As reported previously (Erichsen et al., 2010; Abrahamsen et al., 2013; Jensen et al., 2009), glutamate-induced EAAT1 anion current was inhibited in a concentration-dependent manner by UCPH-101 (Figure 3A and B). At low [UCPH-101] (2 μM) (Figure 3A, red trace) onset of inhibition was slow with complete inhibition reached only after several seconds. In agreement with the expectation of a non-competitive inhibition mechanism, the apparent K_i was essentially independent of the glutamate concentration (Figure 3B and C). In contrast, if UCPH-101 would show a competitive inhibition pattern, an increase of apparent K_i with the glutamate concentration would be expected, according to Equation 2.

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In Equation 1, K_i(0) and K_i(S) are the K_i values (inhibition constants) in absence and presence of glutamate. K_m(substrate) is the apparent Michaelis-Menten constant for glutamate, and [S] is the substrate concentration. Furthermore, we determined the voltage dependence of the UCPH-101 inhibitory effect. As expected, anion currents were fully inhibited at all membrane potentials (Figure 3—figure supplement 1).

To obtain a high time resolution for determining the effect of UCPH-101 on transport kinetics, we applied glutamate rapidly to EAAT1 using a piezo-based solution exchange device. This system has a 5–10 ms time resolution when applied to whole cells, and also allows the rapid removal of substrate, providing information on the recovery of current after glutamate removal. However, due to the millisecond time resolution, it will limit determination of very early intermediates in the transport cycle, which are present in a sub-millisecond time domain, but the time resolution is high enough for determining glutamate transporter turnover rate, and how it is affected by the presence of inhibitor. EAAT1 anion currents (Figure 4A) and transport currents (Figure 4E) show rapid rise of the current after glutamate application within the time resolution afforded by solution exchange (5–10 ms). The rise of the current is followed by rapid decay of a transient current component to the steady state, as demonstrated previously (Grewer et al., 2000). This transient phase of the current was previously assigned to steps associated with the glutamate translocation reaction (Wang et al., 2018). After pre-incubation and in the continuous presence of UCPH-101, both transient and steady-state current amplitude were reduced in a dose-dependent manner, as expected (Figure 4B and F, currents were fully eliminated at 40 μM UCPH-101), but at concentrations close to the apparent K_i, the decay of the current was also slowed (Figure 4D, τ=11 ± 1.3, 16±2.1, 20±2.1 ms, at 0, 0.2, and 2 μM UCPH-101, respectively). The reduction of the decay rate of the transient current indicates a slowing of the translocation reaction in the presence of UCPH-101. In contrast to competitive inhibitors, UCPH-101 application in the absence of glutamate did not induce any currents, as expected for non-competitive inhibitors, which are not known to be able to block the glutamate transporter leak anion conductance (Figure 4C and G).

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Upon removal of glutamate, recovery of the transient current upon glutamate application in a second pulse was relatively slow, with a time constant of 95±4 ms, most likely reflecting the turnover time of the transporter, which has to recycle its binding sites to outward-facing, after passing through a whole transport cycle. At 0.2 μM UCPH-101 recovery of the transient current after glutamate removal occurred with a time constant of 115±11 ms, as quantified in Figure 4F and H. Therefore, it appears that UCPH-101 does not significantly slow the recovery rate of the transient current. The most likely explanation is that, at low concentrations (<1 μM) UCPH-101 binding to EAAT1 and unbinding are very slow, with time constant of 10 s for binding, and 100 s for dissociation (Abrahamsen et al., 2013). Thus, within the time course of the paired-pulse experiment (1.4 s), UCPH-101-bound and -unbound transporter populations do no interconvert, and the time course of current recovery, thus, reflects that of the UCPH-101-free state.

Finally, we tested whether UCPH-101 binding affects how Na⁺ interacts with the apo (glutamate-free) form of the transporter. This question was raised from the crystal structures of EAAT1 in the presence of UCPH-101 (Canul-Tec et al., 2017). The structure shows Na⁺ bound only at the Na2 position (Canul-Tec et al., 2017). However, two more Na⁺ binding sites exist, Na1 and Na3 (Canul-Tec et al., 2017; Reyes et al., 2009; Boudker et al., 2007; Yernool et al., 2004; Verdon and Boudker, 2012; Guskov et al., 2016; Wang et al., 2019). As reported previously, Na⁺ binding to a glutamate-free form of EAAT2 and -3 is electrogenic (Grewer et al., 2000; Watzke et al., 2001; Grewer et al., 2012), generating transient currents due to Na⁺ movement into its binding site upon voltage jumps to more negative membrane potentials. Consistently, step changes of the membrane potential from –100 to +60 mV resulted in transient currents (Figure 4—figure supplement 1), which decayed with a time constant in the 0.5 ms range (140 mM Na⁺), in the absence of glutamate. Non-specific currents were subtracted by applying 200 μM TBOA. In the presence of UCPH-101, the charge movement was still present (Figure 4—figure supplement 1B), and the midpoint potential (a measure of Na⁺ affinity) was not significantly changed (Figure 4—figure supplement 1C). These results are consistent with the interpretation that Na⁺ binding (most likely to the Na1 and Na3 sites) is not inhibited by bound UCPH-101 and occurs with similar affinity as in the absence of the inhibitor.

