(148), was protonated and unprotonated. When the glutamate gate is protonated, Cl(-) favorably occupies an exterior site, S(ext), to form a queue of anions in the pore. However, when the glutamate gate is unprotonated, Cl(-) cannot occupy this site nor, consequently, pass through the pore. An additional, previously undetected, site was found in the pore near the outer membrane that exists regardless of the protonation state of Glu(148). Although this suggests that, for the prokaryotic homolog, protonation of Glu(148) may be the first step in transporting Cl(-) at the expense of H(+) transport in the opposite direction, an evolutionary argument might suggest that Cl(-) opens the ClC gate in eukaryotic channels by inducing the conserved glutamate's protonation. During an additional 20 ns free dynamics simulation, the newly discovered outermost site, S(out), and the innermost site, S(int), were seen to allow spontaneous exchange of Cl(-) ions with the bulk electrolyte while under depolarization conditions.     

Proton pathways and H+/Cl- stoichiometry in bacterial chloride transporters

H+/Cl- antiport behavior has recently been observed in bacterial chloride channel homologs and eukaryotic CLC-family proteins. The detailed molecular-level mechanism driving the stoichiometric exchange is unknown. In the bacterial structure, experiments and modeling studies have identified two acidic residues, E148 and E203, as key sites along the proton pathway. The E148 residue is a major component of the fast gate, and it occupies a site crucial for both H+ and Cl- transport. E203 is located on the intracellular side of the protein; it is vital for H+, but not Cl-, transport. This suggests two independent ion transit pathways for H+ and Cl- on the intracellular side of the transporter. Previously, we utilized a new pore-searching algorithm, TransPath, to predict Cl- and H+ ion pathways in the bacterial ClC channel homolog, focusing on proton access from the extracellular solution. Here we employ the TransPath method and molecular dynamics simulations to explore H+ pathways linking E148 and E203 in the presence of Cl- ions located at the experimentally observed binding sites in the pore. A conclusion is that Cl- ions are required at both the intracellular (S(int)) and central (S(cen)) binding sites in order to create an electrostatically favorable H+ pathway linking E148 and E203; this electrostatic coupling is likely related to the observed 1H+/2Cl- stoichiometry of the antiporter. In addition, we suggest that a tyrosine residue side chain (Y445), located near the Cl- ion binding site at S(cen), is involved in proton transport between E148 and E203.     

On the mechanism of gating charge movement of ClC-5, a human Cl(-)/H(+) antiporter

ClC-5 is a Cl(-)/H(+) antiporter that functions in endosomes and is important for endocytosis in the proximal tubule. The mechanism of transport coupling and voltage dependence in ClC-5 is unclear. Recently, a transport-deficient ClC-5 mutant (E268A) was shown to exhibit transient capacitive currents. Here, we studied the external and internal Cl(-) and pH dependence of the currents of E268A. Transient currents were almost completely independent of the intracellular pH. Even though the transient currents are modulated by extracellular pH, we could exclude that they are generated by proton-binding/unbinding reactions. In contrast, the charge movement showed a nontrivial dependence on external chloride, strongly supporting a model in which the movement of an intrinsic gating charge is followed by the voltage-dependent low-affinity binding of extracellular chloride ions. Mutation of the external Glu-211 (a residue implicated in the coupling of Cl(-) and proton transport) to aspartate abolished steady-state transport, but revealed transient currents that were shifted by ~150 mV to negative voltages compared to E268A. This identifies Glu(ext) as a major component of the gating charge underlying the transient currents of the electrogenic ClC-5 transporter. The molecular events underlying the transient currents of ClC-5 emerging from these results can be explained by an inward movement of the side chain of Glu(ext), followed by the binding of extracellular Cl(-) ions.     

