Juan C Canul-Tec1,2, Reda Assal1,2, Erica Cirri1,2, Pierre Legrand3, Sébastien Brier4,2, Julia Chamot-Rooke4,2, Nicolas Reyes1,2. 1. Molecular Mechanisms of Membrane Transport Laboratory, Institut Pasteur, 25-28 rue du Docteur Roux, 75015 Paris, France. 2. UMR 3528, CNRS, Institut Pasteur, 25-28 rue du Docteur Roux, 75015 Paris, France. 3. Synchrotron SOLEIL, L'Orme des Merisiers, 91192 Gif-sur-Yvette, France. 4. Structural Mass Spectrometry and Proteomics Unit, Institut Pasteur, 25-28 rue du Docteur Roux, 75015 Paris, France.
Abstract
Human members of the solute carrier 1 (SLC1) family of transporters take up excitatory neurotransmitters in the brain and amino acids in peripheral organs. Dysregulation of the function of SLC1 transporters is associated with neurodegenerative disorders and cancer. Here we present crystal structures of a thermostabilized human SLC1 transporter, the excitatory amino acid transporter 1 (EAAT1), with and without allosteric and competitive inhibitors bound. The structures reveal architectural features of the human transporters, such as intra- and extracellular domains that have potential roles in transport function, regulation by lipids and post-translational modifications. The coordination of the allosteric inhibitor in the structures and the change in the transporter dynamics measured by hydrogen-deuterium exchange mass spectrometry reveal a mechanism of inhibition, in which the transporter is locked in the outward-facing states of the transport cycle. Our results provide insights into the molecular mechanisms underlying the function and pharmacology of human SLC1 transporters.
Human members of the solute carrier 1 (SLC1) family of transporters take up excitatory neurotransmitters in the brain and amino acids in peripheral organs. Dysregulation of the function of SLC1 transporters is associated with neurodegenerative disorders and cancer. Here we present crystal structures of a thermostabilized human SLC1 transporter, the excitatory amino acid transporter 1 (EAAT1), with and without allosteric and competitive inhibitors bound. The structures reveal architectural features of the human transporters, such as intra- and extracellular domains that have potential roles in transport function, regulation by lipids and post-translational modifications. The coordination of the allosteric inhibitor in the structures and the change in the transporter dynamics measured by hydrogen-deuterium exchange mass spectrometry reveal a mechanism of inhibition, in which the transporter is locked in the outward-facing states of the transport cycle. Our results provide insights into the molecular mechanisms underlying the function and pharmacology of human SLC1 transporters.
SLC1 transporters constitute a large family of ion-coupled transporters present
in all kingdoms of life1. There are seven human
SLC1 transporters (Extended Data Fig. 1) that
evolved to serve two specialized functions2: in
the central nervous system, SLC1 excitatory amino acid transporters (EAAT1-5) take up
the neurotransmitter glutamate into the cell. In peripheral organs, EAATs take up
glutamate and aspartate, while SLC1 neutral amino acid transporters (ASCT1-2) exchange
small amino acids between the extra- and intracellular compartments, contributing to the
cellular solute homeostasis.
Extended Data Figure 1
Alignment of human SLC1 transporters.
Amino acid sequences of EAAT1-5, ASCT1-2 and EAAT1cryst
are compared. The boundaries of the α-helices (cylinders) in the
TranD (orange) and the ScaD (teal) seen in the EAAT1cryst
structure are shown. In order to confer crystallizability, the region
between TM3 and TM4c (arrows) from ASCT2 was transferred to a thermally
stabilized EAAT1. To further improve crystal formation in the absence of
UPCH101, mutations M231I and F235I (circles) were introduced
to generate EAAT1cryst-II. These substitutions are found in
EAAT2. Other residues involved in UPCH101 coordination are more
conserved (triangles). Sequences were aligned with Jalview59.
Glutamate is the most important excitatory transmitter in the mammalian brain and
it has to be continuously pumped into the cytoplasm to allow for rounds of transmission
and prevent cytotoxicity. This essential neurological function is done by EAAT1-5
expressed at the plasma membrane of astrocytes and neurons3. In particular, astroglial EAAT1 and EAAT2 orthologs are highly expressed
in the hind- and forebrain, respectively, and are responsible for most of the glutamate
uptake in the rodent brain4. EAATs are powerful
molecular pumps capable of maintaining up to 104-fold glutamate gradients by
using energy stored in sodium, proton and potassium gradients5. Remarkably, their dysregulation has been associated with several
neurological diseases, including amyotrophic lateral sclerosis6, ataxia7,8, stroke9,
depression10 and glioma11, making them important drug targets.ASCTs are structurally related to EAATs, and function as sodium-dependent neutral
amino acid exchangers at the plasma membrane12.
Importantly, ASCT2 is up regulated in several forms of cancer, including melanoma13, lung14,
prostate15 and breast cancer16, and it is a key drug target in cancer
therapy.Despite the need for small compounds that selectively and allosterically modulate
SLC1 human transporters, most of their pharmacology is based on substrate-analogs that
inhibit transport competitively17,18. The only known selective allosteric modulators
of SLC1 transporters are a series of non-competitive EAAT1-selective inhibitors, of
which
2-Amino-4-(4-methoxyphenyl)-7-(naphthalen-1-yl)-5-oxo-5,6,7,8-tetrahydro-4H-chromene-3-carbonitrile
(UCPH101) is the best studied19,20. However, its mechanism of
action is still poorly understood at the molecular level.In structural terms, most our knowledge on the transport mechanism and
pharmacology of SLC1 transporters comes from the prokaryotic homolog GltPh that has been
crystallized in the main conformational states of the transport cycle, outward-21 and inward-facing states22,23, as well as in complex
with a non-selective and competitive inhibitor of the EAATs24, DL-threo-β-benzyloxyaspartic acid (TBOA). However, the
presence of amino acid insertions and deletions, as well as important differences in the
transport function and pharmacology of GltPh, make this homolog a limited structural
model to understand the molecular mechanism of the human SLC1 proteins.Here we present 3.1-3.3 Å X-ray crystal structures of thermostable EAAT1
variants in complex with a substrate (L-aspartate), and the allosteric inhibitor
UCPH101. The structures, and supporting functional data, show new
architectural features of the EAATs and ASCTs, and unravel the allosteric mechanism of
UCPH101-like inhibitors in atomic detail. Taken together, these
structural data can prove useful for the design of novel allosteric compounds with
improved selectivity for both EAATs and ASCTs.