In the next paragraphs, we describe electrophysiological measurements on ASCT2 in the presence of UCPH-101, to test whether the inhibition mechanism is conserved between the EAAT1 and ASCT2 members of the SLC1 family. To corroborate the residues directly contributing to the UCPH-101-bound state in EAAT1 suggested by docking, we used molecular dynamics (MD) simulations, to investigate the stability of UCPH-101 in its EAAT1 binding pocket (Materials and methods). From the EAAT1 structure bound to the substrate aspartate and UCPH-101 in the allosteric site (5LLM), we generated a model of EAAT1 inserted into a lipid bilayer in a water box. After equilibration, UCPH-101 remained stable in the original binding pocket in six 100 ns simulations (four representative ones shown in Figure 5D). We selected two conserved residues (Y127, M271; Figure 5A and Figure 1—figure supplement 1) to estimate distance changes to bound UCPH-101 together with RMSD calculations. Interestingly, the trajectories show that the position of UCPH-101 is stable relative to Y127 and M271 in 100 ns simulations, and these two residues stay in close contact with the UCPH-101 pyran ring oxygen and the amino group nitrogen (Figure 5D). It should be noted that UCPH-101 has two stereo-centers. For the simulations, we used the stereo-configuration analogous to the one from the EAAT1 UCPH-101-bound structure.

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Trajectory and RMSD data for panels (D-F).

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To investigate the stability of inhibitors in the predicted ASCT2 allosteric binding pocket, we also performed MD simulations on UCPH-101-bound ASCT2_WT and ASCT2_F136Y/I237M. Residues F136Y and I237M (Figure 5C, Figure 5—figure supplement 1) were selected to evaluate distance changes to UCPH-101 during equilibration. The distance of UCPH-101 is relatively stable with respect to Y136 and M237 in 300–500 ns simulation trajectories (Figure 5E, Figure 5—figure supplement 1), while a slight, initial increase in the RMSD indicates relaxation of the structure compared to the initial, docked starting state. Two full dissociation events into the lipid bilayer were observed in six simulations within 300 ns for ASCT wild-type (Figure 5E), consistent with the predicted slow binding/dissociation kinetics, while no dissociation was observed in the double-mutant transporter (Figure 5F). The distance between selected atoms of UCPH-101 and ASCT2 were maintained within 6 Å in the double-mutant transporter, whereas in the wild-type these distances were 8–11 Å (Figure 5E), indicating that these interactions are less favorable in the wild-type transporter. Finally, as a control, we measured the distance between bound amino acid substrate and a residue in the binding site throughout the simulation. This distance remained stable throughout the simulations, until amino acid substrate dissociation occurred (dissociation is expected due to the low substrate affinity), illustrating convergence of our simulations and increasing the confidence in our approach.

To test the predictions from docking calculations and MD simulations, we next experimentally investigated the interaction of UCPH-101 with ASCT2_WT, and transporters with mutations to the analogous positions in ASCT2, using electrophysiological characterization of anion current, which is activated during substrate exchange. Anion conductance is an indirect measure of ASCT2 transport activity, but was previously shown to correlate with transport activity (direct amino acid transport measurements are shown below) (Grewer and Grabsch, 2004). Typical anion currents, using the highly permeant anion SCN^-, were inwardly directed, due to SCN^- outflow through the ASCT2 anion conductance (Figure 6A). As expected, the anion currents increased with increasing serine concentration, with an apparent K_m of 280±40 μM. When serine was co-applied together with UCPH-101, the current was inhibited, but not to 100%, even at saturating [UCPH-101] (Figure 6B). In addition, inhibition required much higher UCPH-101 concentrations than in EAAT1. The UCPH-101 dose-response relationship, at a constant serine concentration of 100 μM (Figure 6C) demonstrates maximum inhibition of about 45% at 200 μM UCPH-101, with an apparent K_i value of 77±20 μM (Figure 6C and D). Although full saturation could not be reached due to UCPH-101 not being fully soluble at a concentration of 500 μM, the fit to the dose-response curve indicates partial inhibition even at saturating concentration (Figure 6C, red line). Maximum inhibition was not dependent on the serine concentration, as expected (Figure 6D). Furthermore, the apparent K_i was only weakly dependent on [serine] (Figure 7D). From these results, we presume that UCPH-101 operates as a weak, non-competitive, partial inhibitor for the wild-type ASCT2 transporter.

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Current traces for Figure 7B, and the original data for panels (C-E).