Pre-steady-state and reverse transport currents in the GABA transporter GAT1

The role of internal substrates in the biophysical properties of the GABA transporter GAT1 has been investigated electrophysiologically in Xenopus oocytes heterologously expressing the cotransporter. Increments in Cl(-) and/or Na(+) concentrations caused by intracellular injections did not produce significant effects on the pre-steady-state currents, while a positive shift of the charge-voltage (Q-V) and decay time constant (τ)-voltage (τ-V) curves, together with a slowing of τ at positive potentials, was observed following treatments producing cytosolic Cl(-) depletion. Activation of the reverse transport mode by injections of GABA caused a reduction in the displaced charge. In the absence of external Cl(-), a stronger reduction in the displaced charge, together with a significant increase in reverse transport current, was observed. Therefore, complementarity between pre-steady-state and transport currents, observed in the forward mode, is preserved in the reverse mode. All these findings can be qualitatively reproduced by a kinetic scheme in which, in the forward mode, the Cl(-) ion is released first, after the inward charge movement, while the two Na(+) ions can be released only after binding of external GABA. In the reverse mode, internal GABA must bind first to the empty transporter, followed by internal Na(+) and Cl(-).     

Reconstructing a chloride-binding site in a bacterial neurotransmitter transporter homologue

In ion-coupled transport proteins, occupation of selective ion-binding sites is required to trigger conformational changes that lead to substrate translocation. Neurotransmitter transporters, targets of abused and therapeutic drugs, require Na(+) and Cl(-) for function. We recently proposed a chloride-binding site in these proteins not present in Cl(-)-independent prokaryotic homologues. Here we describe conversion of the Cl(-)-independent prokaryotic tryptophan transporter TnaT to a fully functional Cl(-)-dependent form by a single point mutation, D268S. Mutations in TnaT-D268S, in wild type TnaT and in serotonin transporter provide direct evidence for the involvement of each of the proposed residues in Cl(-) coordination. In both SERT and TnaT-D268S, Cl(-) and Na(+) mutually increased each other's potency, consistent with electrostatic interaction through adjacent binding sites. These studies establish the site where Cl(-) binds to trigger conformational change during neurotransmitter transport.     

Intracellular proton regulation of ClC-0

Some CLC proteins function as passive Cl(-) ion channels whereas others are secondary active chloride/proton antiporters. Voltage-dependent gating of the model Torpedo channel ClC-0 is modulated by intracellular and extracellular pH, possibly reflecting a mechanistic relationship with the chloride/proton coupling of CLC antiporters. We used inside-out patch clamp measurements and mutagenesis to explore the dependence of the fast gating mechanism of ClC-0 on intracellular pH and to identify the putative intracellular proton acceptor(s). Among the tested residues (S123, K129, R133, K149, E166, F214L, S224, E226, V227, C229, R305, R312, C415, H472, F418, V419, P420, and Y512) only mutants of E166, F214, and F418 qualitatively changed the pH(int) dependence. No tested amino acid emerged as a valid candidate for being a pH sensor. A detailed kinetic analysis of the dependence of fast gate relaxations on pH(int) and [Cl(-)](int) provided quantitative constraints on possible mechanistic models of gating. In one particular model, a proton is generated by the dissociation of a water molecule in an intrapore chloride ion binding site. The proton is delivered to the side chain of E166 leading to the opening of the channel, while the hydroxyl ion is stabilized in the internal/central anion binding site. Deuterium isotope effects confirm that proton transfer is rate limiting for fast gate opening and that channel closure depends mostly on the concentration of OH(-) ions. The gating model is in natural agreement with the finding that only the closing rate constant, but not the opening rate constant, depends on pH(int) and [Cl(-)](int).     

