PepT1 and PepT2 are major facilitator superfamily (MFS) transporters that utilize a proton gradient to drive the uptake of di‐ and tri‐peptides in the small intestine and kidney, respectively. They are the major routes by which we absorb dietary nitrogen and many orally administered drugs. Here, we present the crystal structure of PepTSo, a functionally similar prokaryotic homologue of the mammalian peptide transporters from Shewanella oneidensis. This structure, refined using data up to 3.6 Å resolution, reveals a ligand‐bound occluded state for the MFS and provides new insights into a general transport mechanism. We have located the peptide‐binding site in a central hydrophilic cavity, which occludes a bound ligand from both sides of the membrane. Residues thought to be involved in proton coupling have also been identified near the extracellular gate of the cavity. Based on these findings and associated kinetic data, we propose that PepTSo represents a sound model system for understanding mammalian peptide transport as catalysed by PepT1 and PepT2.
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The absorption of dietary nitrogen in the form of peptides by plasma membrane transporters belonging to the solute carrier (SLC) 15 family is essential for human health. Evolutionarily, these transporters form part of the widely distributed proton‐dependent oligopeptide transporter (POT) family (TC 2.A.17), also referred to as the peptide transporter or PTR2 family (Paulsen and Skurray, 1994; Steiner et al, 1995), members of which transport peptides, amino acids and nitrate (Huang et al, 1999). They are proton‐driven symporters, and in both eukaryotes and prokaryotes use the inwardly directed proton (H+) electrochemical gradient to drive the uptake of peptides across cell membranes (Ganapathy and Leibach, 1983; Daniel et al, 2006). Human PepT1 (SLC15A1) is found predominantly in the small intestine, whereas PepT2 (SLC15A2) is found in the kidney, the lungs and central nervous system (Daniel and Kottra, 2004). PepT1 and PepT2 are predicted to contain 12 transmembrane (TM) helices with both N‐ and C‐termini facing the cytoplasm, as is typical for major facilitator superfamily (MFS) members (Fei et al, 1994; Covitz et al, 1998). PepT1 is a high‐capacity, low‐affinity transporter and is the main route for dietary peptide uptake, whereas PepT2 operates as a low‐capacity, high‐affinity transporter, thought to mediate more selective transport in the kidney and other tissues (Terada et al, 1997; Doring et al, 2002; Daniel and Kottra, 2004; Biegel et al, 2006). In addition to peptides, the human proteins transport a broad spectrum of orally administered drugs, including the β‐lactam antibiotics (Wenzel et al, 1995; Tamai et al, 1997; Faria et al, 2004), and are under active clinical investigation to improve the pharmacokinetic properties of antivirals such as valacyclovir (Ganapathy et al, 1998) and the vasopressor midodrine (Tsuda et al, 2006).
To study the function of the mammalian transporters, a number of distantly related prokaryotic homologues with similar substrate specificities have been employed as model systems (Hagting et al, 1994; Harder et al, 2008; Ernst et al, 2009). Here, we report the crystal structure of a peptide transporter from the bacterium Shewanella oneidensis, PepTSo, which shows a high degree of sequence conservation within the TM region (∼30% identity) to the mammalian PepT1 and PepT2 proteins. All previously identified residues proposed to be functionally important in the mammalian transporters are conserved, including a critical histidine residue (Uchiyama et al, 2003) (His57 in human PepT1) (Supplementary Figure S1). The structure of PepTSo reveals important information concerning the spatial arrangement of residues involved in peptide and drug transport as catalysed by mammalian peptide transporters. In addition, it represents a ligand‐bound occluded conformation for an MFS symporter, providing fresh insight into the alternating access model of membrane transport.