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As a direct measure of amino acid transport, we next tested the effect of UCPH-101 on amino acid (L-serine) uptake. The competitive inhibitor L-cis-BPE was used to determine the specific component of L-serine uptake (Garibsingh et al., 2021). We observed that serine uptake was also inhibited by UCPH-101 at a saturating concentration (Figure 6E); however, similar to the electrophysiological data, this inhibition was not complete, with 58% of the specific uptake being blocked by UCPH-101.

To experimentally test the hypothesis, predicted by docking (see above), that residues F136 and I237 contribute to UCPH-101 binding, four mutant ASCT2s were generated based on EAAT1, F135Y, F136Y, I237M, and the F136Y/I237M double mutant (predicted docking pose for the double-mutant ASCT2 is shown in Figure 7A). Before testing with UCPH-101, the mutant transporters were functionally analyzed by whole-cell current recording experiments, to check whether the mutations altered transporter functionality. All four mutant transporters exhibited wild-type-like anion currents upon substrate application. Mutant transporters with F136Y and F136Y/I237M substitutions changed the substrate selectivity, that is, in contrast to ASCT2_WT, anion current could not be observed after application of glutamine (Table 1). In addition, the F136Y mutation decreased the serine apparent affinity from a K_m of 280±40 μM (ASCT2_WT) to 790±130 μM (Table 1). None of the other mutant transporters showed a significant effect on the K_m for Ser/Ala current activation. It remains unclear why mutations to these sites have some effect on substrate selectivity/affinity, despite being far removed from the substrate binding site. We hypothesize that indirect effects of the mutations are involved.

We next determined the effect of UCPH-101 on the mutant ASCT2s. Serine-induced anion currents were inhibited by UCPH-101 in all four mutant transporters (Figure 7B–E), however, to varying degrees. Original UCPH-101 inhibition data for the double-mutant transporter and dose-response curves are shown in Figure 7B and C. In contrast to the wild-type transporter, UCPH-101 was able to block virtually 100% of the serine-induced inward current at a concentration of 200 μM in both F136Y and the double-mutant transporter (Figure 7B and C). However, no complete block was observed in ASCT2_I237M, and the UCPH-101 interaction was of low affinity. (Figure 7C and D). For the double-mutant F136Y/I237M transporter, the apparent UCPH-101 affinity was significantly increased over the wild-type transporter, at least at low [serine]. As shown in Figure 7B and D, in ASCT2_F136Y/I237M, UCPH-101 fully blocked the anion currents above 100 μM UCPH, resulting in an apparent K_i value of 4.3±2.4 μM (Figure 7C and E).

Subsequently, we compared the UCPH-101 apparent K_i as a function of the substrate concentration (Figure 7D). For the double-mutant transporter, the apparent K_i increased with increasing [serine] at low concentration but leveled off at high concentrations, which is unexpected for a purely non-competitive inhibition, but consistent with a mixed inhibition mechanism, in which the inhibitor binds somewhat more strongly to the apo-transporter than the substrate-bound form.

Finally, we tested the UCPH-101 inhibition of the double-mutant transporter at varying membrane potentials. Serine-induced anion currents were significantly smaller than in the presence of UCPH-101 (Figure 6—figure supplement 1B), compared to control (Figure 6—figure supplement 1A). Inhibition was more pronounced at negative membrane potentials, as shown in Figure 6—figure supplement 1C.

When serine was applied rapidly to ASCT2_WT and ASCT2_F136Y/I237M, in the presence of intracellular SCN^- (substrate-induced anion current), the current was activated immediately (Figures 8A and 9A), within the time resolution of the solution exchange (5–10 ms). In some experiments, a small, but significant transient current component was observed (Figure 9A), due to the population of an intermediate along the translocation pathway with high anion conductance, as proposed previously (Zander et al., 2013). Unlike EAAT1 in forward transport mode, ASCT2 anion current also deactivated rapidly upon serine removal, and recovered very quickly when a second pulse of serine was applied (Figure 8A, time of decay and recovery all within the time resolution of solution exchange). Similar results were observed for ASCT2_F136Y/I237M (Figure 9A). However, when serine was applied in the presence of 100 μM UCPH-101 (pre-incubated for 5 min), steady-state anion current was inhibited, as expected, but in addition a significant slowing of anion current rise after serine application, decay after serine removal, and recovery after a second pulse of serine application was observed, for both ASCT2_WT (Figure 8B) and ASCT2_F136Y/I237M (Figure 9B). The time constant of the responses, which were biphasic and required fitting with two exponential components, are summarized in Figures 8D and 9D, demonstrating a significant increase in the time constant for recovery, in particular for the fast component of the recovery. These results suggest that UCPH-101 not only inhibits current amplitude, but also slows current kinetics and serine exchange turnover (as measured by current recovery), as expected for a fast-binding inhibitor that shows rapid pre-equilibrium between the UCPH-101-bound and -unbound transporter states, with respect to the substrate-induced transporter kinetics. Using pre-equilibrium conditions, the following equation can be used to describe the kinetics of the translocation equilibrium:

Here, k_obs is the observed rate constant for the rise or decay of the anion current (i.e. equilibration of the translocation equilibrium), which is a sum of the rate constants for forward (k_f) and reverse (k_r) translocation. [S]_o and [S]_i are the external and internal substrate concentrations, respectively, [I] is the UCPH-101 concentration and K_m and K_i have their regular meaning. When amino acid substrate is rapidly removed, [S]_o becomes 0 and it is possible to isolate the reverse translocation rate constant.