Structure of a slow CLC Cl⁻/H+ antiporter from a cyanobacterium

X-ray crystal structures have been previously determined for three CLC-type transporter homologues, but the absolute unitary transport rate is known for only one of these. The Escherichia coli Cl(-)/H(+) antiporter (EC) moves ～2000 Cl(-) ions/s, an exceptionally high rate among membrane-transport proteins. It is not known whether such rapid turnover is characteristic of ClCs in general or if the E. coli homologue represents a functional outlier. Here, we characterize a CLC Cl(-)/H(+) antiporter from the cyanobacterium Synechocystis sp. PCC6803 (SY) and determine its crystal structure at 3.2 ? resolution. The structure of SY is nearly identical to that of EC, with all residues involved in Cl(-) binding and proton coupling structurally similar to their equivalents in EC. SY actively pumps protons into liposomes against a gradient and moves Cl(-) at ～20 s(-1), 1% of the EC rate. Electrostatic calculations, used to identify residues contributing to ion binding energetics in SY and EC, highlight two residues flanking the external binding site that are destabilizing for Cl(-) binding in SY and stabilizing in EC. Mutation of these two residues in SY to their counterparts in EC accelerates transport to ～150 s(-1), allowing measurement of Cl(-)/H(+) stoichiometry of 2/1. SY thus shares a similar structure and a common transport mechanism to EC, but it is by comparison slow, a result that refutes the idea that the transport mechanism of CLCs leads to intrinsically high rates.     

Leucokinin and the modulation of the shunt pathway in Malpighian tubules

Transepithelial secretion in Malpighian tubules of the yellow fever mosquito (Aedes aegypti) is mediated by active transport of Na(+) and K(+) through principal cells and passive Cl(-) transport through the shunt. Permeation through the shunt was assessed by measuring transepithelial halide diffusion potentials in isolated perfused Malpighian tubules, after first inhibiting active transport with dinitrophenol. Diffusion potentials were small under control conditions, revealing Eisenman selectivity sequence I (I(-)>Br(-)>Cl(-)>F(-)) which is the halide mobility sequence in free solution. Accordingly, electrical field strengths of the shunt are small, selecting halides for passage on the basis of hydrated size. Leucokinin-VIII (LK-VIII) significantly increased the shunt conductance from 57.1 μS/cm to 250.0 μS/cm. In parallel, the shunt selectivity sequence shifted to Eisenman sequence III (Br(-)>Cl(-)>I(-)>F(-)), revealing increased electrical field strengths in the shunt, now capable of selecting small, dehydrated halides for passage. High concentrations of peritubular F(-) (142.5 mM) duplicated the effects of LK-VIII on shunt conductance and selectivity, suggesting a role for G-protein. In the presence of LK-VIII (or F(-)), coulombic interactions between the shunt and I(-) and F(-) may be strong enough to cause binding, thereby blocking the passage of Cl(-). Thus, LK-VIII increases both shunt conductance and selectivity, presumably via G-protein.     

Molecular mechanism of substrate specificity in the bacterial neutral amino acid transporter LeuT

The recently published X-ray structure of LeuT, a Na(+)/Cl(-)-dependent neurotransmitter transporter, has provided fresh impetus to efforts directed at understanding the molecular principles governing specific neurotransmitter transport. The combination of the LeuT crystal structure with the results of molecular simulations enables the functional data on specific binding and transport to be related to molecular structure. All-atom FEP and molecular dynamics (MD) simulations of LeuT embedded in an explicit membrane were performed alongside a decomposition analysis to dissect the molecular determinants of the substrate specificity of LeuT. It was found that the ligand must be in a zwitterionic (ZW) form to bind tightly to the transporter. The theoretical results on the absolute binding-free energies for leucine, alanine, and glycine show that alanine can be a potent substrate for LeuT, although leucine is preferred, which is consistent with the recent experimental data (Singh et al., Nature 2007;448:952-956). Furthermore, LeuT displays robust specificity for leucine over glycine. Interestingly, the ability of LeuT to discriminate between substrates relies on the dynamics of residues that form its binding pocket (e.g., F253 and Q250) and the charged side chains (R30-D404) from a second coordination shell. The water-mediated R30-D404 salt bridge is thought to be part of the extracellular (EC) gate of LeuT. The introduction of a polar ligand such as glycine to the water-depleted binding pocket of LeuT gives rise to structural rearrangements of the R30-D404-Q250 hydrogen-bonding network and leads to increased hydration of the binding pocket. Conformational changes associated with the broken hydrogen bond between Q250 and R30 are shown to be important for tight and selective ligand binding to LeuT.     

