The anion conductance of the glutamate transporter EAAC1 depends on the direction of glutamate transport

The steady-state and pre-steady-state kinetics of glutamate transport by the neuronal glutamate transporter EAAC1 were determined under conditions of outward glutamate transport and compared to those found for the inward transport mode. In both transport modes, the glutamate-induced current is composed of two components, the coupled transport current and the uncoupled anion current, and inhibited by a specific non-transportable inhibitor. Furthermore, the glutamate-independent leak current is observed in both transport modes. Upon a glutamate concentration jump outward transport currents show a distinct transient phase that deactivates within 15 ms. The results demonstrate that the general properties of EAAC1 are symmetric, but the rates of substrate transport and anion flux are asymmetric with respect to the orientation of the substrate binding site in the membrane. Therefore, the EAAC1 anion conductance differs from normal ligand-gated ion channels in that it can be activated by glutamate and Na(+) from both sides of the membrane.     

Structural rearrangements at the translocation pore of the human glutamate transporter, EAAT1

Structure-function studies of mammalian and bacterial excitatory amino acid transporters (EAATs), as well as the crystal structure of a related archaeal glutamate transporter, support a model in which TM7, TM8, and the re-entrant loops HP1 and HP2 participate in forming a substrate translocation pathway within each subunit of a trimer. However, the transport mechanism, including precise binding sites for substrates and co-transported ions and changes in the tertiary structure underlying transport, is still not known. In this study, we used chemical cross-linking of introduced cysteine pairs in a cysteine-less version of EAAT1 to examine the dynamics of key domains associated with the translocation pore. Here we show that cysteine substitution at Ala-395, Ala-367, and Ala-440 results in functional single and double cysteine transporters and that in the absence of glutamate or dl-threo-beta-benzyloxyaspartate (dl-TBOA), A395C in the highly conserved TM7 can be cross-linked to A367C in HP1 and to A440C in HP2. The formation of these disulfide bonds is reversible and occurs intra-molecularly. Interestingly, cross-linking A395C to A367C appears to abolish transport, whereas cross-linking A395C to A440C lowers the affinities for glutamate and dl-TBOA but does not change the maximal transport rate. Additionally, glutamate and dl-TBOA binding prevent cross-linking in both double cysteine transporters, whereas sodium binding facilitates cross-linking in the A395C/A367C transporter. These data provide evidence that within each subunit of EAAT1, Ala-395 in TM7 resides close to a residue at the tip of each re-entrant loop (HP1 and HP2) and that these residues are repositioned relative to one another at different steps in the transport cycle. Such behavior likely reflects rearrangements in the tertiary structure of the translocation pore during transport and thus provides constraints for modeling the structural dynamics associated with transport.     

Proximity of two oppositely oriented reentrant loops in the glutamate transporter GLT-1 identified by paired cysteine mutagenesis.

Sodium- and potassium-coupled transporters clear the excitatory neurotransmitter glutamate from the synaptic cleft. Their function is essential for effective glutamatergic neurotransmission. Glutamate transporters have an unusual topology, containing eight membrane-spanning domains and two reentrant loops of opposite orientation. We have introduced pairwise cysteine substitutions in several structural elements of the GLT-1 transporter. A complete inhibition of transport by Cu(II)(1,10-phenanthroline)(3) is observed in the double mutants A412C/V427C and A364C/S440C, but not in the corresponding single mutants. No inhibition is observed in more then 20 other double cysteine mutants. The Cu(II)(1,10-phenanthroline)(3) inhibition can be partly prevented by the nontransportable glutamate analogue dihydrokainate. Treatment with dithiothreitol restores much of the transport activity. Moreover, micromolar concentrations of cadmium ions reversibly inhibit transport catalyzed by A412C/V427C and A364C/S440C double mutants, but not by the corresponding single mutants. Inhibition by Cu(II)(1,10-phenanthroline)(3) and by cadmium is only observed when the cysteine pairs are introduced in the same polypeptide. Therefore, in both cases the proximity appears to be intra- rather than intermolecular. Positions 364 and 440 are located on reentrant loop I and II, respectively. Our results suggest that these two loops, previously shown to be essential for glutamate transport, come in close proximity.     