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Similar to EAAT1, rapid external serine application to ASCT2 elicits transient inward transport currents (in the absence of permeable anion), which decay within 20 ms back to baseline (Figure 8E) in the absence of UCPH-101. In contrast to EAAT1, ASCT2 is an amino acid exchanger, therefore, the experiments were performed in the exchange mode (saturating [Na⁺] and [amino acid] on the intracellular side of the membrane). Because ASCT2 amino acid exchange is electroneutral at equilibrium (equal net rate of forward and reverse charge movement), no steady-state current was observed under these conditions (Figure 8E). However, upon rapid removal of extracellular amino acid, transient outward current was observed (Figure 8E), due to the re-equilibration of the homo-exchange translocation equilibrium to favor the outward-facing conformation in the absence of external amino acid. In contrast to the EAATs, Na⁺ apparent binding affinity to the apo-form of the ASCT2 transporter is high (K_m < 1 mM [Zander et al., 2013]). Therefore, the Na⁺ binding equilibria of the amino acid-free transporter are fully saturated at 140 mM external [Na⁺], and the amino acid-induced charge movement can only be caused by Na⁺ binding to the amino acid-bound transporter, substrate translocation, or, most likely, both of those processes. Alanine and serine exchange was previously reported to be rapid in ASCT2 (Wang et al., 2022). Consistent with this proposal, transient transport current recovered much faster than in EAAT1 after amino acid removal (Figure 8E and H), with a time constant of 15±0.2 ms (Figure 8H).

When the same paired-pulse serine solution exchange protocol was applied to ASCT2 in the presence of UCPH-101, similar transient currents were observed (inward upon serine application and outward upon removal), but the amplitude of the transient currents was significantly reduced (Figure 8F). However, similar to the observations from the anion currents, UCPH-101 was unable to completely block transient transport current. Residual inward transient current amplitude at 100 μM [UCPH-101] was 50% compared to control. As expected, UCPH-101 application alone did not generate any transient currents (Figure 8G). Recovery time of the current was increased twofold to 30±0.4 ms at 100 μM UCPH-101 (Figure 8H). Overall, these data indicate that UCPH-101 reduces, but does not eliminate charge movements induced by Na⁺ binding to the amino acid-bound transporter, and/or substrate translocation across the membrane, in other words, the steps needed for amino acid transport by ASCT2.

Similar results were obtained for ASCT2_F136Y/I237M (Figure 9). As in the case for anion current, UCPH-101 also significantly slowed the kinetics of decay and recovery of the transient transport current (Figure 9E–H), indicating that UCPH-101, due to decreased affinity compared to EAAT1, also acts like a rapidly equilibrating inhibitor in the double-mutant ASCT2 transporter.

It was previously shown that voltage jumps to substrate-free ASCT2 result in transient charge movement from Na⁺ binding/dissociation (Zander et al., 2013) similar to EAATs (Grewer et al., 2012). When a step change in the membrane potential was applied to ASCT2_F136Y/I237M-expressing cells (Figure 9—figure supplement 1A), transient currents were observed. In these recordings, non-specific currents were subtracted by γ-(4-biphenylmethyl)-L-proline, which is a commercially available, competitive inhibitor of ASCT2 (Singh et al., 2017). In the presence of UCPH-101, the transient currents were reduced at all membrane potentials (Figure 9—figure supplement 1B). Q-V relationships are shown in Figure 9—figure supplement 1C, suggesting that Na⁺ binding and release steps in apo-transporter were inhibited by UCPH-101, but not eliminated, similar to our results obtained with EAAT1 shown above (Figure 4—figure supplement 1). Since under substrate-free conditions the translocation is not going to proceed, these results suggest that UCPH-101 likely affects Na⁺ binding to the proposed Na3/Na1 binding sites.