Ionic currents in the human serotonin transporter reveal inconsistencies in the alternating access hypothesis

We have investigated the conduction states of human serotonin transporter (hSERT) using the voltage clamp, cut-open frog oocyte method under different internal and external ionic conditions. Our data indicate discrepancies in the alternating access model of cotransport, which cannot consistently explain substrate transport and electrophysiological data. We are able simultaneously to isolate distinct external and internal binding sites for substrate, which exert different effects upon currents conducted by hSERT, in contradiction to the alternating access model. External binding sites of coupled Na ions are likewise simultaneously accessible from the internal and external face. Although Na and Cl are putatively cotransported, they have opposite effects on the internal face of the transporter. Finally, the internal K ion does not compete with internal 5-hydroxytryptamine for empty transporters. These data can be explained more readily in the language of ion channels, rather than carrier models distinguished by alternating access mechanisms: in a channel model of coupled transport, the currents represent different states of the same permeation path through hSERT and coupling occurs in a common pore.     

Cysteine 144 in the third transmembrane domain of the creatine transporter is located close to a substrate-binding site

All creatine transporters contain a cysteine residue (Cys(144)) in the third transmembrane domain that is not present in other members of the Na+,Cl(-)-dependent family of neurotransmitter transporters. Site-directed mutagenesis and reaction with methane thiosulfonates were used to investigate the importance of Cys(144) for transporter function. Replacement of Cys(144) with Ser did not significantly affect the kinetics or activity of the transporter, whereas a C144A mutant had a higher K(m) (0.33 compared with 0.18 mm). Substitution of Cys(144) with Leu gave a mutant with a 5-fold higher K(m) and a reduced specificity for substrate. Low concentrations of 2-aminoethyl methanethiosulfonate (MTSEA) resulted in rapid inactivation of the creatine transporter. The C144S mutant was resistant to inactivation, indicating that modification of Cys(144) was responsible for the loss of transport activity. Creatine and analogues that function as substrates of the creatine transporter were able to protect from MTSEA inactivation. Na+ and Cl(-) ions were not necessary for MTSEA inactivation, but Na+ was found to be important for creatine protection from inactivation. Our results indicate that cysteine 144 is close to the binding site or part of a permeation channel for creatine.     

Interfacial interactions of glutamate, water and ions with carbon nanopore evaluated by molecular dynamics simulations

Molecular dynamics simulations were used to assess the transport of glutamate, water and ions (Na(+) and Cl(-)) in a single wall carbon nanopore. The spatial profiles of Na(+) and Cl(-) ions are largely determined by the pore wall charges. Co-ions are repelled whereas the counter-ions are attracted by the pore charges, but this 'rule' breaks down when the water concentration is set to a level significantly below that in the physiological bulk solution. In such cases water is less able to counteract the ion-wall interactions (electrostatic or non-electrostatic), co-ions are layered near the counter-ions attracted by the wall charges and are thus layered as counter-ions. Glutamate is concentrated near the pore wall even at physiological water concentration, and irrespective of whether the pore wall is neutral or charged (positively or negatively), and its peak levels are up to 40 times above mean values. The glutamate is thus always layered as a counter-ion. Layering of water near the wall is independent of charges on the pore wall, but its peak levels near the wall are 'only' 6-8 times above the pore mean values. However, if the mean concentration of water is significantly below the level in the physiological bulk solution, its layering is enhanced, whereas its concentration in the pore center diminishes to very low levels. Reasons for such a 'paradoxical' behavior of molecules (glutamate and water) are that the non-electrostatic interactions are (except at very short distances) attractive, and electrostatic interactions (between the charged atoms of the glutamate or water and the pore wall) are also attractive overall. Repulsive interactions (between equally charged atoms) exist, and they order the molecules near the wall, whereas in the pore center the glutamate (and water) angles are largely randomly distributed, except in the presence of an external electric field. Diffusion of molecules and ions is complex. The translational diffusion is in general both inhomogeneous and anisotropic. Non-electrostatic interactions (ion-wall, glutamate-wall or water-wall) powerfully influence diffusion. In the neutral nanopore the effective axial diffusion constants of glutamate, water and Na(+) and Cl(-) ions are all <10% of their values in the bulk, and the electrostatic interactions can reduce them further. Diffusion of molecules and ions is further reduced if the water concentration in the pore is low. Glutamate(-) is slowed more than water, and ions are reduced the most especially co-ions. In conclusion the interfacial interactions influence the spatial distribution of glutamate, water and ions, and regulate powerfully, in a complex manner and over a very wide range their transport through nanosize pores.     