Two conformational changes are associated with glutamate translocation by the glutamate transporter EAAC1

Glutamate is transported across membranes by means of a carrier mechanism that is thought to require conformational changes of the transport protein. In this work, we have determined the thermodynamic parameters of glutamate and the Na+ binding steps to their extracellular binding sites along with the activation parameters of rapid, glutamate-induced processes in the transport cycle by analyzing the temperature dependence of glutamate transport at steady state and pre-steady state. Our results suggest that glutamate binding to the transporter is driven by a negative reaction enthalpy (DeltaH0 = -33 kJ/mol), whereas the tighter binding of the non-transportable inhibitor TBOA is caused by an additional increase in entropy. Processes linked to the binding of glutamate and Na+ to the transporter are associated with low activation barriers, indicative of diffusion-controlled reactions. The activation enthalpies of two processes in the glutamate translocation branch of the transport cycle were DeltaH++ = 95 kJ/mol and DeltaH++ = 120 kJ/mol, respectively. Such large values of DeltaH++ suggest that these processes are rate-limited by conformational changes of the transporter. We also found a large activation barrier for steady-state glutamate transport, which is rate-limited by the K+-dependent relocation of the empty transporter. Together, these results suggest that two conformational changes accompany glutamate translocation and at least one conformational change accompanies the relocation of the empty transporter. We interpret the data with an alternating access model that includes the closing and opening of an extracellular and an intracellular gate, respectively, in analogy to a hypothetical model proposed previously on the basis of the crystal structure of the bacterial glutamate transporter GltPh.     

Functional Consequences of Sulfhydryl Modification of the γ-Aminobutyric Acid Transporter 1 at a Single Solvent-Exposed Cysteine Residue

The aims of this study were to optimize the experimental conditions for labeling extracellularly oriented, solvent-exposed cysteine residues of ??-aminobutyric acid transporter 1 (GAT1) with the membrane-impermeant sulfhydryl reagent [2-(trimethylammonium)ethyl]methanethiosulfonate (MTSET) and to characterize the functional and pharmacological consequences of labeling on transporter steady-state and presteady-state kinetic properties. We expressed human GAT1 in Xenopus laevis oocytes and used radiotracer and electrophysiological methods to assay transporter function before and after sulfhydryl modification with MTSET. In the presence of NaCl, transporter exposure to MTSET (1?C2.5?mM for 5?C20?min) led to partial inhibition of GAT1-mediated transport, and this loss of function was completely reversed by the reducing reagent dithiothreitol. MTSET treatment had no functional effect on the mutant GAT1 C74A, whereas the membrane-permeant reagents N-ethylmaleimide and tetramethylrhodamine-6-maleimide inhibited GABA transport mediated by GAT1 C74A. Ion replacement experiments indicated that MTSET labeling of GAT1 could be driven to completion when valproate replaced chloride in the labeling buffer, suggesting that valproate induces a GAT1 conformation that significantly increases C74 accessibility to the extracellular fluid. Following partial inhibition by MTSET, there was a proportional reduction in both the presteady-state and steady-state macroscopic signals, and the functional and pharmacological properties of the remaining signals were indistinguishable from those of unlabeled GAT1. Therefore, covalent modification of GAT1 at C74 results in completely nonfunctional as well as electrically silent transporters.     

A conserved aspartate residue located at the extracellular end of the binding pocket controls cation interactions in brain glutamate transporters