EAAT1 engineering and crystallization
Purified wild-type EAAT1 lacks transport activity upon reconstitution in
synthetic liposomes (Fig. 1a), and was
recalcitrant to crystallization. To obtain functional protein suitable for
crystallographic studies, we engineered a thermostable EAAT1, called
EAATcryst that shares an overall ~75% sequence identity with
the wild type, and up to ~90% identity at the C-terminal core of the protein
(Extended Data Fig. 1; Methods), where the transported substrate and coupled ions are
expected to bind24–29. Indeed, purified EAAT1cryst
reconstituted in liposomes showed robust glutamate uptake that depends on opposite
gradients of sodium and potassium ions across the bilayer (Fig. 1a and Extended Data Fig.
2a), and was inhibited by the EAAT1-selective compound UCPH101
(IC50 of 4.5±0.3 μM, Hill coefficient 0.92±0.07)
(Fig. 1b). These data show that the
transport mechanism and pharmacological selectivity are conserved in
EAAT1cryst.
Figure 1
Function and architecture of EAAT1cryst.
a-b, Uptake of radioactive L-glutamate by purified EAAT1 (grey),
EAAT1cryst (blue), and EAAT1cryst-II (red)
reconstituted in liposomes. Transport was abolished when choline
(Ch+) was used in the extra- or intra-liposomal solutions (yellow
circles) (a). UCPH101 inhibits glutamate transport in a
concentration dependent manner (b). Plots depict an average of
three independent experiments performed with duplicate measurements, and error
bars represent s.e.m. c-d, Structure of EAAT1cryst
trimer viewed from the extracellular solution (c) and from the
membrane (d) highlighting the ScaD (teal) and TranD (orange).
e, EAAT1cryst monomer viewed parallel to the
membrane. The ScaD domain is represented as surface (teal), and several helices
and loops in the TranD (orange) have been removed. f, Domain
organization diagram of EAAT1cryst monomer.
Extended Data Figure 2
EAAT1cryst and EAAT1 glutamate uptake.
a, Initial rates of L-glutamate uptake from purified
EAAT1cryst reconstituted in liposomes. The solid line is the
fit of a Michaelis-Menten equation to the data with KM=21
± 10 μM and Vmax= 13 ± 1 pmol
μg-1 protein min-1. The graph is the mean
of three independent experiments, and error bars represent s.e.m..
b, L-glutamate uptake was measured in HEK293 cells
expressing WT EAAT1 (black circles) and a truncated mutant beyond E501 (red
symbols). The initial rate of uptake decreased by ~2-fold in the
EAAT1 truncated mutant. Data were normalized to the asymptotic level of
glutamate uptake based on a monoexponential function. The rates obtained
from the fits were 0.16 ± 0.03 and 0.08 ± 0.03
min-1 for EAAT1 and the truncated mutant, respectively. The
graphs are means of 4 independent experiments done in duplicates. Error bars
represent the s.e.m..
Notably, EAAT1cryst crystallized in the presence of
UCPH101, and we solved its inhibitor-bound structure (see Methods and Extended Data Table 1), but it was refractory to crystallization in the
absence of UCPH101. To overcome this, we introduced M231I and F235I
mutations in the inhibitor-binding pocket (Extended
Data Fig. 1), and solved the crystal structures of the so-called
EAAT1cryst-II both in the presence and absence of the inhibitor
(Extended Data Table 1). Purified
EAAT1cryst-II also showed robust sodium- and potassium-dependent
glutamate uptake, while the UCPH101 IC50 increased
>30-fold (>131±38 μM, Hill coefficient 0.92±0.0;
Fig. 1a,b), as expected due to the
mutations in the inhibitor binding pocket (see below).
Extended Data Table 1
Data collection and refinem ent statistics.
EAATlcrystUCPH101bound
EAATIcryst-IIUCPH101bound
EAATIcryst-II
EAATlcrystUCPH101
andTBOATFBbound
Data collection*
Space group
P63
P63
P63
P63
Cell dimensions
a=b, c
(Å)
123.27, 89.87
123.11, 89.62
123.32, 89.57
124.33, 90.81
α=β, γ
(°)
90.0, 120.0
90.0, 120.0
90.0, 120.0
90.0, 120.0
Wavelength
0.979
0.976
1.009
0.977
Resolution (Å)
34.50-3.25 (3.34-3.25)
45.82 -3.1 (3.18-3.1)
45.87-3.32 (3.41-3.32)
46.31-3.71 (3.81-3.71)
Anisotropy direction$Resolution
whereCC1/2 >0.3
Overall (Å)
3.37
3.1
3.32
3.71
along h, k axis (Å)
3.75
3.68
3.85
4.35
along l axis (Å)
3.25
3.1
3.32
3.71
Measured reflections
333978 (24261)
290672 (21906)
326273 (21829)
141904 (11176)
Unique reflections
12338 (902)
14115 (1 032)
11556 (834)
8570 (628)
Completeness (%)
100 (100)
99.9 (99.9)
100 (100)
99.9 (100.0)
Mn (I) half-set correlation
0.99 (0.22)
1 (0.43)
0.99 (0.31)
0.99 (0.373)
I/σ(I)
11.7 (0.7)
15.8 (0.8)
13 (0.7)
12.1 (0.9)
Rmerge
0.19 (6.8)
0.1 (6.71)
0.15 (8.03)
0.14 (3.71)
Redundancy
27.1 (26.9)
20.6 (21.2)
28.2 (26.2)
16.3 (14.3)
StructuredeterminationRefinement
Resolution cut-off (Å)
34.50-3.25
45.80-3.10
20.00-3.32
25.00-3.71
No. of Work / Test reflections
9888/474
10725/528
9251/445
6860/684
Rcrvst (%) /
Rfree (%)
216/23.5
21.7/25.9
20.9/25.3
22.7/25.4
No. of protein atoms
3008
2960
2995
3008
No. of
heteroatomsB factors
(Å)2
42
42
10
62
Protein
126.2
111.8
137.0
135.5
Heteroatoms
123.5
99.5
125.6
132.7
R.m.s. deviations from ideal
Bond
lengths (Å)
0.009
0.01
0.009
0.009
Bond
angles (°)
1.06
1.12
1.05
1.03
One crystal was used to collect diffraction datasets for each
structure, except in the EAAT1cryst UCPH101 and
TFB-TBOA bound structure, where datasets from three crystals were
merged.