Evidence for a second binding/transport site for chloride in erythrocyte anion transporter AE1 modified at glutamate 681

Transport kinetics have been examined in erythrocyte anion transporter AE1 that has been chemically modified to convert glutamate 681 to an alcohol (E681OH AE1). Outward conductive Cl(-) flux in E681OH AE1 is inhibited by removal of extracellular Cl(-); this effect is the opposite of that in native AE1 and is consistent with coupled electrogenic 2:1 Cl(-)/Cl(-) exchange. A second Cl(-) binding/transport site is also suggested by the characteristics of (35)SO(4)(2-) flux in E681OH AE1: bilateral and cis Cl(-), which are normally inhibitory, accelerate (35)SO(4)(2-) flux. These effects would be expected if Cl(-) binds to a second transport site on SO(4)(2-)-loaded E681OH AE1, thereby allowing Cl(-)/SO(4)(2-) cotransport. Alternatively, the data can be explained without proposing Cl(-)/SO(4)(2-) cotransport if the rate-limiting event for (35)SO(4)(2-)/SO(4)(2-) exchange is external SO(4)(2-) release, and the binding of external Cl(-) accelerates SO(4)(2-) release. With either interpretation, these data indicate that E681OH AE1 has a binding/transport site for Cl(-) that is distinct from the main transport site. The effects of graded modification of E681 or inhibition by H(2)DIDS are consistent with the idea that the new Cl(-) binding site is on the same E681OH-modified subunit of the AE1 dimer as the normal transport site.     

Presteady-state and steady-state kinetics and turnover rate of the mouse gamma-aminobutyric acid transporter (mGAT3)

We expressed mouse gamma-aminobutyric acid (GABA) transporter (mGAT3) in Xenopus laevis oocytes and examined its steady-state and presteady-state kinetics and turnover rate by using tracer flux and electrophysiological methods. In oocytes expressing mGAT3, GABA evoked a Na+-dependent and Cl(-)-facilitated inward current. The dependence on Na+ was absolute, whereas that for Cl(-) was not. At a membrane potential of -50 mV, the half-maximal concentrations for Na+, Cl(-), and GABA were 14 mM, 5 mM, and 3 microM. The Hill coefficient for GABA activation and Cl(-) enhancement of the inward current was 1, and that for Na+ activation was > or =2. The GABA-evoked inward current was directly proportional to GABA influx (2.2 +/- 0.1 charges/GABA) into cells, indicating that under these conditions, there is tight ion/GABA coupling in the transport cycle. In response to step changes in the membrane voltage and in the absence of GABA, mGAT3 exhibited presteady-state current transients (charge movements). The charge-voltage (Q-V) relation was fitted with a single Boltzmann function. The voltage at half-maximal charge (V(0.5)) was +25 mV, and the effective valence of the moveable charge (zdelta) was 1.6. In contrast to the ON transients, which relaxed with a time constant of < or =30 msec, the OFF transients had a time constant of 1.1 sec. Reduction in external Na+ ([Na+]o) and Cl(-) ([Cl(-)]o) concentrations shifted the Q-V relationship to negative membrane potentials. At zero [Na+]o (106 mM Cl(-)), no mGAT3-mediated transients were observed, and at zero [Cl(-)]o (100 mM Na+), the charge movements decreased to approximately 30% of the maximal charge (Q(max)). GABA led to the elimination of charge movements. The half-maximal concentrations for Na+ activation, Cl(-) enhancement, and GABA elimination of the charge movements were 48 mM, 19 mM, and 5 mM, respectively. Q(max) and I(max) obtained in the same cells yielded the mGAT3 turnover rate, 1.7 sec(-1) at -50 mV. The low turnover rate of mGAT3 may be due to the slow return of the empty transporter from the internal to the external membrane surface.     