In the brain, transporters of the major excitatory neurotransmitter glutamate remove their substrate from the synaptic cleft to allow optimal glutamatergic neurotransmission. Their transport cycle consists of two sequential translocation steps, namely cotransport of glutamic acid with three Na(+) ions, followed by countertransport of K(+). Recent studies, based on several crystal structures of the archeal homologue Glt(Ph), indicate that glutamate translocation occurs by an elevator-like mechanism. The resolution of these structures was not sufficiently high to unambiguously identify the sites of Na(+) binding, but functional and computational studies suggest some candidate sites. In the Glt(Ph) structure, a conserved aspartate residue (Asp-390) is located adjacent to a conserved tyrosine residue, previously shown to be a molecular determinant of ion selectivity in the brain glutamate transporter GLT-1. In this study, we characterize mutants of Asp-440 of the neuronal transporter EAAC1, which is the counterpart of Asp-390 of Glt(Ph). Except for substitution by glutamate, this residue is functionally irreplaceable. Using biochemical and electrophysiological approaches, we conclude that although D440E is intrinsically capable of net flux, this mutant behaves as an exchanger under physiological conditions, due to increased and decreased apparent affinities for Na(+) and K(+), respectively. Our present and previous data are compatible with the idea that the conserved tyrosine and aspartate residues, located at the external end of the binding pocket, may serve as a transient or stable cation binding site in the glutamate transporters.     

The accessibility in the external part of the TM5 of the glutamate transporter EAAT1 is conformationally sensitive during the transport cycle

Background

Excitatory amino acid transporter 1 (EAAT1) is a glutamate transporter which is a key element in the termination of the synaptic actions of glutamate. It serves to keep the extracellular glutamate concentration below neurotoxic level. However the functional significance and the change of accessibility of residues in transmembrane domain (TM) 5 of the EAAT1 are not clear yet.

Methodology/Principal Findings

We used cysteine mutagenesis with treatments with membrane-impermeable sulfhydryl reagent MTSET [(2-trimethylammonium) methanethiosulfonate] to investigate the change of accessibility of TM5. Cysteine mutants were introduced from position 291 to 300 of the cysteine-less version of EAAT1. We checked the activity and kinetic parameters of the mutants before and after treatments with MTSET, furthermore we analyzed the effect of the substrate and blocker on the inhibition of the cysteine mutants by MTSET. Inhibition of transport by MTSET was observed in the mutants L296C, I297C and G299C, while the activity of K300C got higher after exposure to MTSET. V_max of L296C and G299C got lower while that of K300C got higher after treated by MTSET. The L296C, G299C, K300C single cysteine mutants showed a conformationally sensitive reactivity pattern. The sensitivity of L296C to MTSET was potentiated by glutamate and TBOA,but the sensitivity of G299C to MTSET was potentiated only by TBOA.

Conclusions/Significance

All these facts suggest that the accessibility of some positions of the external part of the TM5 is conformationally sensitive during the transport cycle. Our results indicate that some residues of TM5 take part in the transport pathway during the transport cycle.     

The discovery of slowness: low-capacity transport and slow anion channel gating by the glutamate transporter EAAT5

Excitatory amino acid transporters (EAATs) control the glutamate concentration in the synaptic cleft by glial and neuronal glutamate uptake. Uphill glutamate transport is achieved by the co-/countertransport of Na⁺ and other ions down their concentration gradients. Glutamate transporters also display an anion conductance that is activated by the binding of Na⁺ and glutamate but is not thermodynamically coupled to the transport process. Of the five known glutamate transporter subtypes, the retina-specific subtype EAAT5 has the largest conductance relative to glutamate uptake activity. Our results suggest that EAAT5 behaves as a slow-gated anion channel with little glutamate transport activity. At steady state, EAAT5 was activated by glutamate, with a K_m= 61 ± 11 μM. Binding of Na⁺ to the empty transporter is associated with a K_m = 229 ± 37 mM, and binding to the glutamate-bound form is associated with a K_m = 76 ± 40 mM. Using laser-pulse photolysis of caged glutamate, we determined the pre-steady-state kinetics of the glutamate-induced anion current of EAAT5. This was characterized by two exponential components with time constants of 30 ± 1 ms and 200 ± 15 ms, which is an order of magnitude slower than those observed in other glutamate transporters. A voltage-jump analysis of the anion currents indicates that the slow activation behavior is caused by two slow, rate-limiting steps in the transport cycle, Na⁺ binding to the empty transporter, and translocation of the fully loaded transporter. We propose a kinetic transport scheme that includes these two slow steps and can account for the experimentally observed data. Overall, our results suggest that EAAT5 may not act as a classical high-capacity glutamate transporter in the retina; rather, it may function as a slow-gated glutamate receptor and/or glutamate buffering system.     