Structure of PepTSo
PepTSo contains 14 TM helices (Figure 1A), of which helices H1–H12 adopt the overall fold observed previously for the MFS transporters LacY, GlpT and EmrD (Figure 1B) (Abramson et al, 2003; Huang et al, 2003; Yin et al, 2006). The arrangement of the helices is also consistent with the EM projection structure of a previously studied POT protein, DtpD from Escherichia coli (Casagrande et al, 2009). Like previous MFS transporter structures, the N‐ and C‐terminal six‐helix bundles, formed by helices H1–H6 and H7–H12, come together to form a ‘V’‐shaped transporter, related by a pseudo two‐fold symmetry axis running perpendicular to the membrane plane. PepTSo has two additional TM helices, HA and HB, which are inserted into the cytoplasmic loop connecting the N‐ and C‐terminal bundles. These form a hairpin‐like structure in the membrane that packs against the periphery of the protein (Figure 1C). Their role is currently unclear. The apparent absence of these helices in the fungal, plant and metazoan protein sequences, however, suggests they do not contribute to any conserved transport mechanism. The position of PepTSo within the membrane has been examined using coarse‐grained lipid bilayer self‐assembly simulations (Scott et al, 2008). These demonstrate that PepTSo, including the hairpin helices HA and HB, reproducibly inserts into a modelled bilayer (Supplementary Figure S2).
The apparent KM for transport of the hydrolysis resistant di‐peptide glycylsarcosine is 1.5±0.15 mM, similar to the value reported for human PepT1 of 1.1±0.1 mM (Brandsch et al, 1994) (Figure 2A). Uptake of a fluorescent di‐peptide, β‐Ala‐Lys‐Ne‐7‐amino‐4‐methylcoumarin‐3‐acetic acid (β‐Ala‐Lys‐(AMCA)) in cells overexpressing the PepTSo gene was reduced upon addition of either di‐ or tri‐alanine peptides to the media (Supplementary Figure S3). Addition of l‐alanine or the larger tetra‐alanine peptide, however, had little effect, suggesting a similar preference for di‐ and tri‐peptides as reported for the mammalian transporters (Fei et al, 1994). Uptake was also abolished by the proton ionophore carbonyl cyanide p‐chlorophenylhydrazone, consistent with a dependence on the proton electrochemical gradient (ΔμH+) to drive transport. The crystal structure was solved by multiple isomorphous replacement with anomalous scattering using mercury derivative crystals and seleno‐l‐methionine incorporated protein (Table I and Supplementary Tables I and II). Assignment of the amino‐acid sequence to the density map was aided through identification of the 22 selenium and three mercury sites present in the molecule (Supplementary Figure S4). The model was built and refined using data with anisotropic truncation of the observed structure factors (Strong et al, 2006) to 4.3 Å along the A and B axes, while keeping the C axis at 3.6 Å (Supplementary Figure S5). The final model was refined to an Rfactor of 27.8% and a corresponding Rfree of 29.6% (Table I). There are three PepTSo molecules in the crystallographic asymmetric unit and their structures are identical in the context of this analysis.
In the structure, we observe a central cavity and a smaller extracellular cavity, both of which are hydrophilic (Figure 1B). The central cavity is situated within the centre of the membrane and closed to the extracellular space by a gate made of helices H1, H2, H7 and H8, which pack closely together (Figures 1C and 2C). Previous secondary active transporter structures have all revealed a ligand‐binding site located within the centre of the membrane, essentially equidistant between extracellular and intracellular sides (reviewed in Boudker and Verdon, 2010). Indeed, the residues extending into the central cavity in PepTSo are all known to affect peptide binding and/or transport in the mammalian proteins (Terada et al, 1996, 2004; Fei et al, 1997; Bolger et al, 1998; Yeung et al, 1998; Chen et al, 2000; Uchiyama et al, 2003; Hauser et al, 2005; Pieri et al, 2009; Xu et al, 2009). This cavity is therefore an obvious location for the peptide‐binding site, as we discuss below. As further confirmation, we also observe clear electron density within this cavity for a bound ligand. The apparent Km for the substrate peptide glycylsarcosine is low, 1.5 mM; therefore, this density is unlikely to represent a co‐purified natural peptide. The density is more likely to represent a non‐natural ligand or a high‐affinity inhibitor acquired from either the purification or the crystallization conditions. The position of this density corresponds to the same location of the bound sugar analogue β‐d‐galactopyranosyl‐thio‐β‐d‐galactopyranoside observed in the binding site of LacY (Abramson et al, 2003) (Supplementary Figure S6). Access to the cytoplasm from this cavity is restricted by an intracellular gate formed by side‐chain interactions between two‐helix hairpins, helices H4 and H5 on the N‐terminal side, and H10 and H11 on the opposing C‐terminal side (Figure 2D). The interaction between these helices occurs through residues that are conserved across the vertebrate peptide transporters (Figure 1A; Supplementary Figure S1). The most prominent of these interactions involves Leu427(603) on helix H10 packing against Tyr154(167) and Phe150(163) on helix H4, both of which form part of the highly conserved POT family PTR2_2 motif (FYxxINxG), suggesting a possible role in regulating the exit of peptides from the central cavity. Numbers in brackets correspond to the equivalent residues in human PepT1. Indeed, several point mutations within the PTR2_2 motif have been found to inactivate or greatly impair transport (Hauser et al, 2005). Considering the position of a bound ligand within the central cavity and its confinement through the closure of both extracellular and intracellular gates (Figure 3A and B), we have described the present state of PepTSo as substrate occluded, in analogy with the LeuT superfamily transporters (Krishnamurthy et al, 2009).