Homology model of the GABAA receptor examined using Brownian dynamics

We have developed a homology model of the GABA(A) receptor, using the subunit combination of alpha1beta2gamma2, the most prevalent type in the mammalian brain. The model is produced in two parts: the membrane-embedded channel domain and the extracellular N-terminal domain. The pentameric transmembrane domain model is built by modeling each subunit by homology with the equivalent subunit of the heteropentameric acetylcholine receptor transmembrane domain. This segment is then joined with the extracellular domain built by homology with the acetylcholine binding protein. The all-atom model forms a wide extracellular vestibule that is connected to an oval chamber near the external surface of the membrane. A narrow, cylindrical transmembrane channel links the outer segment of the pore to a shallow intracellular vestibule. The physiological properties of the model so constructed are examined using electrostatic calculations and Brownian dynamics simulations. A deep energy well of approximately 80 kT accommodates three Cl(-) ions in the narrow transmembrane channel and seven Cl(-) ions in the external vestibule. Inward permeation takes place when one of the ions queued in the external vestibule enters the narrow segment and ejects the innermost ion. The model, when incorporated into Brownian dynamics, reproduces key experimental features, such as the single-channel current-voltage-concentration profiles. Finally, we simulate the gamma2 K289M epilepsy inducing mutation and examine Cl(-) ion permeation through the mutant receptor.     

A synthetic chloride channel restores chloride conductance in human cystic fibrosis epithelial cells

Mutations in the gene-encoding cystic fibrosis transmembrane conductance regulator (CFTR) cause defective transepithelial transport of chloride (Cl(-)) ions and fluid, thereby becoming responsible for the onset of cystic fibrosis (CF). One strategy to reduce the pathophysiology associated with CF is to increase Cl(-) transport through alternative pathways. In this paper, we demonstrate that a small synthetic molecule which forms Cl(-) channels to mediate Cl(-) transport across lipid bilayer membranes is capable of restoring Cl(-) permeability in human CF epithelial cells; as a result, it has the potential to become a lead compound for the treatment of human diseases associated with Cl(-) channel dysfunction.     

The Molecular Mechanism of Ion-Dependent Gating in Secondary Transporters

LeuT-like fold Na-dependent secondary active transporters form a large family of integral membrane proteins that transport various substrates against their concentration gradient across lipid membranes, using the free energy stored in the downhill concentration gradient of sodium ions. These transporters play an active role in synaptic transmission, the delivery of key nutrients, and the maintenance of osmotic pressure inside the cell. It is generally believed that binding of an ion and/or a substrate drives the conformational dynamics of the transporter. However, the exact mechanism for converting ion binding into useful work has yet to be established. Using a multi-dimensional path sampling (string-method) followed by all-atom free energy simulations, we established the principal thermodynamic and kinetic components governing the ion-dependent conformational dynamics of a LeuT-like fold transporter, the sodium/benzyl-hydantoin symporter Mhp1, for an entire conformational cycle. We found that inward-facing and outward-facing states of Mhp1 display nearly the same free energies with an ion absent from the Na2 site conserved across the LeuT-like fold transporters. The barrier separating an apo-state from inward-facing or outward-facing states of the transporter is very low, suggesting stochastic gating in the absence of ion/substrate bound. In contrast, the binding of a Na2 ion shifts the free energy stabilizing the outward-facing state and promoting substrate binding. Our results indicate that ion binding to the Na2 site may also play a key role in the intracellular thin gate dynamics modulation by altering its interactions with the transmembrane helix 5 (TM5). The Potential of Mean Force (PMF) computations for a substrate entrance displays two energy minima that correspond to the locations of the main binding site S1 and proposed allosteric S2 binding site. However, it was found that substrate''s binds to the site S1 ∼5 kcal/mol more favorable than that to the site S2 for all studied bound combinations of ions and a substrate.     