Cysteine-scanning mutagenesis reveals a conformationally sensitive reentrant pore-loop in the glutamate transporter GLT-1

Removal of glutamate from the synaptic cleft by (Na(+) + K(+))-coupled transporters prevents neurotoxicity due to elevated concentrations of the transmitter. These transporters exhibit an unusual topology, including two reentrant loops. Reentrant loop II plays a pivotal role in coupling ion and glutamate fluxes. Here we used cysteine-scanning mutagenesis of the GLT-1 transporter to test the idea that this loop undergoes conformational changes following sodium and substrate binding. 15 of 22 consecutive single cysteine mutants in the stretch between Gly-422 and Ser-443 exhibited 30-100% of the transport activity of the cysteine-less transporter when expressed in HeLa cells. The transport activity of 11 of the 15 active mutants including five consecutive residues in the ascending limb was inhibited by small hydrophilic methanethiosulfonate reagents. The sensitivity of seven cysteine mutants, including A438C and S440C, to the reagents was significantly reduced by sodium ions, but the opposite was true for A439C. The non-transportable analogue dihydrokainate protected at almost all positions throughout the loop, and at two of the positions, the analogue protected even in the absence of sodium. Our results indicate that reentrant loop II forms part of an aqueous pore, the access of which is blocked by the glutamate analogue dihydrokainate, and that sodium influences the conformation of this pore-loop.     

Neutralization of the aspartic acid residue Asp-367, but not Asp-454, inhibits binding of Na+ to the glutamate-free form and cycling of the glutamate transporter EAAC1

Substrate transport by the plasma membrane glutamate transporter EAAC1 is coupled to cotransport of three sodium ions. One of these Na(+) ions binds to the transporter already in the absence of glutamate. Here, we have investigated the possible involvement of two conserved aspartic acid residues in transmembrane segments 7 and 8 of EAAC1, Asp-367 and Asp-454, in Na(+) cotransport. To test the effect of charge neutralization mutations in these positions on Na(+) binding to the glutamate-free transporter, we recorded the Na(+)-induced anion leak current to determine the K(m) of EAAC1 for Na(+). For EAAC1(WT), this K(m) was determined as 120 mm. When the negative charge of Asp-367 was neutralized by mutagenesis to asparagine, Na(+) activated the anion leak current with a K(m) of about 2 m, indicating dramatically impaired Na(+) binding to the mutant transporter. In contrast, the Na(+) affinity of EAAC1(D454N) was virtually unchanged compared with the wild type transporter (K(m) = 90 mm). The reduced occupancy of the Na(+) binding site of EAAC1(D367N) resulted in a dramatic reduction in glutamate affinity (K(m) = 3.6 mm, 140 mm [Na(+)]), which could be partially overcome by increasing extracellular [Na(+)]. In addition to impairing Na(+) binding, the D367N mutation slowed glutamate transport, as shown by pre-steady-state kinetic analysis of transport currents, by strongly decreasing the rate of a reaction step associated with glutamate translocation. Our data are consistent with a model in which Asp-367, but not Asp-454, is involved in coordinating the bound Na(+) in the glutamate-free transporter form.     

Cysteine Scanning Mutagenesis of Transmembrane Helix 3 of a Brain Glutamate Transporter Reveals Two Conformationally Sensitive Positions

