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

Pre-steady-state Kinetic Analysis of Amino Acid Transporter SLC6A14 Reveals Rapid Turnover Rate and Substrate Translocation

SLC6A14 (solute carrier family 6 member 14) is an amino acid transporter, driven by Na⁺ and Cl⁻ co-transport, whose structure, function, and molecular and kinetic mechanism have not been well characterized. Its broad substrate selectivity, including neutral and cationic amino acids, differentiates it from other SLC6 family members, and its proposed involvement in nutrient transport in several cancers suggest that it could become an important drug target. In the present study, we investigated SLC6A14 function and its kinetic mechanism after expression in human embryonic kidney (HEK293) cells, including substrate specificity and voltage dependence under various ionic conditions. We applied rapid solution exchange, voltage jumps, and laser photolysis of caged alanine, allowing sub-millisecond temporal resolution, to study SLC6A14 steady state and pre-steady state kinetics. The results highlight the broad substrate specificity and suggest that extracellular chloride enhances substrate transport but is not required for transport. As in other SLC6 family members, Na⁺ binding to the substrate-free transporter (or conformational changes associated with it) is electrogenic and is likely rate limiting for transporter turnover. Transient current decaying with a time constant of <1ms is also observed after rapid amino acid application, both in forward transport and homoexchange modes, indicating a slightly electrogenic, but fast and not rate-limiting substrate translocation step. Our results, which are consistent with kinetic modeling, suggest rapid transporter turnover rate and substrate translocation with faster kinetics compared with other SLC6 family members. Together, these results provided novel information on the SLC6A14 transport cycle and mechanism, expanding our understanding of SLC6A14 function.

The high-energy transition state of the glutamate transporter homologue GltPh

Membrane transporters mediate cellular uptake of nutrients, signaling molecules, and drugs. Their overall mechanisms are often well understood, but the structural features setting their rates are mostly unknown. Earlier single-molecule fluorescence imaging of the archaeal model glutamate transporter homologue GltPh from Pyrococcus horikoshii suggested that the slow conformational transition from the outward- to the inward-facing state, when the bound substrate is translocated from the extracellular to the cytoplasmic side of the membrane, is rate limiting to transport. Here, we provide insight into the structure of the high-energy transition state of GltPh that limits the rate of the substrate translocation process. Using bioinformatics, we identified GltPh gain-of-function mutations in the flexible helical hairpin domain HP2 and applied linear free energy relationship analysis to infer that the transition state structurally resembles the inward-facing conformation. Based on these analyses, we propose an approach to search for allosteric modulators for transporters.

Molecular and cellular physiology of sodium-dependent glutamate transporters

Glutamate is the major excitatory transmitter in the vertebrate brain. After its release from presynaptic nerve terminals, it is rapidly taken up by high-affinity sodium-dependent plasma membrane transporters. While both neurons and glial cells express these excitatory amino acid transporters (EAATs), the majority of glutamate uptake is accomplished by astrocytes, which convert synaptically-released glutamate to glutamine or feed it into their own metabolism. Glutamate uptake by astrocytes not only shapes synaptic transmission by regulating the availability of glutamate to postsynaptic neuronal receptors, but also protects neurons from hyper-excitability and subsequent excitotoxic damage. In the present review, we provide an overview of the molecular and cellular characteristics of sodium-dependent glutamate transporters and their associated anion permeation pathways, with a focus on astrocytic glutamate transport. We summarize their functional properties and roles within tripartite synapses under physiological and pathophysiological conditions, exemplifying the intricate interactions and interrelationships between neurons and glial cells in the brain.