Our next goal was to confirm the location of the allosteric binding site by identifying compounds chemically different from UCPH-101 that interact with the ASCT2 allosteric binding site. We therefore employed virtual screening of the ZINC20 lead-like library (3.8 million compounds) to identify potential binders (Materials and methods). We analyzed the top scoring compounds for closer inspection and selected compounds that made predicted hydrogen bonding interactions to side chains of the allosteric binding site. From the best compounds found in the virtual screening, 11 were tested experimentally. We tested the inhibitory effect at 100 µΜ of serine. One of these compounds (#302, Figure 10A, docking pose shown in Figure 10B) inhibited ASCT2 anion current (Figure 10G and H), with an apparent K_i of 238±58 µM, as well as transient transport current elicited by the transported substrate L-serine. In addition, 300 μM compound #302 inhibited the peak amplitude of ASCT2 transient transport current after rapid application of 1 mM serine to 48 ± 6% of the control current (Figure 10C and D). In contrast to UCPH-101, however, the presence of compound #302 did not have significant effect on the decay kinetics of the transient current, or the recovery of transient transport current after removal of amino acid substrate (τ=19 ± 2.0 ms in the absence and 39±1.4 ms in the presence of #302, recovery kinetics shown in Figure 10F). As for UCPH-101, application of compound #302 alone (in the absence of serine) did not induce any current response (Figure 10E). To test whether compound #302 binds to the predicted allosteric ASCT2 binding site, we determined the apparent K_i with ASCT2_F136Y/I237M (Figure 10G) as 90±30 µM, demonstrating that the double mutation in the binding site increases the apparent affinity for compound #302, as was expected from the UCPH-101 results. Furthermore, the inhibition mechanism of compound #302 was found to be non-competitive (Figure 10I). Finally, compound #302 is able to inhibit ASCT1 substrate-induced anion current. This result was expected, since the allosteric binding site is largely conserved between ASCT1 and -2 (I237 is substituted by L in ASCT1, Figure 1—figure supplement 1) Notably, while compound #302 is not an optimized allosteric inhibitor of ASCT2, it provides a further validation for the location of the binding site as well as a starting point for developing future tool compounds targeting ASCT2 allosterically.

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This report provides additional mechanistic information on the action of the allosteric inhibitor, UCPH-101 on EAATs. In agreement with previous studies, UCPH-101 shows the hallmark of a non-competitive inhibitor of EAAT1, that is, a lack of effect of substrate concentration on the inhibitor K_i. In addition, Na⁺ affinity of the apo-transporter seems to be unaffected. We also concluded that UCPH-101 does not affect the substrate binding steps, mainly by analysis of the kinetics of pre-steady-state currents in the presence of UCPH-101. These conclusions are in agreement with the EAAT1 structure in complex with both UCPH-101 and a competitive inhibitor, TFB-TBOA (Shimamoto et al., 2004), which demonstrated that the allosteric and substrate binding sites can be occupied at the same time.

In contrast to substrate binding, we propose that the substrate translocation step is the major partial reaction that is blocked in the UCPH-101-bound state. This interpretation is based on the significant reduction of the amplitude and the rate of the transient current decay in response to glutamate application (Figure 4), which for EAAC1 was previously assigned to the glutamate translocation step. From a structural viewpoint, this interpretation is logical, and was proposed by Canul-Tec et al. in 2017 from the EAAT1 structure in complex with UCPH-101 (Canul-Tec et al., 2017). Since binding occurs at the interface between transport and the trimerization domain, it is likely that transport domain movements relative to the trimerization domain are affected by the occupied allosteric site, either fully inhibiting those movements or slowing them to attain partial activity.

The effect of UCPH-101 on the glutamate-induced anion current of EAAT1 fits with this interpretation. It was shown previously that UCPH-101 exhibits very slow binding and dissociation kinetics (on the 10 s second time scale), much slower than the partial reactions of the glutamate-induced transport process and the turnover rate (in the 10–30 s^–1 range). Therefore, it is likely that the UCPH-101-free and -bound states interconvert slowly on the time scale of transport. Thus, UCPH-101 reduces the amplitude of glutamate-induced anion and transport current, without a significant effect on the observed kinetics associated with these reactions.

The development of novel inhibitors are essential steps for potential treatment of diseases, especially for ASCT2 transporter. In previous reports, overexpression of ASCT2 was observed in several cancer cell lines (Bröer et al., 1999; Son et al., 2013; Wahi and Holst, 2019; Kanai et al., 2013). Among the several published ASCT2 inhibitors, most of them target the substrate binding site. However, allosteric modulators would be useful because of the independence of their inhibitory effect on substrate concentration. The known allosteric binding pocket of EAAT1 as well as the biomedical importance of ASCT2 prompted us to investigate whether a similar allosteric mechanism is present in ASCT2; and, indeed, UCPH-101 was found to interact with this binding site. Therefore, the importance of this report lies in the generation of a new structural model proposed here to develop future novel allosteric modulators with the potential for higher affinity and specificity for ASCT2 in future compounds.