5% of reflections were used for calculations of
Rfree, except for the EAAT1cryst UCPH101-TBOATFB
bound structure where 10% was used due to the lower number of total reflections.
Values in parentheses are for the highest-resolution shell.
The anisotropy directions where computed with AIMLESS.
Domain organization
The structure of EAAT1cryst shows a symmetric homotrimer in a
substrate- and UCPH101-bound outward-facing conformation (Fig. 1c-e) with an overall GltPh-like fold21,22
(Extended Data Fig. 3). Each monomer is
composed of two domains: a scaffold domain (ScaD), including transmembrane helices
TM1-2 and TM4-5; and a transport domain (TranD), including TM3, TM6-8 and re-entrant
helical loops 1-2 (HP1-2; Fig. 1f). The three
ScaDs form a compact central structure with a propeller-like shape that ensures the
trimeric form of the transporter and anchors it to the membrane (Extended Data Fig. 4). The three TranDs are more
peripheral and localize between the blades of the propeller, making protein contacts
exclusively with the ScaDs of their own monomer. The TranD-ScaD interface buries
~3,500 Å2, including a conserved salt bridge between E256
and K364, through interactions of residues in the cytoplasmic parts of HP1, TM7, and
TM3 (TranD), and TM2, TM4c, and TM5 (ScaD). On the extracellular side, additional
contacts occurred between residues in HP2 and TM4 that are well conserved among
human transporters (Extended Data Fig. 5).
Extended Data Figure 3
EAAT1cryst and GltPh structural comparison.
a-b EAAT1cryst aligns to a monomer of GltPh
(PDB 2NWL) with α-carbon r.m.s.d. of 1.4 Å. The ScaDs
(EAAT1cryst teal, and GltPh purple, a), and
TranDs (EAAT1cryst orange and GltPh, purple, b) are
shown separately for clarity of display.
Extended Data Figure 4
EAAT1cryst trimeric interface.
a-b, Interface of three ScaDs of the
EAAT1cryst UCPH101-bound structure viewed from the
extracellular side (a) and from the membrane (b).
The TranDs are not shown. The ScaD of one monomer (black) buries 3,000
Å2 in the trimerization interface through extensive
contacts with the two other subunits (teal and purple surfaces), including
six intermolecular salt bridges (shown as green sticks for the monomer in
black). The surface area in the other two monomers is colored in light pink.
Only residues that contribute ≥ 10 Å2 of buried
surface area are highlighted.
Extended Data Figure 5
TranD-ScaD interface.
a-b, EAAT1cryst monomer viewed from the
membrane (solid black line). Residues in the TranD (colored black) bury
1,760 Å2 at the interface with the ScaD (a).
This interface extends to the extracellular side of the transporter through
interactions between HP2-TM4 (sticks and pseudo-transparent spheres)
(b). c, Cytoplasmic view of the monomer
displaying the salt bridge between TM7 and TM5.
Substrate and ion translocation in SLC1 transporters is thought to occur
through large rigid-body movements of the TranD, relative to the static ScaD, that
move the cargo in an elevator-like fashion across the membrane22,30. Thus, during the
isomerization to the inward-facing state the TranD-ScaD interface changes
drastically on the TranD side, and the novel features observed at this interface in
EAAT1cryst might influence the distinct TranD dynamics in human SLC1
proteins.
Transport domain
One of the most remarkable architectural features of the
EAAT1cryst TranD is in TM8, where there are deletions and insertions
compared to prokaryotic homologs (Fig. 2 and
Extended Data Fig. 3). In
EAAT1cryst, TM8 can be divided into extracellular (TM8a),
transmembrane (TM8b), and cytoplasmic (TM8c) helices. The loop connecting TM8a and
HP2 is six residues shorter in human SLC1 transporters, and brings their
extracellular ends in close contact through hydrogen bonding and hydrophobic
interactions (Fig. 2). HP2 is a dynamic element
that controls the access of substrate and ions to their binding sites in the
TranD24,31–33, and its
interactions with TM8b likely play an important role in determining HP2 movements.
Consistently, single-cysteine mutations at positions along TM8a in EAAT134, and in a rodent EAAT2 ortholog35 impaired glutamate transport, highlighting
the significance of this extracellular region for function.
Figure 2
Transport domain.
EAAT1cryst TranD with substrate (spheres) and one sodium ion (purple
spheres) bound. Omit Fo-Fc densities contoured at 2.3 σ (black mesh) show
the position of the ligands. TM8a-c (blue) interacts with other regions on the
TranD (orange), including HP1 (left inset), HP2 (upper right inset), and TM3 and
TM7 (lower right inset).