GABA reverse transport by the neuronal cotransporter GAT1: influence of internal chloride depletion

The role of intracellular ions on the reverse GABA transport by the neuronal transporter GAT1 was studied using voltage-clamp and [(3)H]GABA efflux determinations in Xenopus oocytes transfected with heterologous mRNA. Reverse transport was induced by intracellular GABA injections and measured in terms of the net outward current generated by the transporter. Changes in various intracellular ionic conditions affected the reverse current: higher concentrations of Na(+) enhanced the ratio of outward over inward transport current, while a considerable decrease of the outward current and a parallel reduction of the transporter-mediated GABA efflux were observed after treatments causing a diminution of the intracellular Cl(-) concentration. Particularly interesting was the impairment of the reverse transport observed after depletion of internal Cl(-) generated by the activity of a coexpressed K(+)-Cl(-) exporter KCC2. This finding suggests that reverse GABA transport may be physiologically regulated during early neuronal development, similarly to the functional alterations seen in GABA receptors caused by KCC2 activity.     

Oxidation of the Mn cluster induces structural changes of NO3- functionally bound to the Cl- site in the oxygen-evolving complex of photosystem II

Cl(-) is an indispensable cofactor for photosynthetic O(2) evolution and is functionally replaced by NO(3)(-). Structural changes of an isotopically labeled NO(3)(-) ion, induced by the oxidation of the Mn cluster (S(1)-to-S(2)), were detected by FTIR spectroscopy. NO(3)(-)-substituted photosystem II core particles showed (14)N(16)O(3)(-)/(15)N(16)O(3)(-) and (14)N(16)O(3)(-)/(14)N(18)O(3)(-) isotopic bands in the S(2)/S(1) spectra with markedly high signal/noise ratio. These bands appeared only in the region from 1415 to 1284 cm(-1), indicating that the bands do not arise from a metal-bound NO(3)(-) but from an ionic NO(3)(-). The intensity of the bands exhibited a quantitatively proportional relationship with the O(2) activity. These results demonstrate that the NO(3)(-) functionally bound to the Cl(-) site couples to the Mn cluster structurally, but is not associated with the cluster as a direct ligand. Comparison of the bands for two isotopes ((15)N and (18)O) and their simulations enable us to assign each band to the S(1) and S(2) states. The results indicate that the NO(3)(-) ion bound to the Cl(-) site is highly asymmetric in S(1) but rather symmetric in S(2). Since NO(3)(-) functionally replaces Cl(-), most of the conclusions drawn from this study will be also applicable to Cl(-).     

Does the presence of a seawater gill morphology induced by dietary salt loading affect Cl(-) uptake and acid-base regulation in freshwater rainbow trout Oncorhynchus mykiss

The goal of this study was to determine the effect of the changes in gill morphology induced by dietary salt feeding on several aspects of gill function in rainbow trout Oncorhynchus mykiss maintained in fresh water with specific emphasis on Cl(-) uptake (J(IN)Cl(-)) and acid-base regulation. The addition of 11% NaCl to the diet caused J(IN)Cl(-) to be reduced by c. 45% from 214·4 ± 26·7 to 117·3 ± 17·4 μmol kg(-1) h(-1) (mean ± s.e.). Rates of Cl(-) efflux (J(OUT)Cl(-)), net Cl(-) flux (J(NET)Cl(-)), J(NET) Na(+) and plasma levels of Na(+) or Cl(-) were unaffected by salt feeding. On the basis of significant effect of the salt diet on decreasing the maximal uptake rate of Cl(-)(J(MAX)Cl(-)), it would appear that internal salt loading caused a decrease in the number of functional ion transport proteins involved in Cl(-) uptake (e.g. Cl(-) -HCO(3)(-) exchangers) and decreased the transporting capacity of existing proteins. The acid-base regulating capacity of control fish and salt-loaded fish was assessed by monitoring arterial blood acid-base status [partial pressure of CO(2) (PCO(2)), pH and HCO(3)(-)] during exposure to external hypercapnia (nominally 7·5 mm Hg). Both groups of fish exhibited typical compensatory responses to sustained hypercapnia consisting of the gradual accumulation of plasma HCO(3) (-) and thus metabolic restoration within 24 h of the initial respiratory acidosis elicited by hypercapnia. Overall, the results demonstrate that while Cl(-) uptake capacity is reduced in salt-fed fish, there is no associated alteration in acid-base regulating capability.