Electrogenic Steps Associated with Substrate Binding to the Neuronal Glutamate Transporter EAAC1

Glutamate transporters actively take up glutamate into the cell, driven by the co-transport of sodium ions down their transmembrane concentration gradient. It was proposed that glutamate binds to its binding site and is subsequently transported across the membrane in the negatively charged form. With the glutamate binding site being located partially within the membrane domain, the possibility has to be considered that glutamate binding is dependent on the transmembrane potential and, thus, is electrogenic. Experiments presented in this report test this possibility. Rapid application of glutamate to the wild-type glutamate transporter subtype EAAC1 (excitatory amino acid carrier 1) through photo-release from caged glutamate generated a transient inward current, as expected for the electrogenic inward movement of co-transported Na(+) In contrast, glutamate application to a transporter with the mutation A334E induced transient outward current, consistent with movement of negatively charged glutamate into its binding site within the dielectric of the membrane. These results are in agreement with electrostatic calculations, predicting a valence for glutamate binding of -0.27. Control experiments further validate and rule out other possible explanations for the transient outward current. Electrogenic glutamate binding can be isolated in the mutant glutamate transporter because reactions, such as glutamate translocation and/or Na(+) binding to the glutamate-bound state, are inhibited by the A334E substitution. Electrogenic glutamate binding has to be considered together with other voltage-dependent partial reactions to cooperatively determine the voltage dependence of steady-state glutamate uptake and glutamate buffering at the synapse.

Allosteric Mechanisms of Molecular Machines at the Membrane: Transport by Sodium-Coupled Symporters

Solute transport across cell membranes is ubiquitous in biology as an essential physiological process. Secondary active transporters couple the unfavorable process of solute transport against its concentration gradient to the energetically favorable transport of one or several ions. The study of such transporters over several decades indicates that their function involves complex allosteric mechanisms that are progressively being revealed in atomistic detail. We focus on two well-characterized sodium-coupled symporters: the bacterial amino acid transporter LeuT, which is the prototype for the "gated pore" mechanism in the mammalian synaptic monoamine transporters, and the archaeal GltPh, which is the prototype for the "elevator" mechanism in the mammalian excitatory amino acid transporters. We present the evidence for the role of allostery in the context of a quantitative formalism that can reconcile biochemical and biophysical data and thereby connects directly to recent insights into the molecular structure and dynamics of these proteins. We demonstrate that, while the structures and mechanisms of these transporters are very different, the available data suggest a common role of specific models of allostery in their functions. We argue that such allosteric mechanisms appear essential not only for sodium-coupled symport in general but also for the function of other types of molecular machines in the membrane.

Molecular dynamics simulations elucidate the mechanism of proton transport in the glutamate transporter EAAT3

The uptake of glutamate in nerve synapses is carried out by the excitatory amino acid transporters (EAATs), involving the cotransport of a proton and three Na(+) ions and the countertransport of a K(+) ion. In this study, we use an EAAT3 homology model to calculate the pKa of several titratable residues around the glutamate binding site to locate the proton carrier site involved in the translocation of the substrate. After identifying E374 as the main candidate for carrying the proton, we calculate the protonation state of this residue in different conformations of EAAT3 and with different ligands bound. We find that E374 is protonated in the fully bound state, but removing the Na2 ion and the substrate reduces the pKa of this residue and favors the release of the proton to solution. Removing the remaining Na(+) ions again favors the protonation of E374 in both the outward- and inward-facing states, hence the proton is not released in the empty transporter. By calculating the pKa of E374 with a K(+) ion bound in three possible sites, we show that binding of the K(+) ion is necessary for the release of the proton in the inward-facing state. This suggests a mechanism in which a K(+) ion replaces one of the ligands bound to the transporter, which may explain the faster transport rates of the EAATs compared to its archaeal homologs.

SLC1 glutamate transporters

The plasma membrane transporters for the neurotransmitter glutamate belong to the solute carrier 1 family. They are secondary active transporters, taking up glutamate into the cell against a substantial concentration gradient. The driving force for concentrative uptake is provided by the cotransport of Na(+) ions and the countertransport of one K(+) in a step independent of the glutamate translocation step. Due to eletrogenicity of transport, the transmembrane potential can also act as a driving force. Glutamate transporters are expressed in many tissues, but are of particular importance in the brain, where they contribute to the termination of excitatory neurotransmission. Glutamate transporters can also run in reverse, resulting in glutamate release from cells. Due to these important physiological functions, glutamate transporter expression and, therefore, the transport rate, are tightly regulated. This review summarizes recent literature on the functional and biophysical properties, structure-function relationships, regulation, physiological significance, and pharmacology of glutamate transporters. Particular emphasis is on the insight from rapid kinetic and electrophysiological studies, transcriptional regulation of transporter expression, and reverse transport and its importance for pathophysiological glutamate release under ischemic conditions.