In TM8b, we found strong electron density for the substrate (L-aspartate)
and one of the sodium ions (Na2) in similar sites than in the structures of
prokaryotic homologs24,29 (Fig. 2). Remarkably,
the carboxylate group of D456 (TM8b), which coordinates the α-amino group of
the substrate, is also at hydrogen bond distance with the hydroxyl group of S343
(HP1). Moreover, the guanidinium group of R457 (TM8b) engages in hydrogen bonding
with HP1 residue G341, and possibly L340 and T342 that point their backbone carbonyl
oxygen atoms towardsTM8b. Residues S343 and R457 are well conserved in human SLC1
transporters, and substitutions at equivalent positions in EAAT1 (S363 and
R477)36, and EAAT3 (R445)37 inactivate transport. In addition, the
loss-of-function mutation R445W in EAAT3, equivalent to R457 in
EAAT1cryst, causes human dicarboxylic aminoaciduria38. Overall, the functional studies and our
structural data converge to suggest that interactions between conserved human
residues at HP1 and TM8b are important to the correct folding and function of the
transporters.On the cytoplasmic side, TM8 extends beyond the membrane through a
hydrophilic helix (TM8c) that makes contact with TM3 and TM7a (Fig. 2). EAAT2 deletion mutants in this region have a
deleterious effect on transport function and membrane trafficking39. Accordingly, an EAAT1 deletion in TM8c
decreased glutamate uptake rate by ~2-fold (Extended Data Fig. 2b). Indeed, the functional data and the TM8c amino
acid conservation among EAATs underscore the pivotal role of this novel structural
motif in protein folding and transport kinetics.
Scaffold domain
The ScaD contains highly divergent regions, especially in TM4 (Extended Data Fig. 1), where
EAAT1cryst shows several unique architectural features. On the
extracellular side, TM4a forms inter- and intra-monomeric contacts with TM2 and HP2,
respectively. Moreover, an amino acid insertion between TM4b and TM4c (TM4b-c loop)
that appeared during the evolution of eukaryotic transporters protrudes into the
central vestibule of the EAAT1cryst trimer (Fig. 3a and Extended Data Fig. 4).
The TM4b-c loop forms the center of the propeller, and makes extensive contacts
within and between protomers. Although, we could not model the outermost residues in
the TM4b-c loop (Y200-V210), they are expected to each out to the bulk solvent
exposing an N-glycosylation site (N204). Notably, all human SLC1 transporters
contain predicted N-glycosylation sites in the TM4b-c loop, suggesting a conserved
role of this loop in the posttranslational processing of these proteins.
Figure 3
Scaffold domain.
a, TM4 (purple) makes extensive contacts with the ScaD of the
neighboring monomer (monomer 2, teal surface), and the TranD (orange) of the
same subunit (monomer 1). The TranD of monomer 2, and several TMs of monomer 1
were removed for clarity of display. Fo-Fc density in the HP2-TM4 crevice is
contoured at 2.7σ (red mesh). b, Two monomers of
EAATcryst show TM1a laying parallel to the membrane. The third
monomer is not shown. TM1 (teal) and HP1a (dark blue) form a hydrophobic crevice
containing non-protein Fo-Fc density (purple mesh, contour 2.7σ).
On the cytoplasmic side, TM1 bends and re-orients its N-terminal part (TM1a)
nearly parallel to the membrane plane, which forms the tips of the
propeller’s blades (Fig. 1c and Fig. 3b). The position and amphipathic nature of
TM1a suggests that it somehow interacts with the inner leaflet of the membrane.
Consistently, in the hydrophobic crevice between TM1a and HP1a, we observe strong
non-protein electron density that likely corresponds to bound detergent or lipid
molecules (Fig. 3b). Interestingly, a second
hydrophobic crevice between the extracellular part of TM4 and HP2, also shows strong
non-protein electron density (Fig. 3a). A
similar crevice was also noted in a substrate-bound structure of GltPh21.Lipids strongly regulate SLC1 transport function40–44, and those
hydrophobic crevices at the interface between the TranD and ScaD, where large
conformational changes occur during substrate translocation, might constitute sites
for lipid regulation of transport function.
UCPH101 binding site
The structure of EAAT1cryst showed strong electron density for
UCPH101 in a hydrophobic pocket between TM3, TM7 and TM4c at the
TranD-ScaD interface, where the compound extends the interface by ~ 500
Å2 (Fig. 1d,e and Fig. 4a,b). The chromene skeleton, the parental
group of the UCPH series of compounds, is buried deeply in the domains interface,
and coordinated by a direct ring-stacking interaction with F369 (TM7a), as well as
hydrophobic interactions with G120 (TM3), V373 (TM7a) and M231 (TM4c) (Fig. 4b). In addition, the amine group of
UCPH101 forms a hydrogen bond with the main-chain carbonyl of F369,
while its carbonitrile group interacts with Y127 (TM3). The methoxy-phenyl and
naphthalene groups appear partially facing the hydrocarbon core of the membrane.
Yet, the former establishes hydrophobic interactions with V124 (TM3), V373 and M231,
while the latter is mainly coordinated by F235 (TM4c). The majority of the
above-mentioned residues are important for UCPH101 transport inhibition
of an EAAT1 rodent ortholog20. Furthermore,
the M231I-F235I double mutant (EAAT1cryst-II) showed >30-fold
increase in UCPH101 IC50 compared to EAAT1cryst in
proteo-liposomes (Fig. 1b). Hence, there is an
excellent agreement between the crystallographic and functional data.
Figure 4
UCPH101 binding site.
a, Lateral view of EAAT1cryst monomer showing
UCPH101 bound (pink) between the TranD (orange) and ScaD (teal).
b-c, UCPH101 coordination and Fo-Fc densities
contoured at 2.0σ (blue mesh) in EAAT1cryst (b)
and EAAT1cryst-II (c), respectively. Side chains of
residues in TM3, TM4c, and TM7 involved in coordination are shown. F369 side
chain moves outward in the EAAT1cryst-II unbound state (grey)
(c).
Several mechanistically-relevant observations can be made regarding the
UCPH101 binding pocket in EAAT1cryst: i) it is over 15
Å away from the substrate and sodium binding sites, suggesting that
UCPH101 does not preclude extracellular substrate binding; ii) it
faces the inner leaflet of the membrane, implying that UCPH101 accesses
its binding site from the lipidic, and not the aqueous phase, when applied
extracellularly; iii) it is fully contained in a single subunit, in agreement with
the lack of cooperativity observed in proteo-liposome (Fig. 1b), and cell assays20; iv)
a comparison of the EAAT1-5 sequences suggests that the main determinants of
UCPH101 selectivity for EAAT1 are in TM4c, where M231 and F235 are
the only coordinating residues that differ between EAAT1 and all other EAATs (Extended Data Fig. 1). Consistently, the double
mutant EAAT1cryst-II containing EAAT2 residues equivalent to M231-F235 shows a large
IC50 increase.