Comparing this conformation with previous MFS transporter structures has highlighted a potentially important structural feature of transport within the MFS. The various LacY structures are all in inward‐facing open conformations (Abramson et al, 2003). The EmrD structure on the other hand likely corresponds to an occluded state, although no evidence of bound ligand could be observed in the electron density maps (Yin et al, 2006). Using a secondary structure matching algorithm (Krissinel and Henrick, 2004) to overlay these evolutionarily distinct proteins, it is clear that the structure of PepTSo is more similar to that of EmrD than to LacY, with an average distance of 2.4 Å for 155 equivalent Cα atoms (Supplementary Figure S7). This observation supports the conclusion that PepTSo also represents the occluded conformation for the POT family.
To further understand the differences between PepTSo and LacY, which represent two different conformational states for MFS transporters, we also compared their structures by calculating the change in position between Cα atoms of related helical segments within the N‐ and C‐terminal six‐helix bundles, respectively (see Supplementary data). The main difference was clearly identified as residing within the C‐terminal domain, the average distances between atoms that make up the N‐ and C‐terminal helix bundles being 2.8 and 4.4 Å, respectively (Supplementary Table III). Further insight was drawn from comparing Cα displacements of individual helices within the C‐terminal domain. In this case, helix H7 of PepTSo and LacY showed the largest average Cα displacement between the two structures of 5.7 Å. The C‐terminal six‐helix bundle of MFS transporters is made up of inverted repeats constructed from helices H7–H9 and H10–H12. Structurally, however, they also form two sub‐bundles of helices consisting of H7, H11 and H12 (sub‐bundle C1) and H8, H9 and H10 (sub‐bundle C2) (Figure 3C). When the N‐terminal domains of PepTSo and LacY are superimposed, the largest deviation is observed in sub‐bundle C1, which is displaced by an approximate 11° rotation (Supplementary Figure S8). These helices seem to be the ones mainly responsible for the asymmetry between the N‐ and C‐terminal helix bundles between the occluded conformation of PepTSo and inward open conformation of LacY. These observations suggest that a large conformational change takes place predominantly within the C‐terminal domain of MFS transporters during the transition from ligand‐bound occluded to inward open state.
The observed extracellular cavity is also located at the interface between the N‐ and C‐terminal domains and is roughly cone shaped, with the apex at the bottom near the central cavity, opening outward (Figures 1B and 2C). The overall dimensions of the cavity are ∼16 × 8 × 8 Å. Atomistic molecular dynamics (MD) simulations reproducibly show that both this extracellular cavity and the central cavity are fully solvated and not blocked by lipid molecules in the present conformation (Supplementary Figure S9). The EmrD structure exhibits a similar cavity (Supplementary Figure S7), which differs mainly in that its surface is composed primarily of hydrophobic residues. This observation supports the possibility that this cavity represents the vestiges of either an entrance (for PepTSo) or an exit (for EmrD) pathway for substrates, these being hydrophilic peptides for PepTSo and hydrophobic compounds for EmrD, when the central cavity is open towards the extracellular side.