Glutamate transporters in the brain remove the neurotransmitter from the synapse by cotransport with three sodium ions into the surrounding cells. Recent structural work on an archaeal homolog suggests that, during substrate translocation, the transport domain, including the peripheral transmembrane helix 3 (TM3), moves relative to the trimerization domain in an elevator-like process. Moreover, two TM3 residues have been proposed to form part of a transient Na3′ site, and another, Tyr-124, appears close to both Na3′ and Na1. To obtain independent evidence for the role of TM3 in glutamate transport, each of its 31 amino acid residues from the glial GLT-1 transporter was individually mutated to cysteine. Except for six mutants, substantial transport activity was detected. Aqueous accessibility of the introduced cysteines was probed with membrane-permeant and membrane-impermeant sulfhydryl reagents under a variety of conditions. Transport of six single cysteine mutants, all located on the intracellular side of TM3, was affected by membrane-permeant sulfhydryl reagents. However, only at two positions could ligands modulate the reactivity. A120C reactivity was diminished under conditions expected to favor the outward-facing conformation of the transporter. Sulfhydryl modification of Y124C by 2-aminoethyl methanethiosulfonate, but not by N-ethylmaleimide, was fully protected in the presence of sodium. Our data are consistent with the idea that TM3 moves during transport. Moreover, computational modeling indicated that electrostatic repulsion between the positive charge introduced at position 124 and the sodium ions bound at Na3′ and Na1 underlies the protection by sodium.     

Molecular Motions Involved in Na-K-Cl Cotransporter-mediated Ion Transport and Transporter Activation Revealed by Internal Cross-linking between Transmembrane Domains 10 and 11/12

We examined the relationship between transmembrane domain (TM) 10 and TM11/12 in NKCC1, testing homology models based on the structure of AdiC in the same transporter superfamily. We hypothesized that introduced cysteine pairs would be close enough for disulfide formation and would alter transport function: indeed, evidence for cross-link formation with low micromolar concentrations of copper phenanthroline or iodine was found in 3 of 8 initially tested pairs and in 1 of 26 additionally tested pairs. Inhibition of transport was observed with copper phenanthroline and iodine treatment of P676C/A734C and I677C/A734C, consistent with the proximity of these residues and with movement of TM10 during the occlusion step of ion transport. We also found Cu²⁺ inhibition of the single-cysteine mutant A675C, suggesting that this residue and Met³⁸² of TM3 are involved in a Cu²⁺-binding site. Surprisingly, cross-linking of P676C/I730C was found to prevent rapid deactivation of the transporter while not affecting the dephosphorylation rate, thus uncoupling the phosphorylation and activation steps. Consistent with this, (a) cross-linking of P676C/I730C was dependent on activation state, and (b) mutants lacking the phosphoregulatory domain could still be activated by cross-linking. These results suggest a model of NKCC activation that involves movement of TM12 relative to TM10, which is likely tied to movement of the large C terminus, a process somehow triggered by phosphorylation of the regulatory domain in the N terminus.     

G117C MelB, a mutant melibiose permease with a changed conformational equilibrium

Replacement of the glycine at position 117 by a cysteine in the melibiose permease creates an interesting phenotype: while the mutant transporter shows still transport activity comparable to the wild type its pre steady-state kinetic properties are drastically altered. The transient charge displacements after substrate concentration jumps are strongly reduced and the fluorescence changes disappear. Together with its maintained transport activity this indicates that substrate translocation in G117C melibiose permease is not impaired but that the initial conformation of the mutant transporter differs from that of the wild type permease. A kinetic model for the G117C melibiose permease based on a rapid dynamic equilibrium of the substrate free transporter is proposed. Implications of the kinetic model for the transport mechanism of the wild type permease are discussed.     

Electrogenic Glutamate Transporters in the CNS: Molecular Mechanism,Pre-steady-state Kinetics,and their Impact on Synaptic Signaling

Glutamate is the major excitatory neurotransmitter in the mammalian CNS. The spatiotemporal profile of the glutamate concentration in the synapse is critical for excitatory synaptic signalling. The control of this spatiotemporal concentration profile requires the presence of large numbers of synaptically localized glutamate transporters that remove pre-synaptically released glutamate by uptake into neurons and adjacent glia cells. These glutamate transporters are electrogenic and utilize energy stored in the transmembrane potential and the Na⁺/K⁺-ion concentration gradients to accumulate glutamate in the cell. This review focuses on the kinetic and electrogenic properties of glutamate transporters, as well as on the molecular mechanism of transport. Recent results are discussed that demonstrate the multistep nature of the transporter reaction cycle. Results from pre-steady-state kinetic experiments suggest that at least four of the individual transporter reaction steps are electrogenic, including reactions associated with the glutamate-dependent transporter halfcycle. Furthermore, the kinetic similarities and differences between some of the glutamate transporter subtypes and splice variants are discussed. A molecular mechanism of glutamate transport is presented that accounts for most of the available kinetic data. Finally, we discuss how synaptic glutamate transporters impact on glutamate receptor activity and how transporters may shape excitatory synaptic transmission.     