In the EAAT members of the SLC1 family, UCPH-101 was found to be specific for EAAT1. For example, in wild-type Glt-1 (EAAT2), no inhibition was observed, unless EAAT1/EAAT2 chimeras were generated that contained the EAAT1 N-terminal six transmembrane domains (Abrahamsen et al., 2013). In contrast to the EAATs, however, it was not known whether UCPH-101 can interact with the ASCT members of the SLC1 family. Our results reported here are, to our knowledge, the first to show that UCPH-101 inhibits ASCT2, providing evidence for the existence of the allosteric binding site in the same location as in EAAT1. While UCPH-101 is only a partial inhibitor of wild-type ASCT2, and its apparent inhibition constant is relatively high (low affinity, in the range of 100 μM), it demonstrates the principle of allosteric inhibition, or modulation of ASCT function through the allosteric binding site. Importantly, we were able to restore complete inhibition of substrate-induced anion current in mutant ASCT2 transporters, in which the proposed UCPH-101 binding site was modified to resemble that of EAAT1. In the double-mutant ASCT2_F136Y/I237M the affinity was also increased compared to the wild-type transporter, although not reaching the high-affinity levels seen in EAAT1.

As expected, UCPH-101 shows the hallmarks of a non-competitive inhibitor for ASCT2_WT, however, for the double-mutant transporter a mixed inhibition mechanism was observed, pointing to higher affinity of the apo-transporter for UCPH-101, compared to the substrate-bound form. The reason for this is not known, but somehow the UCPH-101 binding site in this mutant transporter must communicate with the substrate binding site. A proposed kinetic mechanism for inhibition of EAAT1/ASCT2 by UCPH-101 is shown in Figure 11, in analogy to previously published alternating access mechanisms for the SLC1 family (Kanner and Bendahan, 1982; Kanner and Zomot, 2008). Here, UCPH-101 can bind to all of the states the transporter can access during the transport cycle, including substrate- and Na⁺-bound states. The reaction that is affected by occupation of the allosteric site is the translocation reaction, or reactions closely associated with it, such as Na⁺ binding to the substrate-bound transporter. In EAAT1, due to the high affinity of the compound, equilibration of the UCPH-101-bound and -unbound states is slow, thus, UCPH-101 inhibits the transient and steady-state currents, with little effect on apparent transport kinetics. In essence, UCPH-101 acts by removing active EAAT1 transporters from the pool, thus inhibiting the overall transport rate. On the other hand, equilibration of the UCPH-101-bound and -unbound states is fast in ASCT2, therefore, kinetics of substrate-induced current activation and recovery are slowed in the presence of inhibitor. Thus, the kinetic mechanism shown in Figure 11 can account for the subtleties of kinetic differences in UPCPH-101 effects between EAAT1 and ASCT2.

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One limitation with current compounds targeting ASCT2 for cancer therapy is that they are amino acid-like compounds targeting the substrate binding site, and thus have poor pharmacokinetics. Interestingly, we were able to identify a compound with a structure unrelated to UCPH-101, compound #302, which inhibited wild-type ASCT2 in a non-competitive manner, although at relatively high concentrations and, like UCPH-101, showing only partial inhibition of the transient transport current elicited by substrate application. This compound was found from virtual screening against the putative allosteric binding site. Interestingly compound #302 also inhibited ASCT1, in which the critical residues in the allosteric binding site are similar to ASCT2. Like UCPH-101, compound #302 is relatively hydrophobic and harbors an amino function. However, it also has a OH group, suggesting that additional hydrophilic interaction may be important in the allosteric binding site. These results further support the presence of the allosteric binding site in ASCT2 and suggest that it may be possible to identify allosteric inhibitors of ASCT2 with novel scaffolds, opening new avenues for future structure-activity relationship studies, to improve affinity and specificity.

ASCT2 has recently received attention due to its involvement in neutral amino acid homeostasis in cells, in particular cancer cells. It was shown that down-regulation of ASCT2 function either by siRNA or by competitive inhibitors, can block the growth of cancer cells in cell-line models, as well as in vivo tumor transplants (Ni et al., 2019; Wang et al., 2015). Competitive inhibitors have the disadvantage of becoming less effective as the amino acid concentration rises. Having allosteric inhibitors available would result in amino acid concentration independent block of ASCT2 function, which would be much more desirable for pharmacological applications. The existence of the allosteric binding site on ASCT2 raises the possibility that such compounds could be developed, which, in contrast to UCPH-101, would result in complete inhibition of transporter function.

The results presented in this report reveal a conserved allosteric inhibition mechanism for SLC1 members for the first time. The results suggest that the major effect of the compound, once bound to the binding site at the interface between the transport and trimerization domain, is to block reactions associated with substrate translocation and anion conductance activation. In contrast, other partial reactions, such as substrate and Na⁺ binding can still take place, although the electrogenicity of Na⁺ binding is reduced, pointing to a slight conformational change of the substrate-free transporter state induced by UCPH-101. While UCPH-101 is a partial and weak inhibitor of wild-type ASCT2, complete inhibition could be restored by mutating the UCPH-101 binding site to one that resembles EAAT1. Therefore, our results suggest that ASCT2 also harbors the allosteric binding site, however, with differences in the amino acid side chains contributing to the site. These results raise the possibility that this allosteric binding site can be exploited by future compounds specifically targeting ASCT2. Our results involving the novel inhibitor compound #302 further confirm the location of the allosteric binding site in ASCT and suggest that compounds with varying chemical scaffolds could be found that modulate or completely inhibit SLC1 activity. In light of the emerging role of ASCT2 as an anti-cancer drug target, the future characterization of this allosteric site appears promising.