The peptide‐binding site
As previously noted, many of the residues conserved between PepTSo and the mammalian peptide transporters cluster around the central hydrophilic cavity, with approximate dimensions of 13 × 12 × 11 Å. These dimensions are sufficient to accommodate both di‐ and tri‐peptides, although would be sterically restrictive for larger tetra‐peptide ligands. This may explain the competition we observe in the in vivo transport assay between peptides of this size and the β‐Ala‐Lys‐(AMCA) (Supplementary Figure S3). The dimensions of the cavity could also explain the lack of affinity for single amino acids, as these would presumably be incapable of interacting sufficiently with both the N‐ and C‐terminal domains of the transporter. Sitting within the centre of the cavity we observe strong (>4σ) electron density for an unidentified ligand (Figure 4; Supplementary Figure S10) of approximately the same dimensions as a di‐peptide. In the figure, a Cα model of a di‐alanine peptide has been placed into the density as a reference to evaluate the size of the cavity, although no peptide was modelled during refinement.
The binding site is formed by residues from helices H1, H2, H4 and H5 from the N‐terminal six‐helix bundle and from helices H7, H8, H10 and H11 from the C‐terminal bundle. On the N‐terminal side of the binding site, three conserved positively charged residues, Arg25(27), Arg32(34) and Lys127(140) extend into the cavity. It has been reported that mutation of Arg25(27) in human PepT2 to a histidine completely inactivates transport (Terada et al, 2004). Two conserved tyrosine residues, Tyr29(31) and Tyr68(64), are positioned close to this positively charged cluster. On the C‐terminal side of the binding site, at a distance of ∼13 Å from Lys127(140), are two further strictly conserved residues, Glu419(595) and Ser423(599), located in close proximity to Tyr154(167). Various mutants of Glu419(595) in PepT1 have been reported to drastically reduce transport activity, except where mutation was to an aspartic acid (Xu et al, 2009), indicating the importance of a negatively charged residue at this position. The arrangement of opposite charges within the binding site may have an important role in the recognition and orientation of peptides through the creation of a dipole moment. The presence of several possible hydrogen‐bond donors and acceptors could be advantageous in adapting to peptides of various lengths, sequences and charges. For example, the tyrosine residues described above could have important roles in forming hydrogen bonds and for providing a hydrophobic environment for side chains, as observed in many antigen‐recognition sites (Fellouse et al, 2004).
Most of the other residues in the binding site are conserved hydrophobic residues, including Ile157(170), Trp312(294), Phe315(297) and Trp446(622). These residues are likely to provide a suitable environment for peptide side chains that in general are more hydrophobic than the peptide backbone. This idea is supported by the fact that mutation of Trp312(294) of PepT1 to alanine reduces substrate uptake in HEK293 cells (Bolger et al, 1998). The presence of hydrophobic pockets formed by these residues in the peptide‐binding site of PepT1 has also been predicted through biochemical studies (Bailey et al, 2000). The water molecules that were identified by the MD simulation as filling the central cavity may also have an important role in allowing the binding site to accommodate various types of amino‐acid side chain, as shown in the study of OppA, a periplasmic protein that also binds a diverse library of oligopeptides (Tame et al, 1996).
Interestingly, some conserved residues are not located within the central cavity. The PTR2_1 motif, also conserved throughout the POT family (Daniel et al, 2006), spans the cytoplasmic linker connecting helices H2 and H3 (Supplementary Figure S1). Residues within this motif do not make any contribution to the interior of the protein and most likely sit in the interfacial region of the lipid bilayer, a location also suggested by the coarse‐grained MD simulations (Supplementary Figure S2). Glu21(23) and Glu24(26) on helix H1 are also well conserved among the POTs. These residues are not located in the peptide‐binding site but are in close proximity to Arg25(27) and Lys127(140), and may have an important role in positioning these residues.
Implications for proton‐driven peptide symport
Although MFS transporters have been extensively studied using biochemical and biophysical methods, the current lack of additional structural information pertaining to the multiple states has hampered further understanding of the transport mechanism in this large and important transporter family. The PepTSo structure presents a ligand‐bound occluded conformation for an MFS symporter with a clearly identified substrate‐binding site. Its comparison with the inward‐facing LacY structure in this study provides new insight into the transition states of the alternating access mechanism as operating within the MFS. Figure 5 summarizes a possible model for transport, which is further discussed below.