Mechanism of transport modulation by an extracellular loop in an archaeal excitatory amino acid transporter (EAAT) homolog

Secondary transporters in the excitatory amino acid transporter family terminate glutamatergic synaptic transmission by catalyzing Na(+)-dependent removal of glutamate from the synaptic cleft. Recent structural studies of the aspartate-specific archaeal homolog, Glt(Ph), suggest that transport is achieved by a rigid body, piston-like movement of the transport domain, which houses the substrate-binding site, between the extracellular and cytoplasmic sides of the membrane. This transport domain is connected to an immobile scaffold by three loops, one of which, the 3-4 loop (3L4), undergoes substrate-sensitive conformational change. Proteolytic cleavage of the 3L4 was found to abolish transport activity indicating an essential function for this loop in the transport mechanism. Here, we demonstrate that despite the presence of fully cleaved 3L4, Glt(Ph) is still able to sample conformations relevant for transport. Optimized reconstitution conditions reveal that fully cleaved Glt(Ph) retains some transport activity. Analysis of the kinetics and temperature dependence of transport accompanied by direct measurements of substrate binding reveal that this decreased transport activity is not due to alteration of the substrate binding characteristics but is caused by the significantly reduced turnover rate. By measuring solute counterflow activity and cross-link formation rates, we demonstrate that cleaving 3L4 severely and specifically compromises one or more steps contributing to the movement of the substrate-loaded transport domain between the outward- and inward-facing conformational states, sparing the equivalent step(s) during the movement of the empty transport domain. These results reveal a hitherto unknown role for the 3L4 in modulating an essential step in the transport process.

Induced fit substrate binding to an archeal glutamate transporter homologue

Excitatory amino acid transporters (EAATs) are a class of glutamate transporters that terminate glutamatergic synaptic transmission in the mammalian CNS. GltPh, an archeal EAAT homolog from Pyrococcus horikoshii, is currently the only member with a known 3D structure. Here, we studied the kinetics of substrate binding of a single tryptophan mutant (L130W) GltPh in detergent micelles. At low millimolar [Na(+)], the addition of L-aspartate resulted in complex time courses of W130 fluorescence changes over tens of seconds. With increasing [Na(+)], the kinetics were dominated by a fast component [k(obs,fast); K(D) (Na(+)) = 22 ± 3 mM, n(Hill )= 1.7 ± 0.3] with values of k(obs,fast) rising in a saturable manner to ≈ 500 s(-1) (at 6 °C) with increasing [L-aspartate]. The binding kinetics of L-aspartate differed from the binding kinetics of two alternative substrates: L-cysteine sulfinic acid and d-aspartate. L-cysteine sulfinic acid bound with higher affinity than L-aspartate but involved lower saturating rates, whereas the saturating rates after D-aspartate binding were higher. Thus, after the association of two Na(+) to the empty transporter, GltPh binds amino acids by induced fit. Cross-linking and proteolysis experiments suggest that the induced fit results from the closure of helical hairpin 2. This conformational change is faster for GltPh than for most mammalian homologues, whereas the amino acid association rates are similar. Our data reveal the importance of induced fit for substrate selection in EAATs and illustrate how high-affinity binding and the efficient transport of glutamate can be accomplished simultaneously by this class of transporters.