HEK293 cells (American Type Culture Collection, ATCC No. CRL 1573) were cultured as described previously (Wang et al., 2022). The cell line was authenticated by STR profiling (ATCC). Cells were tested for mycoplasm contamination using 4′,6-diamidino-2-phenylindole staining and confocal microscopy. Cell cultures were transiently transfected with wild-type EAAT1 or wild-type/mutant rASCT2 cDNAs, inserted into a modified pBK-CMV expression plasmid. Transfection were performed according to Jetprime transfection reagent and protocol (Polyplus). The cells were transfected after 24–36 hr then used for electrophysiological analysis.

Currents associated with ASCT2 and EAAT1 were measured in the whole-cell current recording configuration. Whole-cell currents were recorded with an EPC7 patch-clamp Amplifier (ALA Scientific, Westbury, NY, USA) under voltage-clamp conditions. The resistance of the recording electrode was 3–6 MΩ. Series resistance was not compensated because of the small whole-cell currents carried out by EAAT1, ASCTs. The composition of the solutions for measuring amino acid exchange currents in the anion conducting mode was: 140 mM NaMes (Mes = methanesulfonate), 2 mM MgGluconate₂, 2 mM CaMes₂, 10 mM 4-(2-hydroxyethyl)piperazine-1-ethanesulfonic acid (HEPES), with additional amino acid substrate (Glu or Ser) pH 7.3 (extracellular), and 130 mM NaSCN (SCN = thiocyanate, for EAAT1 NaSCN was replaced with KSCN), 2 mM MgGluconate₂, 5 mM ethylene glycol-bis(2-aminoethylether)-N,N,N',N'-tetraacetic acid (EGTA), 10 mM HEPES, pH 7.3 (intracellular), as published previously (Wang et al., 2020). For the measurement of the transport component of the current, intracellular SCN^- was replaced with the Mes^- anion.

Voltage jumps (–100 to +60 mV) were applied to perturb the translocation equilibrium and to determine the voltage dependence of the anion conductance (Wang et al., 2018). To determine EAAT1/ASCT-specific currents, external solution contained 140 mM NaMes in the presence of varying concentrations of amino acid substrate. The internal solution contained 130 mM NaSCN (KSCN for EAAT1) in the presence of 10 mM amino acid substrate. Competitive blocker TBOA (Shimamoto et al., 1998; Shimamoto et al., 2004), or (R)-gamma-(4-biphenylmethyl)-L-proline (Singh et al., 2017) was used in control voltage jump experiments, yielding the unspecific current component, which was subtracted from the total current. Capacitive transient compensation and series resistance compensation of up to 80% was employed using the EPC-7 amplifier. Non-specific transient currents were subtracted in Clampfit software (Molecular Devices).

Fast solution exchanges were performed using the SF-77B (Warner Instruments, LLC, MA, USA) piezo-based solution exchanger, allowing a time resolution in the 10 ms range. Amino acid substrate was applied through a theta capillary glass tubing (TG200-4, OD = 2.00 mm, ID = 1.40 mm. Warner Instruments, LLC, MA, USA), with the tip of the theta tubing pulled to a diameter of 350 μm and positioned at 0.5 mm to the cell (Wang et al., 2022; Shi et al., 2021). For paired-pulse experiments, currents were recorded with 10/20 ms interval time after removal of amino acid.

HEK293T cells were plated on collagen-coated 24-well plates (0.5×10⁵ cells/well) in Dulbecco’s modified Eagle’s medium containing 10% fetal bovine serum, penicillin/streptomycin (100 units/ml), 4.5 g/l glucose, sodium pyruvate, and glutamine (4 mM). Forty-eight hr post transfection with hASCT2 (see above), the cells were washed with uptake buffer (140 mM NaMes, 2 mM magnesium methanesulfonate, 2 mM calcium gluconate, 10 mM HEPES, pH 7.4, 5 mM glucose) two times and pre-incubated in the same buffer for 10 min. Subsequently, buffer was replaced with fresh buffer containing unlabeled L-serine and 0.1 μCi of [¹⁴C] L-serine (Moravek Biochemicals; total concentration 100 μCi/ml). After 5 min of incubation at room temperature, uptake was terminated by washing twice with 0.1 ml of uptake buffer on ice (after 5 min, uptake was in the linear range, as determined by quantifying the time dependence of uptake for times up to 5 min). The cells were then solubilized in 0.2 ml of 1% SDS, and radioactivity was measured by scintillation counting in 3 ml of scintillation fluid. Unspecific L-serine uptake was determined using the ASCT2 competitive inhibitor L-cis-BPE (Garibsingh et al., 2021).