In the present structure, both ends of the central cavity containing residues involved in peptide binding are closed (Figure 5B). For uptake of peptide, the central cavity needs to be connected to the extracellular space, potentially through the extracellular cavity observed in PepTSo (Figure 5A). The central and extracellular cavities are separated by a putative extracellular gate, which is made of helix H7 packed against helix H2 at the interface between the N‐ and C‐terminal helix bundles (Figure 2C). Kaback and colleagues have identified this region in LacY as forming a periplasmic gate, the opening of which is essential for substrate uptake from the extracellular space (Zhou et al, 2008; Nie et al, 2009). Exit of bound peptide to the intracellular side is currently restricted by side‐chain interactions between two helix hairpins formed by helices H4 and H5 and H10 and H11 on the opposing N‐ and C‐terminal helix bundles, respectively (Figure 2D). When we compare the occluded structure of PepTSo with the inward‐facing LacY and occluded EmrD structures, the N‐terminal helix sub‐bundles, including the helix hairpin formed by H4 and H5, maintain similar positions as discussed above (Figure 3C; Supplementary Figure S7). Opening of the intracellular gate, therefore, seems to be controlled by the movement of helix hairpin H10–H11 in the C‐terminal helix bundle. This hairpin would move together with the sub‐bundle C1, composed of helices H7, H11 and H12, which show the largest difference between the LacY and PepTSo structures (Supplementary Figure S8).
Considering the proton–substrate symport mechanism within the peptide transporter family, one of the more interesting residues is His61(57) buried within the H2–H7 helix interface that forms the extracellular gate (Figures 2C and 5B). The region containing His61(57) is completely exposed to the intracellular side in the LacY structures, suggesting a significant conformational change in moving from the occluded to inward‐facing state (Figure 5C). The His61(57) residue has been identified as the primary protonation site in human PepT1 and PepT2 (Fei et al, 1997; Uchiyama et al, 2003). Indeed, a His61(57)Arg mutant of human PepT1 is active only at higher pH, indicating that protonation and deprotonation of this side chain is essential for peptide transport (Fei et al, 1997; Uchiyama et al, 2003). Mutation of this residue in PepTSo to cysteine also inactivates the transporter in an in vivo peptide uptake assay (Figure 2B). In the vicinity of His61(57), there is Asp316(298) that sits at the top of the central cavity. This residue is currently interacting with Arg32(34) in the ligand‐binding site (Figure 2C). Although neither His61(57) nor Asp316(298) is strictly conserved in POTs from bacteria and lower eukaryotes, this region is clearly important in proton binding and/or opening of the extracellular gate in PepTSo and its mammalian homologues. In EmrD and related homologues, a conserved glutamate, Glu227, in helix H7, which is located close to the equivalent position of Asp316(298) in PepTSo, has been suggested as a possible proton‐binding site (Yin et al, 2006) (Supplementary Figure S7). An EmrD homologue, LmrP from Lactococcus lactis, also conserves a carboxylate group (Asp235) in a similar region of the protein, which is suggested to form part of a flexible proton/ligand‐binding site (Bapna et al, 2007; Schaedler and van Veen, 2010) and is responsible in part for conformational changes observed in LmrP upon proton binding (Gbaguidi et al, 2007).
The structural model employed to explain transport within the MFS has to date been a symmetrical rigid body rocking motion between the N‐ and C‐terminal six‐helix bundles (Abramson et al, 2003; Huang et al, 2003). The occluded PepTSo structure, however, indicates that there is a potentially important role sharing arrangement between these bundles. Our structure suggests the N‐terminal helix bundle should be less dynamic, and in the POT family more involved in peptide binding, whereas the C‐terminal helix bundle contains the mobile gates, quite possibly driven by the proton electrochemical gradient. Such a functional division between the two halves of MFS transporters is supported by previous biochemical studies in LacY and other distantly related transporters (Guan and Kaback, 2006; Kasho et al, 2006; Boudker and Verdon, 2010). This mechanism is conceptually similar to the one reported for the benzyl‐hydantoin transporter Mhp1, wherein the central four‐helix bundle provides a stable platform and the ‘hash motif’, made by the other four‐helix bundle, acts as a mobile gate (Shimamura et al, 2010).
