Abstract
The leucine transporter (LeuT) from Aquifex aeolicus is a bacterial homolog of neurotransmitter/sodium symporters (NSSs) that catalyze reuptake of neurotransmitters at the synapse. Crystal structures of wild-type and mutants of LeuT have been interpreted as conformational states in the coupled transport cycle. However, the mechanistic identities inferred from these structures have not been validated, and the ligand-dependent conformational equilibrium of LeuT has not been defined. Here, we used distance measurements between spin-label pairs to elucidate Na+- and leucine-dependent conformational changes on the intracellular and extracellular sides of the transporter. The results identify structural motifs that underlie the isomerization of LeuT between outward-facing, inward-facing and occluded states. The conformational changes reported here present a dynamic picture of the alternating-access mechanism of LeuT and NSSs that is different from the inferences reached from currently available structural models.
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Acknowledgements
The authors gratefully acknowledge R. Stein for assistance with EPR data collection and EPR distance analysis. We thank H. Koteiche and P.R. Steed for critical reading and editing of the manuscript. We thank Extreme Science and Engineering Discovery Environment (XSEDE) for computer time. This work was supported by US National Institutes of Health grants U54-GM087519 (H.S.M., S.S., H.W., J.A.J., S.M.I. and B.R.), K05DA022414 (J.A.J.) and P01DA012408 (H.W.). K.K. was supported by a predoctoral National Research Service Award (F31-MH095383-01).
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K.K. and S.S. constructed mutants, expressed and purified protein, prepared samples and conducted DEER experiments. K.K. and H.S.M. designed the DEER experiments. K.K., S.S. and H.S.M. analyzed DEER data and interpreted the distance distributions. M.Q. designed, conducted and analyzed leucine-binding and alanine-transport experiments. S.M.I. and B.R. refined structural models with the restrained ensemble simulations method. All authors contributed to the mechanistic interpretation of the data, wrote and edited the manuscript.
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Supplementary Figure 1 Na+-dependent leucine binding to spin-labeled LeuT variants.
Leu binding in the presence of Na+ to spin-labeled LeuT was determined by means of the scintillation proximity assay (SPA) as described in the online Methods. Data were normalized to the level of leucine binding to the LeuT-WT, determined concurrently (n ≥ 3). Data are shown as the mean ± S.E.M. (a) Binding of 1.5 μM 3H-Leu (9 Ci/mmol) to 50 ng of spin-labeled LeuT in the presence of 150 mM NaCl. Most mutants with the exception of those in TM6 or in the Y268A or R5A backgrounds bind Leu with similar affinity and stoichiometry as the WT. (b) Saturation binding of 3H-Leu (9 Ci/mmol) by select mutants as indicated. Saturation binding for the tested LeuT variants was normalized with regard to the level of binding observed for LeuT-WT at 5 μM final concentration. The right shift of the curve indicates that these mutants, destabilized either by the Y268A or R5A substitutions or spin labeling of TM6, have lower affinity to leucine. Nevertheless, they bind leucine to the same level as WT at high leucine concentrations.
Supplementary Figure 2 Na+-dependent [3H]alanine uptake by spin-labeled LeuT variants.
Uptake of 3H-Ala by spin-labeled LeuT mutants reconstituted into proteoliposomes was conducted as described in the online Methods. Data were normalized to the level of alanine transport by the LeuT-WT, determined concurrently (n ≥ 3). Data are shown as the mean ± S.E.M. (a) Alanine transport (1 μM final concentration; 20 Ci/mmol) was monitored for 5 and 30 minutes, as indicated. (b) Kinetics of 3H-Ala transport. The initial rates of 3H-Ala transport were measured for 1 minute time periods at 3H-Ala concentrations ranging from 0.125 – 5 μM (with specific radioactivites from 49.5 Ci/mmol – 5 Ci/mmol). The transport rates of most mutants do not differ significantly from WT. For F208C-F306C, the deviation is attributable to a change in Km.
Supplementary Figure 3 Spin labeling of TM6 residues.
(a) The intracellular network of hydrogen bonding and electrostatic interactions stabilized by Y268A of IL3. (b) The network of spin label pairs monitoring the movement of TM6b and the loop connecting to TM7a is shown by black spheres connected by solid lines. b) Na+- and Leu-dependent changes in the distance distributions demonstrating the movement of TM6b in the WT (solid lines) and the R5A (dashed lines) backgrounds. The broad distributions hinder analysis of the magnitude of distance changes but are consistent with the ligand-dependent equilibrium of this TM between multiple conformations.
Supplementary Figure 4 Crystal structures of LeuT underestimate the closing of the extracellular vestibule.
Comparison of experimental distance distributions (solid lines) with predicted distributions based on the “inward-facing” (3TT3), “outward-facing” (3TT1) and “substrate-occluded” (2A65) crystal structures. The MMM package was used to generate predicted distance distributions on the extracellular side. This comparison demonstrates that the experimental distances in the Na+- and Leu-bound state fall outside the predicted distributions regardless of the crystal structure. Because MMM typically overestimates the distribution width, we interpret the systematic deviations between calculated and experimental distributions as evidence that the substrate-occluded conformation we observe in solution is not represented in the crystallographic record. Hence the crystal structures underestimate the closing of the extracellular side upon Na+ and Leu binding. The only exception to this seems to be EL4, for which the predicated distribution from the inward-facing structure overlaps the experimental distribution obtained in the presence of Na+ and Leu.
Supplementary Figure 5 The ‘substrate-occluded’ crystal structure overestimates the closing of TMs 1a and 2 on the intracellular side.
Comparison between experimental and MMM-predicted distances shows systematic deviations in the distributions of TMs 1a and 2. In contrast to the extracellular side, here the average distances are larger than those predicted by the occluded structure.
Supplementary Figure 6 Comparison of distance distributions at selected sites in the WT (solid line) and the Y268A and R5A (dashed lines) backgrounds.
The Y268A mutation induces movement of TMs 1a and 5 in the direction expected based on the inward-facing crystal structure. The (*) indicates components arising from aggregation during concentration of the mutants after gel filtration. The addition of Na+ and Leu does not reset the distributions back to WT-like. This suggests a loss of conformational coupling. Areas known to be a part of the rigid C structure (grey helices) also show changes in the distance distributions in the Y268A background. We interpret these changes as indicative of the global destabilization effects of these mutations.
Supplementary Figure 7 The LeuT scaffold.
(a) The static scaffold of LeuT. Narrow distance distributions between TMs 2, 3, 4, 5, 8, and 9 suggest a predominantly rigid scaffold. TM1a may undergo small scale movement as indicated by the width change in the TM1a-TM9 distribution. (b) Evidence of small scale movements of TMs 10 and 11 relative to TM2. This movement appears to be coordinated with that of TM7a as their pairwise distributions do not show Na+-dependent or Na+- and Leu-dependent changes in average distance or width.
Supplementary Figure 8 Analysis of DEER distance distributions.
(a) in WT background, (b) in WT background in the presence of β-OG, and (c) in R5A and Y268A backgrounds. For each mutant, we present the background-corrected decays and fits (left), the L curves with α parameter selected at the elbow (middle), and the normalized distance distributions (right).
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Kazmier, K., Sharma, S., Quick, M. et al. Conformational dynamics of ligand-dependent alternating access in LeuT. Nat Struct Mol Biol 21, 472–479 (2014). https://doi.org/10.1038/nsmb.2816
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DOI: https://doi.org/10.1038/nsmb.2816
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