The model system for MD simulations was generated with VMD software (Humphrey et al., 1996) using an EAAT1 (5LLM) and ASCT2 (7BCS) structure. The final EAAT1/ASCT2 model was inserted in a pre-equilibrated POPC lipid bilayer with the dimensions about 130×130×90 Å. TIP3P water was added to generate a box measuring about 100 Å in the z-direction. NaCl were added at a total concentration of 0.15 M and the system was neutralized. The total numbers of atoms in the EAAT1 system were 168926, 193804 in ASCT2. Simulations were run using the CHARMM36 force field. NAMD (Phillips et al., 2005) simulations were performed using 2000 steps of minimization, followed by 10 ns equilibration runs under constant pressure conditions (NPT), and then for 100 ns, 300 ns or 500 ns (Wang et al., 2021). The RMSD (calculated from the peptide backbone) increased from 1.5 Å soon after simulation start to ~3 Å after 2 ns of equilibration, after which it was in steady state. The cutoff for local electrostatic and van der Waals interactions was set to 12 Å. For long-range electrostatic interactions, we used the particle-mesh Ewald method implemented in NAMD. Bonds to hydrogen atoms and TIP3P water were kept rigid using SHAKE. The time steps of the simulations were 2 fs. The time evolution of distances and distribution function analysis were calculated by Tcl/Tk programs built in the VMD software. For distance calculations, in EAAT1, we selected atoms Y127(CA) and M271(CA) for EAAT1 and (O) and (N) for UCPH-101 as reference atoms. In ASCT2_WT, we selected atoms F136(CZ) and I237(CD) for ASCT2_WT and (N1) and (O2) for UCPH-101. In ASCT2_F136Y/I237M distance calculation, we selected atoms Y136(OH) and M237(SD) from the transporter, and (N1) and (O2) from UCPH-101 as reference. We also selected S601(CA) and S353(CA) for ASCT2_WT and ASCT2_F136Y/I237M to evaluate the distance changes of substrate. The UCPH1-101 force field parameters were generated by SWISSPARAM. The parameter file is attached to the original data submitted with this manuscript.

The data analysis was performed in Microsoft Excel and Microcal Origin software. Apparent inhibition constants (K_i) were obtained by fitting the dose-response curve of the current (I) with the following equation:

Here, I₁ and I₂ are the current amplitudes in the absence of inhibitor, and at saturating UCPH-101 concentration. Error bars are shown as mean ± standard deviation, collected from recordings of 6–10 cells, for statistical analysis.

Transient signals of piezo-based solution-exchange results were analyzed in Clampfit software (Axon Instruments) by fitting with a sum of two exponential components. I = I₁·exp(−t/τ_rise) + I₂·exp(−t/τ_decay). Here, I is the current amplitude, τ the time constant, and t the time.

All docking calculations were conducted with the Schrödinger package (Maestro, 2021). ASCT2 (PDB ID: 7BCS) was prepared for docking using the Maestro Protein Preparation Wizard under default parameters. Glide v2020-2 was used to perform docking. The allosteric binding site was defined using the Maestro Receptor Grid Generation panel and the coordinates of the site were marked with UCPH-101, a reference ligand extracted from a superposition of an EAAT1 structure solved with bound UCPH-101 (PDB ID:5LLM or 5MJU generated the same result). We performed both rigid and flexible docking with and without hydrogen bond constraints at F377 and positional constraints in the non-mutated ASCT2 structure. However, docking poses were unrealistic and exhibited poor scores, and we thus, concluded they are unusable for further study.

We remodeled the side chains of two residues in ASCT2 (i.e. F136Y and I273M) on a fixed backbone to mimic the UCPH-101 binding site in EAAT1, using SCWRL4 (Krivov et al., 2009). Grid preparation utilized positional constraints as highlighted in Figure 1A and excluded volume at F192 with a radius of 2.5 Å. The pose that had the best docking score was used to carry out the MD simulations.

The ZINC20 Lead-Like library (‘In Stock’; 3.8 million compounds) was virtually screened against the WT ASCT2 allosteric site using Glide, as described above. The 1000 top-scoring compounds from the docking screen were further analyzed. In particular, because errors in docking can occur in large virtual screens, we inspected the docking poses of the top-ranking compounds to remove molecules with problematic pose or strained conformations, and prioritized them for experimental testing (Bender et al., 2021). We focused on molecules that interact with the conserved residues in the allosteric site (Figure 2C). We purchased 11 molecules for experimental testing.

The funders had no role in study design, data collection and interpretation, or the decision to submit the work for publication.

This study was supported by a grant from the National Institutes of Health (http://www.nih.gov.eresources.mssm.edu) (R01 GM108911) to AS and CG; and T32 CA078207 to RAG; and the R15 GM135843-01 awarded to CG.

© 2023, Dong et al.

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