To understand the mechanism in full however, it will be essential to determine the PepTSo structure in different conformational states and determine the sites of protonation and peptide binding. A central question still remaining is how the human peptide transporters PepT1 and PepT2 are able to transport not only peptides and peptide analogues such as β‐lactam antibiotics, but also much larger peptide prodrugs, such as valacyclovir and val‐val‐lopinavir (Brandsch, 2009). The structure of PepTSo provides the first structural model with which to further investigate this important aspect of mammalian peptide transporter biochemistry.
Materials and methods
Protein expression and purification
The gene encoding PepTSo (SO_0002, Uniprot identifier Q8EKT7) was amplified from a previously constructed expression plasmid pMPSIL0079A and cloned into the pWaldo‐GFPe plasmid (Drew et al, 2001) for all subsequent overexpression, purification and crystallization procedures (for details see Supplementary data).
Crystals of PepTSo were obtained in 30% PEG 300, 0.1 M MES pH 6.50 and 0.1 M NaCl using the hanging drop vapour diffusion technique at 4°C. For cryoprotection, the crystals were transferred to a solution containing 36–40% PEG 300, 0.1 M MES pH 6.50, 0.1 M NaCl and 0.03% DDM, before being flash vitrified in liquid nitrogen. The crystals always showed strong anisotropic diffraction, with the best crystals diffracting between 3.6 and 3.8 Å in the best direction. Mercury derivatives were prepared in two ways, either before crystallization or through soaking of native crystals. Data sets MMC‐1, HgAc and MMC‐3 were obtained from crystals grown using protein pre‐incubated with mercury compounds, while data set MMC‐2 was obtained through soaking a seleno‐l‐methionine incorporated crystal. Modification of free cysteines and seleno‐l‐methionine incorporation of the protein before crystal growth was carried out as described in Extended experimental procedures. Data were collected on beamlines ID23eh1 and ID29 at the European synchrotron radiation facility and on IO2 and IO3 at the Diamond Light Source Ltd, UK. Data were processed and scaled using the HKL suite of programs (Otwinowski and Minor, 1997). The space group was determined to be P32, with three molecules in the asymmetric unit. Two mercury sites were initially located in each of the three molecules. These were found manually using RSPS (Knight, 2000). The mercury positions were refined and initial phases were calculated using SHARP (de La Fortelle and Bricogne, 1997). The resulting phases were used to locate a third mercury site. Phases from the mercury sites were used to locate the selenium sites in difference Fourier maps and these were added to the nine mercury sites to improve the phase information. Over 30 data sets were collected during the structure determination from >1000 crystals screened at the synchrotron. These data sets were grouped according to isomorphism and anomalous signal strength, as judged by Xtriage (Adams et al, 2002) (Supplementary Tables I and II). Each set of isomorphous data was used to calculate phases in SHARP and the calculated maps were analysed. This process resulted in two sets of non‐isomorphous data that gave good initial maps that showed clear solvent boundaries around the three molecules. Set 1 contained the high‐resolution native and two mercury derivative data sets, MMC‐1 and HgAc. Set 2 contained two mercury derivative data sets, MMC‐2, which was a seleno‐l‐methionine incorporated crystal soaked overnight in 2 mM MMC and MMC‐3. Set 2 also contained a separate seleno‐l‐methionine crystal collected at the anomalous edge for selenium. The three‐fold non‐crystallographic symmetry present in the packing of the crystal was used to improve the phase information. A rough mask was calculated around one of the three molecules using O (Jones and Kjeldgaard, 1997) and the NCS operators calculated and improved using programs from the RAVE (Jones and Kjeldgaard, 1997) package. These were then used in DM (Cowtan, 1994) to average over the three molecules in the asymmetric unit. The two sets of phases were also combined using cross‐crystal averaging in DMMulti (Cowtan, 1994). The resulting maps were then of sufficient quality to see all 14 helices from each of the three molecules. The optimal solvent content for density modification was found to be 79%.