Voltage-dependent processes in the electroneutral amino acid exchanger ASCT2

Neutral amino acid exchange by the alanine serine cysteine transporter (ASCT)2 was reported to be electroneutral and coupled to the cotransport of one Na⁺ ion. The cotransported sodium ion carries positive charge. Therefore, it is possible that amino acid exchange is voltage dependent. However, little information is available on the electrical properties of the ASCT2 amino acid transport process. Here, we have used a combination of experimental and computational approaches to determine the details of the amino acid exchange mechanism of ASCT2. The [Na⁺] dependence of ASCT2-associated currents indicates that the Na⁺/amino acid stoichiometry is at least 2:1, with at least one sodium ion binding to the amino acid–free apo form of the transporter. When the substrate and two Na⁺ ions are bound, the valence of the transport domain is +0.81. Consistently, voltage steps applied to ASCT2 in the fully loaded configuration elicit transient currents that decay on a millisecond time scale. Alanine concentration jumps at the extracellular side of the membrane are followed by inwardly directed transient currents, indicative of translocation of net positive charge during exchange. Molecular dynamics simulations are consistent with these results and point to a sequential binding process in which one or two modulatory Na⁺ ions bind with high affinity to the empty transporter, followed by binding of the amino acid substrate and the subsequent binding of a final Na⁺ ion. Overall, our results are consistent with voltage-dependent amino acid exchange occurring on a millisecond time scale, the kinetics of which we predict with simulations. Despite some differences, transport mechanism and interaction with Na⁺ appear to be highly conserved between ASCT2 and the other members of the solute carrier 1 family, which transport acidic amino acids.

Electrophysiological characterization of membrane transport proteins

Active transport in biological membranes has been traditionally studied using a variety of biochemical and biophysical techniques, including electrophysiology. This review focuses on aspects of electrophysiological methods that make them particularly suited for the investigation of transporter function. Two major approaches to electrical recording of transporter activity are discussed: (a) artificial planar lipid membranes, such as the black lipid membrane and solid supported membrane, which are useful for studies on bacterial transporters and transporters of intracellular compartments, and (b) patch clamp and voltage clamp techniques, which investigate transporters in native cellular membranes. The analytical power of these methods is highlighted by several examples of mechanistic studies of specific membrane proteins, including cytochrome c oxidase, NhaA Na(+)/H(+) exchanger, ClC-7 H(+)/Cl(-) exchanger, glutamate transporters, and neutral amino acid transporters. These examples reveal the wealth of mechanistic information that can be obtained when electrophysiological methods are used in combination with rapid perturbation approaches.

Mechanism of inhibition of the glutamate transporter EAAC1 by the conformationally constrained glutamate analogue (+)-HIP-B

Glutamate transporters play an important role in the regulation of extracellular glutamate concentrations in the mammalian brain and are, thus, promising targets for therapeutics. Despite this importance, the development of pharmacological tools has mainly focused on the synthesis of competitive inhibitors, which are amino acid analogues that bind to the substrate binding site. In this report, we describe the characterization of the mechanism of glutamate transporter inhibition by a constrained, cyclic glutamate analogue, (+)-3-hydroxy-4,5,6,6a-tetrahydro-3aH-pyrrolo[3,4-d]isoxazole-6-carboxylic acid [(+)-(3aS,6S,6aS)-HIP-B]. Our results show that (+)-HIP-B is a nontransportable amino acid that inhibits glutamate transporter function in a mixed mechanism. Although (+)-HIP-B inhibits the glutamate-associated anion conductance, it has no effect on the leak anion conductance, in contrast to competitive inhibitors. Furthermore, (+)-HIP-B is unable to alleviate the effect of the competitive inhibitor dl-threo-β-benzyloxyaspartic acid (TBOA), which binds to the substrate binding site. (+)-HIP-B is more potent in inhibiting forward transport compared to reverse transport. In a mutant transporter, which is activated by glutamine, but not glutamate, (+)-HIP-B still acts as an inhibitor, although this mutant transporter is insensitive to TBOA. Finally, we analyzed the effect of (+)-HIP-B on the pre-steady-state kinetics of the glutamate transporter. The results can be explained with a mixed mechanism at a site that may be distinct from the substrate binding site, with a preference for the inward-facing configuration of the transporter and slow inhibitor binding. (+)-HIP-B may represent a new paradigm of glutamate transporter inhibition that is based on targeting of a regulatory site.