Early intermediates in the transport cycle of the neuronal excitatory amino acid carrier EAAC1

Electrogenic glutamate transport by the excitatory amino acid carrier 1 (EAAC1) is associated with multiple charge movements across the membrane that take place on time scales ranging from microseconds to milliseconds. The molecular nature of these charge movements is poorly understood at present and, therefore, was studied in this report in detail by using the technique of laser-pulse photolysis of caged glutamate providing a 100-micros time resolution. In the inward transport mode, the deactivation of the transient component of the glutamate-induced coupled transport current exhibits two exponential components. Similar results were obtained when restricting EAAC1 to Na(+) translocation steps by removing potassium, thus, demonstrating (1) that substrate translocation of EAAC1 is coupled to inward movement of positive charge and, therefore, electrogenic; and (2) the existence of at least two distinct intermediates in the Na(+)-binding and glutamate translocation limb of the EAAC1 transport cycle. Together with the determination of the sodium ion concentration and voltage dependence of the two-exponential charge movement and of the steady-state EAAC1 properties, we developed a kinetic model that is based on sequential binding of Na(+) and glutamate to their extracellular binding sites on EAAC1 explaining our results. In this model, at least one Na(+) ion and thereafter glutamate rapidly bind to the transporter initiating a slower, electroneutral structural change that makes EAAC1 competent for further, voltage-dependent binding of additional sodium ion(s). Once the fully loaded EAAC1 complex is formed, it can undergo a much slower, electrogenic translocation reaction to expose the substrate and ion binding sites to the cytoplasm.     

Pre-steady-state currents in neutral amino acid transporters induced by photolysis of a new caged alanine derivative

Na+-Dependent transmembrane transport of small neutral amino acids, such as glutamine and alanine, is mediated, among others, by the neutral amino acid transporters of the solute carrier 1 [SLC1, alanine serine cysteine transporter 1 (ASCT1), and ASCT2] and SLC38 families [sodium-coupled neutral amino acid transporter 1 (SNAT1), SNAT2, and SNAT4]. Many mechanistic aspects of amino acid transport by these systems are not well-understood. Here, we describe a new photolabile alanine derivative based on protection of alanine with the 4-methoxy-7-nitroindolinyl (MNI) caging group, which we use for pre-steady-state kinetic analysis of alanine transport by ASCT2, SNAT1, and SNAT2. MNI-alanine has favorable photochemical properties and is stable in aqueous solution. It is also inert with respect to the transport systems studied. Photolytic release of free alanine results in the generation of significant transient current components in HEK293 cells expressing the ASCT2, SNAT1, and SNAT2 proteins. In ASCT2, these currents show biphasic decay with time constants, tau, in the 1-30 ms time range. They are fully inhibited in the absence of extracellular Na+, demonstrating that Na+ binding to the transporter is necessary for induction of the alanine-mediated current. For SNAT1, these transient currents differ in their time course (tau = 1.6 ms) from previously described pre-steady-state currents generated by applying steps in the membrane potential (tau approximately 4-5 ms), indicating that they are associated with a fast, previously undetected, electrogenic partial reaction in the SNAT1 transport cycle. The implications of these results for the mechanisms of transmembrane transport of alanine are discussed. The new caged alanine derivative will provide a useful tool for future, more detailed studies of neutral amino acid transport.     