UCPH101-unbound state
To better understand the conformational changes of the transporter induced
by UCPH101, we set out to determine the structure of the
EAAT1cryst UCPH101-unbound state, but it was refractory to
crystallization. Instead, we solved the structure of the EAAT1cryst-II
UCPH101-unbound state and for comparison, the
EAAT1cryst-II UCPH101-bound state, using an excess of the
compound in the crystallization conditions (see Methods).The EAAT1cryst-II UCPH101-bound state is nearly
identical to that of the EAAT1cryst with the exception of the I231 and
I235 side chains, and a ~2 Å movement of UCPH101methoxy-phenyl and naphthalene groups away from them (Fig. 4c and Extended Data Fig.
6a). However, the EAAT1cryst-II UCPH101-unbound
structure shows notable differences with bound state. First, there is no excess
electron density for UCPH101, and the side chain of F369 moves outward by
as much as 1.9 Å, partly occupying the volume of the UCPH101chromene group (Fig. 4c). Second, there is a
small rigid-body movement of the entire TranD that shifts by as much as 0.7
Å, compared to the UCPH101-bound structures (Extended Data Fig. 6b). This conformational change shows the
EAAT1cryst TranD is able to move as rigid bodies relative to the
ScaD, and highlights the importance of such movements for the function of the human
transporters, as it has been shown for GltPh22,23.
Extended Data Figure 6
Superposition of EAAT1cryst and EAAT1cryst-II
structures.
a-b, The transport domains of EAAT1cryst
(teal) and EAAT1cryst-II (pink) UCPH101-bound
structures superimpose accurately after aligning their scaffold domains
(a). The overall α-carbon r.m.s.d. was 0.3 Å.
However, the same alignment done with EAAT1cryst-II
UCPH101-bound and -unbound structures shows a small but
global movement of the transport domain (b), with a small
increase in the overall α-carbon r.m.s.d. of 0.1 Å.
c,d Anomalous difference Fourier maps contoured at the
2.8σ (pink mesh), from data collected at low
energy X-rays (1.77 Å), show the correct sequence registry in both
the TranD (orange, a) and the ScaD (teal, b).
The structural changes observed in the UCPH101-unbound structure
unambiguously demonstrate that the assigned binding pocket of UCPH101 is
correct, and that within the restricted environment of the crystal lattice,
UCPH101 induces both local and global conformational changes of the
transporter that optimize its coordination in an outward-facing state.
Transport domain dynamics
The coordination of UCPH101 in the crystal structures, wedged in
the TranD-ScaD interface, as well as the effect of the M231I-F235I mutations on its potency
strongly suggest that UCPH101 inhibits transport by trapping the
transporter in an outward-facing state. Consistently, the rigid-body movements of
the TranD to isomerize the transporter into the inward-facing state would separate the coordinating
residues in the TranD from those in the ScaD, and disrupt the UCPH101
coordination. Hence, under equilibrium conditions where the transporters are
sampling outward- and inward-facing states, the expected effect of
UCPH101 binding is to shift the equilibrium in favor of the
outward-facing state.To gain insights into the effects of UCPH101 binding to the
transporters at equilibrium, we probed the detergent solubilized
EAAT1cryst by hydrogen-deuterium exchange mass spectrometry (HDX-MS).
HDX-MS measures the rate of exchange of backbone amidehydrogen atoms that depends
on solvent accessibility and hydrogen bonding, and provides valuable information on
the dynamics and conformational changes of proteins45,46.We compared the HDX behavior of the EAAT1cryst in the presence
and absence of UCPH101. Overall, the deuterium uptake pattern of
EAAT1cryst shows dynamic structural elements in both the TranD and
ScaD (Extended Data Fig. 7-8), and reveals the unstructured and
solvent-exposed nature of several regions that were not resolved in the crystal
structures, including the TM3-TM4a (peptide 153-173) and TM4b-c (peptide 200-208)
loops, as well as the N- (peptide 1-28) and C-termini (peptides 490-522) (Extended Data Fig. 9).
Extended Data Figure 7
Peptide coverage map of EAAT1cryst.
A total of 111 peptides covering 76.3% of the EAAT1cryst
sequence were identified by data independent MS/MS acquisition after 2 min
digestion with immobilized pepsin. Each bar below the EAAT1cryst
sequence corresponds to a unique peptide. The 57 peptides colored in blue
were further selected for HDX-MS data extraction and analysis. The two
additional N-terminal residues (i.e., GP) that remain after
protein purification are also shown. The transmembrane helices (TM) of the
TranD (orange) and the ScaD (cyan) are indicated above the sequence.
Extended Data Figure 8
UCPH101 effect on the local hydrogen exchange behavior of
EAAT1cryst.
a, HDX profiles of EAAT1cryst (see Methods) in the apo (upper panel) and
UCPH101-bound state (middle panel). The relative fractional
uptake determined for each peptide and at each time point is plotted as a
function of peptide position. The black to red lines correspond to data
acquired from 10 sec up to 1h, respectively. b, The fractional
uptake difference plot was generated by subtracting the deuterium uptake
values in the UCPH101-unbound from those in the bound state.
Negative uptake difference indicates UCPH101-induced decrease in
amide hydrogen exchange. Each dot corresponds to an average of three
independent HDX-MS experiments. The four regions (labeled 1 to 4) showing a
statistically significant modification (p <0.01) of
deuterium uptake upon binding of UCPH101 are highlighted in
grey.
Extended Data Figure 9
HDX-MS results mapped on the crystal structure of ScaD and TranD of
EAAT1cryst in the unbound and UCPH101-bound
state.