Charge compensation mechanism of a Na+-coupled, secondary active glutamate transporter

Forward glutamate transport by the excitatory amino acid carrier EAAC1 is coupled to the inward movement of three Na(+) and one proton and the subsequent outward movement of one K(+) in a separate step. Based on indirect evidence, it was speculated that the cation binding sites bear a negative charge. However, little is known about the electrostatics of the transport process. Valences calculated using the Poisson-Boltzmann equation indicate that negative charge is transferred across the membrane when only one cation is bound. Consistently, transient currents were observed in response to voltage jumps when K(+) was the only cation on both sides of the membrane. Furthermore, rapid extracellular K(+) application to EAAC1 under single turnover conditions (K(+) inside) resulted in outward transient current. We propose a charge compensation mechanism, in which the C-terminal transport domain bears an overall negative charge of -1.23. Charge compensation, together with distribution of charge movement over many steps in the transport cycle, as well as defocusing of the membrane electric field, may be combined strategies used by Na(+)-coupled transporters to avoid prohibitive activation barriers for charge translocation.

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.

Identification of the third Na+ site and the sequence of extracellular binding events in the glutamate transporter

The transport cycle in the glutamate transporter (GlT) is catalyzed by the cotransport of three Na(+) ions. However, the positions of only two of these ions (Na1 and Na2 sites) along with the substrate have been captured in the crystal structures reported for both the outward-facing and the inward-facing states of Glt(ph). Characterizing the third ion binding site (Na3) is necessary for structure-function studies attempting to investigate the mechanism of transport in GlTs at an atomic level, particularly for the determination of the sequence of the binding events during the transport cycle. In this study, we report a series of molecular dynamics simulations performed on various bound states of Glt(ph) (the apo state, as well as in the presence of Na(+), the substrate, or both), which have been used to identify a putative Na3 site. The calculated trajectories have been used to determine the water accessibility of potential ion-binding residues in the protein, as a prerequisite for their ion binding. Combined with conformational analysis of the key regions in the protein in different bound states and several additional independent simulations in which a Na(+) ion was randomly introduced to the interior of the transporter, we have been able to characterize a putative Na3 site and propose a plausible binding sequence for the substrate and the three Na(+) ions to the transporter during the extracellular half of the transport cycle. The proposed Na3 site is formed by a set of highly conserved residues, namely, Asp(312), Thr(92), and Asn(310), along with a water molecule. Simulation of a fully bound state, including the substrate and the three Na(+) ions, reveals a stable structure--showing closer agreement to the crystal structure when compared to previous models lacking an ion in the putative Na3 site. The proposed sequence of binding events is in agreement with recent experimental models suggesting that two Na(+) ions bind before the substrate, and one after that. Our results, however, provide additional information about the sites involved in these binding events.

Hetero-oligomerization of neuronal glutamate transporters

Excitatory amino acid transporters (EAATs) mediate the uptake of glutamate into neuronal and glial cells of the mammalian central nervous system. Two transporters expressed primarily in glia, EAAT1 and EAAT2, are crucial for glutamate homeostasis in the adult mammalian brain. Three neuronal transporters (EAAT3, EAAT4, and EAAT5) appear to have additional functions in regulating and processing cellular excitability. EAATs are assembled as trimers, and the existence of multiple isoforms raises the question of whether certain isoforms can form hetero-oligomers. Co-expression and pulldown experiments of various glutamate transporters showed that EAAT3 and EAAT4, but neither EAAT1 and EAAT2, nor EAAT2 and EAAT3 are capable of co-assembling into heterotrimers. To study the functional consequences of hetero-oligomerization, we co-expressed EAAT3 and the serine-dependent mutant R501C EAAT4 in HEK293 cells and Xenopus laevis oocytes and studied glutamate/serine transport and anion conduction using electrophysiological methods. Individual subunits transport glutamate independently of each other. Apparent substrate affinities are not affected by hetero-oligomerization. However, polarized localization in Madin-Darby canine kidney cells was different for homo- and hetero-oligomers. EAAT3 inserts exclusively into apical membranes of Madin-Darby canine kidney cells when expressed alone. Co-expression with EAAT4 results in additional appearance of basolateral EAAT3. Our results demonstrate the existence of heterotrimeric glutamate transporters and provide novel information about the physiological impact of EAAT oligomerization.