Model building and refinement
An initial Cα model was built into the density from all three sources of phases described above, from SHARP, DM and DMMulti, using O (Jones and Kjeldgaard, 1997). The partial models were further cycled back into phase calculation in SHARP to improve the initial solvent envelope used for the solvent flipping procedure. This cycle was iterated many times until a reasonably complete model could be built. The amino‐acid side chains were then built into the partial model using the selenium and mercury sites to determine the correct register. Refinement of the model was carried out in BUSTER (BUSTER‐TNT 2.X) against the highest resolution data set with inclusion of the experimental phase information. Refinement was improved by anisotropic truncation of the structure factors (Strong et al, 2006) along the A and B axes to 4.3 Å, with the C axis kept at 3.6 Å. To increase the contribution of the high‐resolution terms in the resulting 2mFo‐DFc electron density maps, a B‐factor sharpening term was introduced during map calculation in FFT of between −50 and −80 Å2. Model validation was carried out using the Molprobity server (Davis et al, 2007) (Supplementary Table IV). The quality of the model compares favourably with structures of a similar resolution in the Protein Data Bank. Images were prepared using PyMol (The PyMOL Molecular Graphics System) and VMD (Humphrey et al, 1996).
In vivo [3H]‐glycylsarcosine transport assay
Uptake of the radioactive di‐peptide [3H]‐glycylsarcosine (Gly‐Sar) was measured at 37°C in cells overexpressing the PepTSo gene as described in Supplementary data. After an uptake period of 15 s, employed to approximate initial velocities of transport, cells were filtered to terminate transport and washed twice with ice‐cold transport buffer (Henderson and Macpherson, 1986). For estimation of the apparent Vmax and Km values for transport, uptake was measured over a substrate concentration range of 10 μM to 5 mM. PepTSo‐mediated transport was calculated by subtraction of rates seen in induced cells harbouring a control expression vector encoding the E. coli nucleoside transporter NupG. The resultant rates were expressed per milligram of PepTSo protein, as measured by quantitative immunoblotting. Data were fitted to the Michaelis–Menten equation using the non‐linear curve‐fitting program KaleidaGraph (version 4.0, Synergy software) in order to estimate kinetic parameters.
In vivoβ‐Ala‐Lys‐(AMCA) competition transport assay
Uptake of the fluorescent di‐peptide β‐Ala‐Lys‐(AMCA) was measured at 37°C in cells overexpressing the PepTSo gene essentially as described by Weitz et al (2007) and in Supplementary data. Transport of β‐Ala‐Lys‐(AMCA) was measured using fluorescence in a Fluostar Optima plate reader using an excitation wavelength of 340 nm and an emission filter with a wavelength of 460 nm.
Supplementary data are available at The EMBO Journal Online (http://www.embojournal.org).
Conflict of Interest
The authors declare that they have no conflict of interest.
We thank all the members and advisors of the Membrane Protein Structure Initiative for advice and support. We also thank Manami Kanazawa, Mutsuko Grant and Gill Murray for administrative support; and James Mansfield for technical assistance with the bioreactor fermentations and Jocelyn Baldwin for bioinformatic analyses. This research was funded primarily by the Biotechnology and Biological Sciences Research Council (BBSRC), Membrane Protein Structure Initiative (MPSi) (grant BBS/B/14418), with important contributions from the Wellcome Trust (grant 062164/Z/00/Z) and the Japan Science and Technology Agency. We thank the Membrane Protein Laboratory (MPL) staff at the Diamond Light Source Limited for their support. We also thank the beamline staff at the European Synchrotron Radiation Facility (ID23, ID29 and ID14eh4) and Diamond Light Source, UK (IO2, IO3 and IO4). DD was the recipient of an EMBO LT Fellowship. SN and DD acknowledge the current support of the Medical Research Council and Royal Society through the University Research Fellowship schemes, respectively. A part of this work was also supported by the Targeted Proteins Research Program of MEXT, Japan. The atomic coordinates have been deposited in the Protein Data Bank (accession code 2XUT).
Author contributions: SN, XX, DD, VP, MJM and SAB cloned the PepTSo gene and tested expression in the different vectors. VP, XX, JCI and SAB designed, conducted and analysed the transport assay data. SN, DD, AC and SI purified, crystallized and collected X‐ray diffraction data. SN and AC solved the heavy atom substructure, built the model and refined the structure. SN, DD, AC, VP, SAB and SI analysed the structure, functional data and wrote the paper. PWF and MSPS performed and analysed the molecular dynamics calculations.
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