The color code at the bottom shows the average relative fractional
uptake measured in both domains after 10 sec (upper panel), 10 min (middle
panel) and 1h (lower panel) labeling. Missing regions in the crystal
structure are represented by dashed lines. Peptides showing a statistically
significant (p <0.01) modification of deuterium
uptake upon UCPH101 binding are labeled. Uncovered regions are
colored in light blue.
Binding of UCPH101 significantly decreased deuterium uptake in
several areas of the TranD including its binding pocket (residues 112-123 and
370-374), and the surrounding area (residues 354-369), while it left the uptake in
the ScaD unchanged (Fig. 5a). It also decreased
deuterium uptake in distant residues (336-349 and 420-430) at the tips of HP1 and
HP2 involved in substrate coordination and occlusion, suggesting that
UCPH101 induces conformational changes in the transporter upon
binding. To gain insights into the nature of those conformational changes, we first
compared the TranD areas in which UCPH101 decreased uptake with those
buried at the interface with ScaD in the EAAT1cryst structure, and found
that they correlate remarkably well (Fig.
5a-c). Second, we built a model of the EAAT1cryst inward-facing
state, based on a recently solved structure of GltPh23, to assess the changes in solvent accessibility in a possible
transition between inward- and outward-facing states (Fig. 5c,d). Indeed, the comparison between the structure and the model
shows that the UCPH101-modified areas detected by HDX-MS transit as rigid
bodies from being solvent-exposed, in the inward-facing state, to buried at the
TranD-ScaD interface, in the outward-facing state. Such conformational change is
expected to decrease the dynamics of alpha helices and/or the solvent accessibility
of the loops in the UCPH101-modified areas and thus, is consistent with
the observed decrease in deuterium uptake. Overall, the HDX-MS and structural
analysis support the stabilization of the outward-facing state, at the expense of
the inward-facing state(s), induced by UCPH101.
Figure 5
Transport domain dynamics.
a, UCPH101 decreased deuterium uptake in several regions
(black) of the TranD at the interface with the ScaD. The alpha carbon atoms
delimiting such regions are shown as black spheres. Unaffected regions of the
TranD (orange) or those not detected during HDX-MS analysis (grey) are also
highlighted (sequence coverage ~77%). b, TranD residues
buried at the interface with the ScaD, in the UPCH101-bound
outward-facing state, are colored dark blue for comparison with
(a). c-d, Comparison between EAAT1cryst
structure in the UPCH101-bound outward-facing state (c)
and a model of an inward-facing state based on the GltPh
“unlocked” state (PDB 4X2S) (d), in which the TranD
(color code as in a) undergoes a large rigid body movement towards
the cytoplasm.
UCPH101- and TBOATFB-bound state
The distant position of UCPH101 from the substrate and HP2, a
structural element that controls extracellular access to the substrate binding
site24, suggests that the
UCPH101-bound transporters could undergo the conformational changes
required to exchange the substrate with the extracellular solution. To test this, we
solved the crystal structure of EAAT1cryst in complex with both
UCPH101 and
(2S,3S)-3-[3-[4-(trifluoromethyl)benzoylamino]benzyloxy]aspartate
(TBOATFB), a potent and non-selective TBOA derivative47, at 3.7 Å resolution (Extended Data Table 1).Overall, the UCPH101-TBOATFB-bound structure is
similar to that of the UCPH101-bound state, with the exception of HP2
that adopts an “open” conformation and packs against the TM4b-c loop,
disrupting the coordination of the Na2 (Fig.
6a,b). These conformational changes resemble those previously observed in
the structure of the GltPh-TBOA complex, and are in excellent agreement with the
proposed competitive inhibitory mechanism of TBOA-like compounds24.
Figure 6
UCPH101-TBOATFB bound EAAT1cryst
structure.
a, The movement of HP2 (purple) partly exposes the substrate-binding
pocket to the solvent and shows a molecule of TBOATFB (purple sticks)
bound to it. UCPH101 is also observed in this structure (pink
sticks). b, The tip of HP2 moves as much as 9.5 Å in the
UCPH101-TBOATFB- (purple), compared to the
UCPH101-substrate bound (orange) structures, placing the carbonyl
oxygen of A420 away from Na2 (green sphere). c, Omit map Fo-Fc
density for the TBOATFB molecule is contoured at 2.3σ (black
mesh), and some of the residues at Van deer Waals or H-bond distance from the
compound are represented as sticks.
In the substrate-binding site, we observed excess electron density for the
bulky TBOATFB (Fig. 6c), but due to
lack of resolution, we were not able to unambiguously orient the compound. Hence, we
initially positioned the TBOA moiety of TBOATFB using the TBOA-bound
GltPh structure as a guide. After crystallographic refinement, the additional
benzoylamino and trifluoromethyl groups of TBOATFB in
EAAT1cryst localized in a hydrophobic cavity mainly formed by
residues in HP1b and TM7a, and possibly by residues in TM2 and TM4c, likely
explaining the observed ~1500-fold increase in EAAT1 inhibitory potency over
TBOA47.Indeed, in the TBOATFB-bound structure UCPH101 is
bound with an identical coordination than in the substrate-bound state. Therefore,
the EAAT1cryst structures show that UCPH101 binding at its
allosteric site does not preclude the movements of HP2 involved in substrate and
sodium binding from the extracellular solution.
Inhibitory mechanisms of EAAT1
The structural and functional EAAT1cryst data reveal new
architectural features of human SLC1 transporters, and their first molecular
mechanism of allosteric inhibition. UCPH101 binding “glues”
the TranD to the ScaD in the outward-facing states, and precludes substrate
translocation, but not binding from the extracellular solution (Fig. 7). Non-conserved residues in the ScaD determined
UCPH101 selectivity for EAAT1. This inhibitory mechanism contrasts
with that of substrate-analog inhibitors like TBOA. The binding pocket of TBOA-like
compounds overlaps with the conserved substrate binding site24, explaining their lack of selectivity among glutamate
transporters and the inhibition of substrate binding observed on either side of the
membrane48,49.