Transport of Gabapentin, a γ-Amino Acid Drug, by System L α-Amino Acid Transporters: A Comparative Study in Astrocytes, Synaptosomes, and CHO Cells

Abstract: The system L transporter is generally considered to be one of the major Na⁺-independent carriers for large neutral α-amino acids in mammalian cells. However, we found that cultured astrocytes from rat brain cortex accumulate gabapentin, a γ-amino acid, predominantly by this α-amino acid transport system. Uptake of gabapentin by system L transporter was also examined in synaptosomes and Chinese hamster ovary (CHO) cells. The inhibition pattern displayed by various amino acids on gabapentin uptake in astrocytes and synaptosomes corresponds closely to that observed for the system L transport activity in CHO cells. Gabapentin and leucine have K _m values that equal their K _i values for inhibition of each other, suggesting that leucine and gabapentin compete for the same system L transporter. By contrast, gabapentin exhibited no effect on uptake of GABA, glutamate, and arginine, indicating that these latter three types of brain transporters do not serve for uptake of gabapentin. A comparison of computer modeling analysis of gabapentin and l -leucine structures shows that although the former is a γ-amino acid, it can assume a conformation that can resemble the L-form of a large neutral α-amino acid such as l -leucine. The steady-state kinetic study in astrocytes and CHO cells indicates that the intracellular concentrations of gabapentin are about two to four times higher than that of leucine. The uptake levels of these two substrates are inversely related to their relative exodus rates. The concentrating ability by system L observed in astrocytes is consistent with the substantially high accumulation gradient of gabapentin in the brain tissue as determined by microdialysis.     

Water and urea permeation pathways of the human excitatory amino acid transporter EAAT1

Glutamate transport is coupled to the co-transport of 3 Na(+) and 1 H(+) followed by the counter-transport of 1 K(+). In addition, glutamate and Na(+) binding to glutamate transporters generates an uncoupled anion conductance. The human glial glutamate transporter EAAT1 (excitatory amino acid transporter 1) also allows significant passive and active water transport, which suggests that water permeation through glutamate transporters may play an important role in glial cell homoeostasis. Urea also permeates EAAT1 and has been used to characterize the permeation properties of the transporter. We have previously identified a series of mutations that differentially affect either the glutamate transport process or the substrate-activated channel function of EAAT1. The water and urea permeation properties of wild-type EAAT1 and two mutant transporters were measured to identify which permeation pathway facilitates the movement of these molecules. We demonstrate that there is a significant rate of L-glutamate-stimulated passive and active water transport. Both the passive and active L-glutamate-stimulated water transport is most closely associated with the glutamate transport process. In contrast, L-glutamate-stimulated [(14)C]urea permeation is associated with the anion channel of the transporter. However, there is also likely to be a transporter-specific, but glutamate independent, flux of water via the anion channel.     

A complex relative motion between hairpin loop 2 and transmembrane domain 5 in the glutamate transporter GLT-1

Excitatory amino acid transporter 2, also known as glial glutamate transporter type 1 (GLT-1), plays an important role in maintaining suitable synaptic glutamate concentrations. Reentrant helical hairpin loop (HP) 2, as the extracellular gate, has been shown to participate in the binding of substrate and ions. Several residues in transmembrane domain (TM) 5 have been shown to be involved in the construction of the transport pathway. However, the spatial relationship between HP2 and TM5 during the recycling of glutamate has not yet been clarified. We introduced cysteine residue pairs in HP2 and TM5 of cysteine-less-GLT-1 by using site-directed mutagenesis in order to assess the proximity of HP2 and TM5. A significant decrease in substrate uptake was seen in the I283C/S443C and S287C/S443C mutants when the oxidative cross-linking agent copper(II) (1,10-phenanthroline)₃ (CuPh) was used. The inhibitory effect of CuPh on the transport activity of the S287/S443C mutant was increased after the application of glutamate or potassium. In contrast, an apparent protection of the transport activity of the I283C/S443C mutant was observed after glutamate or potassium addition. The membrane-impermeable sulfhydryl reagent (2-trimethylammonium) methanethiosulfonate (MTSET) was used to detect the aqueous permeability of each single mutant. The aqueous permeability of the I283C mutant was identical to that of the S443C mutant. The sensitivity of I283C and S443C to MTSET was attenuated by glutamate and potassium. All these data indicate that there is a complex relative motion between TM5 and HP2 during the transport cycle.