Capturing Functional Motions of Membrane Channels and Transporters with Molecular Dynamics Simulation

Conformational changes of proteins are involved in all aspects of protein function in biology. Almost all classes of proteins respond to changes in their environment, ligand binding, and interaction with other proteins and regulatory agents through undergoing conformational changes of various degrees and magnitudes. Membrane channels and transporters are the major classes of proteins that are responsible for mediating efficient and selective transport of materials across the cellular membrane. Similar to other proteins, they take advantage of conformational changes to make transitions between various functional states. In channels, large-scale conformational changes are mostly involved in the process of "gating", i.e., opening and closing of the pore of the channel protein in response to various signals. In transporters, conformational changes constitute various steps of the conduction process, and, thus, are more closely integrated in the transport process. Owing to significant progress in developing highly efficient parallel algorithms in molecular dynamics simulations and increased computational resources, and combined with the availability of high-resolution, atomic structures of membrane proteins, we are in an unprecedented position to use computer simulation and modeling methodologies to investigate the mechanism of function of membrane channels and transporters. While the entire transport cycle is still out of reach of current methodologies, many steps involved in the function of transport proteins have been characterized with molecular dynamics simulations. Here, we present several examples of such studies from our laboratory, in which functionally relevant conformational changes of membrane channels and transporters have been characterized using extended simulations.

New views of glutamate transporter structure and function: advances and challenges

Neuronal and glial glutamate transporters limit the action of excitatory amino acids after their release during synaptic transmission. Recent structural and functional investigations have revealed much about the transport and conducting mechanisms of members of the sodium-coupled symporter family responsible for glutamate clearance in the nervous system. In this review we summarize emerging views on the general structure, binding sites for substrates and coupled ions, and transport mechanisms of mammalian glutamate transporters, integrating results from a large body of work on carrier structure-function relationships with several crystal structures obtained for the archaeal ortholog, Glt(Ph).

Mechanism of cation binding to the glutamate transporter EAAC1 probed with mutation of the conserved amino acid residue Thr101

The glutamate transporter excitatory amino acid carrier 1 (EAAC1) catalyzes the co-transport of three Na(+) ions, one H(+) ion, and one glutamate molecule into the cell, in exchange for one K(+) ion. Na(+) binding to the glutamate-free form of the transporter generates a high affinity binding site for glutamate and is thus required for transport. Moreover, sodium binding to the transporters induces a basal anion conductance, which is further activated by glutamate. Here, we used the [Na(+)] dependence of this conductance as a read-out of Na(+) binding to the substrate-free transporter to study the impact of a highly conserved amino acid residue, Thr(101), in transmembrane domain 3. The apparent affinity of substrate-free EAAC1 for Na(+) was dramatically decreased by the T101A but not by the T101S mutation. Interestingly, in further contrast to EAAC1(WT), in the T101A mutant this [Na(+)] dependence was biphasic. This behavior can be explained by assuming that the binding of two Na(+) ions prior to glutamate binding is required to generate a high affinity substrate binding site. In contrast to the dramatic effect of the T101A mutation on Na(+) binding, other properties of the transporter, such as its ability to transport glutamate, were impaired but not eliminated. Our results are consistent with the existence of a cation binding site deeply buried in the membrane and involving interactions with the side chain oxygens of Thr(101) and Asp(367). A theoretical valence screening approach confirms that the predicted site of cation interaction has the potential to be a novel, so far undetected sodium binding site.

Inward-facing conformation of glutamate transporters as revealed by their inverted-topology structural repeats