Figure 7
EAAT1 inhibitory mechanisms.
Schematic representation of TBOA-like competitive and UCPH101-like
allosteric inhibition. Competitive inhibitors, occupy the substrate-binding
pocket and preclude substrate binding. UCPH101-like compounds bind at
the TranD-ScaD interface and block the movement of the TranD (orange) relative
to the ScaD (teal).
The unique inhibitory mechanism of UCPH101 makes it an extremely
valuable pharmacological tool to study the conformational changes that EAAT1
undergoes upon substrate and ion binding. Remarkably, the UCPH101
allosteric binding site highlights a cavity that can facilitate the design of
selective compounds for other human SLC1 transporters, and possibly the long-sought
positive modulators of glutamate uptake.
Methods
Construct optimization
We used fluorescence-detection size-exclusion chromatography (FSEC)50 to screen solubilization conditions and
EAAT1 variants fused to enhanced green fluorescent protein (eGFP). EAAT1N-terminal fusions solubilized in dodecanoyl sucrose (DDS, Anatrace) were found
to have good solubility and mono-dispersity by FSEC in clear lysates. However,
EAAT1 looses its transport activity and chromatographic monodispersity upon
purification. To increase its stability, we used consensus mutagenesis51, and screened EAAT1 variants with
different consensus mutations in the predicted transmembrane helices by FSEC.
The apparent melting temperature (Tm) of the most stable EAAT1 construct was
>20 °C over that of the wild-type EAAT1, but the
mutated transporter was still refractory to crystallization. We reasoned that
the divergent extracellular region between TM3-4c could interfere with
crystallization, and changed it for the equivalent region in ASCT2, the shortest
one among human SLC1 members (Extended Data
Fig.1). In addition, we mutated the two predicted N-glycosylation
sites of the transporter (N155T and N204T mutations) to further improve
crystallizability.
Expression and purification
All constructs were introduced into pcDNA3.1(+) (Invitrogen) with
N-terminal Strep-tag II affinity tag followed by eGFP and PreScission protease
cleavage site, and expressed in HEK293F cells (ATCC, mycoplasma test negative)
grown in Excell293 medium (Sigma) and supplemented with 4mM L-glutamine (Sigma)
and 5µg/ml Phenol red (Sigma-Aldrich) to densities of 2.5 x
106 cells ml-1. Cells were transiently transfected in
Freestyle293 medium (Invitrogen) using poly-ethylenimine (PEI) (Polysciences) at a
density of 2.5 x 106 cells ml-1, diluted with an
equivalent volume of Excell293 6 hours post-transfection, and treated with 2.2
mM valproic acid (Sigma) 12 hours after dilution of the cultures. Cells were
collected at ~48 h post-transfection.Initial screens of constructs and detergent solubilization buffers were
done in small-scale (5-10 ml), and cells were collected, mechanically disrupted
with a douncer and solubilized in 50 mM HEPES/Tris-base, pH 7.4, 200 mM NaCl
buffer supplemented with 1 mM L-asp, 1 mM EDTA, 1 mM Phenylmethylsulfonyl
fluoride (PMSF), 1 mM Tris(2-carboxyethyl)phosphine (TCEP), 1:200 (v/v) dilution
of mammalian protease inhibitor cocktail (Sigma), 10 % glycerol, 2% detergent
and 0.4% cholesterol hemisuccinate (CHS) (Anatrace). After 1-hour incubation at
4 °C, clear lysates were obtained by ultracentrifugation
(247,000 g for 45 min). A high-throughput auto-sampler was used to inject the
lysates in a SRT SEC-500 column (Sepax Technologies) equilibrated in 50 mM
HEPES/Tris-base, pH 7.4, 200 mM NaCl buffer supplemented with 1 mM L-asp, 1 mM
(TCEP), 5 % glycerol, 3 x CMC detergent, and ~0.01% CHS, in line with
fluorescence detection (Photon technology international) for FSEC analysis.Large-scale expression was done in 2-4 l cultures with cells collected
in 50 mM HEPES/Tris-base, pH 7.4, 50 mM NaCl buffer supplemented with 1 mM
L-asp, 1 mM EDTA, 1 mM PMSF, 1 mM TCEP, and 1:200 (v/v) dilution of mammalian
protease inhibitor cocktail (Sigma), and disrupted in an cell homogenizer
(EmulsiFlex-C5, Avestin) after 3 runs at 15,000 Psi. The resulting homogenate
was clarified by centrifugation (4,500 g, 0.5 h) and the crude
membranes were collected by ultracentrifugation (186,000 g for 1.5 h). Membranes
were washed once with the above-mentioned buffer and finally homogenized with a
douncer in a buffer containing 50 mM HEPES/Tris-base, pH 7.4, 200 mM NaCl, 1 mM
L-asp, 1 mM EDTA, 1 mM TCEP, and 10% Glycerol, snap-frozen in liquid
N2 and stored at -80°C at 0.5 g of membranes
ml-1.Membrane solubilization was done by thawing out and supplementing the
membrane homogenate with 2% DDS, 0.4% CHS, and 25 μM UCPH101
(Abcam). After 1-hour incubation, the insoluble material was removed by
ultracentrifugation (186,000g for 1 h), and Strep-Tactin
sepharose resin (GE Healthcare) was added to the supernatant and rotated for 2
h. Resin was washed with 25 column volumes of 50 mM HEPES/Tris-base, pH 7.4, 200
mM NaCl, 1 mM L-asp, 1 mM TCEP, 5% Glycerol, 0.05% DDS, 0.01% CHS and 25
μM UCPH101, and the protein was eluted with the same buffer
supplemented with 2.5 mM D-desthiobiotin.The eluted eGFP-transporter fusion was concentrated to 1-2 mg
ml-1 using 100-kDa cutoff membranes (Millipore), and digested
with His-tagged PreScission protease overnight at 4 °C. The protease was
removed by reverse Ni-NTA (Qiagen) affinity chromatography, and the flow through
containing the transporter was concentrated to 500 μl, ultra-centrifuged
(86,900 g, 20 min), and applied to a Superose 6 10/300 gel
filtration column (GE Healthcare) equilibrated with 50 mM HEPES/Tris-base, pH
7.4, 200 mM NaCl, 1 mM L-asp, 1 mM TCEP, 5% Glycerol, 0.25% decanoyl sucrose
(DS, Sigma), 0.05% CHS and 100 μM UCPH101. To obtain the
UCPH101 unbound structure, the protocol was identical, but the
allosteric inhibitor was omitted from all buffers. To obtain the
UCPH101-TBOATFB bound structure, the protein sample
was supplemented with 3 mM TBOATFB (Tocris) before the injection in
the gel filtration column equilibrated with 50 mM HEPES/Tris-base, pH 7.4, 200
mM NaCl, 1 mM TCEP, 5% Glycerol, 0.25% decanoyl sucrose (DS, Sigma), 0.05% CHS,
300 μM TBOATFB and 100 μM UCPH101.Protein samples after the solubilization step were kept on ice or at 4
°C at all times.