Glutamate transporters regulate synaptic concentrations of this neurotransmitter by coupling its flux to that of sodium and other cations. Available crystal structures of an archeal homologue of these transporters, GltPh, resemble an extracellular-facing state, in which the bound substrate is occluded only by a small helical hairpin segment called HP2. However, a pathway to the cytoplasmic side of the membrane is not clearly apparent. We previously modeled an alternate state of a transporter from the neurotransmitter:sodium symporter family, which has an entirely different fold, solely on the presence of inverted-topology structural repeats. In GltPh, we identified two distinct sets of inverted-topology repeats and used these repeats to model an inward-facing conformation of the protein. To test this model, we introduced pairs of cysteines into the neuronal glutamate transporter EAAC1, at positions that are >27 A apart in the crystal structures of GltPh, but approximately = 10 A apart in the inward-facing model. Transport by these mutants was activated by pretreatment with the reducing agent dithithreitol. Subsequent treatment with the oxidizing agent copper(II)(1,10-phenantroline)(3) abolished this activation. The inhibition of transport was potentiated under conditions thought to promote the inward-facing conformation of the transporter. By contrast, the inhibition was reduced in the presence of the nontransportable substrate analogue D,L-threo-beta-benzyloxyaspartate, which favors the outward-facing conformation. Other conformation-sensitive accessibility measurements are also accommodated by our inward-facing model. These results suggest that the inclusion of inverted-topology repeats in transporters may provide a general solution to the requirement for two symmetry-related states in a single protein.

Molecular simulations elucidate the substrate translocation pathway in a glutamate transporter

Glutamate transporters are membrane proteins found in neurons and glial cells, which play a critical role in regulating cell signaling by clearing glutamate released from synapses. Although extensive biochemical and structural studies have shed light onto different aspects of glutamate transport, the time-resolved molecular mechanism of substrate (glutamate or aspartate) translocation, that is, the sequence of events occurring at the atomic level after substrate binding and before its release intracellularly remain to be elucidated. We identify an energetically preferred permeation pathway of approximately 23 A between the helix HP1b on the hairpin HP1 and the transmembrane helices TM7 and TM8, using the high resolution structure of the transporter from Pyrococcus horikoshii (Glt(Ph)) in steered molecular dynamics simulations. Detailed potential of mean force calculations along the putative pathway reveal 2 energy barriers encountered by the substrate (aspartate) before it reaches the exit. The first barrier is surmounted with the assistance of 2 conserved residues (S278 and N401) and a sodium ion (Na2); and the second, by the electrostatic interactions with D405 and another sodium ion (Na1). The observed critical interactions and mediating role of conserved residues in the core domain, the accompanying conformational changes (in both substrate and transporter) that relieve local strains, and the unique coupling of aspartate transport to Na(+) dislocation provide insights into methods for modulating substrate transport.

Glutamate forward and reverse transport: from molecular mechanism to transporter-mediated release after ischemia

Glutamate transporters remove the excitatory neurotransmitter glutamate from the extracellular space after neurotransmission is complete, by taking glutamate up into neurons and glia cells. As thermodynamic machines, these transporters can also run in reverse, releasing glutamate into the extracellular space. Because glutamate is excitotoxic, this transporter-mediated release is detrimental to the health of neurons and axons, and it, thus, contributes to the brain damage that typically follows a stroke. This review highlights current ideas about the molecular mechanisms underlying glutamate uptake and glutamate reverse transport. It also discusses the implications of transporter-mediated glutamate release for cellular function under physiological and patho-physiological conditions.

Dynamics of the extracellular gate and ion-substrate coupling in the glutamate transporter

Glutamate transporters (GluTs) are the primary regulators of extracellular concentration of the neurotransmitter glutamate in the central nervous system. In this study, we have investigated the dynamics and coupling of the substrate and Na(+) binding sites, and the mechanism of cotransport of Na(+) ions, using molecular dynamics simulations of a membrane-embedded model of GluT in its apo (empty form) and various Na(+)- and/or substrate-bound states. The results shed light on the mechanism of the extracellular gate and on the sequence of binding of the substrate and Na(+) ions to GluT during the transport cycle. The results suggest that the helical hairpin HP2 plays the key role of the extracellular gate for the substrate binding site, and that the opening and closure of the gate is controlled by substrate binding. GluT adopts an open conformation in the absence of the substrate exposing the binding sites of the substrate and Na(+) ions to the extracellular solution. Based on the calculated trajectories, we propose that Na1 is the first element to bind GluT, as it is found to be important for the completion of the substrate binding site. The subsequent binding of the substrate, in turn, is shown to result in an almost complete closure of the extracellular gate and the formation of the Na2 binding site. Finally, binding of Na2 locks the extracellular gate and completes the formation of the occluded state of GluT.