Crystallization and structure determination
Purified protein was concentrated to 3.5-4.0 mg ml-1 and 1 mM
UCPH101 was added in experiments with the inhibitor-bound
transporters. Initial vapor diffusion crystallization screens were done by
mixing 300 nl of protein and reservoir solution in sitting drops, dispensed by a
Mosquito robot (TTP labtech) in 96-well Greiner plates. The purified
transporters form three-dimensional crystals in several conditions containing
low molecular weight polyethylene glycols. The best-diffracting crystals were
obtained after manual optimization using 1.6 μl hanging drops at 4
°C, obtained by mixing equal volumes of protein supplemented with 0.2%
n-Octyl-b-D-glucopyranoside (BOG, Anatrace) and 0.04% CHS, and reservoir
solutions containing 100 mM Tris, pH 8.2, 50 mM CaCl2, 50 mM
BaCl2, and 28-30% PEG 400. Crystals appeared after 24-48 h and
reached their maximum size after a week. Crystals were flash-frozen in liquid
nitrogen before X-ray diffraction data collection without any further cryo
protection.X-ray diffraction data were collected at beamlines PROXIMA-1 at the
SOLEIL synchrotron (St Aubin, France) and at beamlines at the European
Synchrotron Radiation Facility (Grenoble, France). In general, 2-3 data sets
from single crystals were collected, and indexed, integrated, scaled and merged
using XDS package52. Due to the
anisotropic nature of the diffraction data, the DEBYE and STARANISO programs
were applied to scale it using the STARANISO server (http://staraniso.globalphasing.org/). The software performs an
anisotropic cut-off of merged intensity data with a Bayesian estimation of the
structure amplitudes, and applies an anisotropic correction to the data. Table 1
shows the refinement statistics for the full sets of reflections truncated at
the best high-resolution along h, k or l axis, values given by AIMLESS53, before the anisotropic corrections
computed by the STARANISO software. The corrected anisotropic amplitudes were
then used for molecular replacement in PHASER54, using the scaffold and transport domains of GltPh (PDB code
2NWL) as independent search models. The initial electron density maps were
clearly interpretable, and the final model was obtained through rounds of manual
building in COOT55 and refinement in
Buster56, until reaching good
crystallographic statistics and stereochemistry (Extended Data Table 1). The model contains one EAAT1cryst
monomer per asymmetric unit and most of the EAAT1cryst polypeptide
(residues 37-487), with the exception of some residues in the extracellular
loops between TM3-4a, TM4b-4c, TM5-6 and TM7b-HP2a. Sequence assignment was
aided by anomalous difference Fourier maps from diffraction data collected with
low energy X-rays (1.77 Å) to highlight the sulfur atoms of methionine
and cysteine residues (Extended Data Fig.
6c,d). EAAT1cryst-II, as well as the EAAT1cryst
UCPH101-TBOATFB bound structures were solved by the
same approach above mentioned, but using the EAAT1cryst TranD and
ScaD as independent search models for molecular replacement.The stereochemical properties of the final models were analyzed with the
Molprobity server (http://molprobity.biochem.duke.edu/). At least 95% of the
residues in all models are in the Ramachandran favored region. Protein
interfaces were analyzed with the PISA server (http://www.ebi.ac.uk/msd-srv/prot_int/pistart.html). Structural
alignments were done with Superpose in the CCP4 suite. All structural figures
were prepared with PyMOL Molecualr Graphics System, Schrodinger, LLC.
Radioactive substrate transport assays
Unilamellar liposomes were made at 9:1 molar ratio of
1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (Avanti Polar Lipids) and CHS,
in a buffer containing 50 mM HEPES/Tris-base, pH 7.4, 200 mM NaCl and 1 mM
L-asp. The transporters were purified as described above, but excluding the
reverse chromatography step after protease cleavage, and using a Superose 6
10/300 column equilibrated with 50 mM HEPES/Tris-base, pH 7.4, 200 mM NaCl, 1 mM
L-asp, 0.5 mM TCEP, 0.0632% DDS, 0.01264% CHS, and 5% glycerol.To reconstitute the protein, liposomes were first mixed with DDS at a
1:2 (w/w) lipid-to-detergent ratio for 1 h, and then the purified transporters
were added at a 1:40 (w/w) protein-to-lipidratio. Detergent removal was done at
4° C using SM-2 biobeads (BioRad) at 100 mg ml-1. The internal
solution of the liposomes was exchanged using 10 freeze-thaw cycles in the
appropriate buffer. After extrusion through 400-nm polycarbonate membranes
(Avanti Polar Lipids), the proteoliposomes were concentrated by
ultracentrifugation (150,000 g for 30 min at 4°C) and resuspended at 20
mg of lipids ml-1, for immediate use.Substrate transport was assayed at 37°C. The uptake reaction was
initiated by diluting the proteo-liposomes 10-fold into a buffer containing 50
mM HEPES/Tris-base, pH 7.4, 200 mM NaCl, 50 µM L-glutamate, and 5
µM [14C]-L-glutamate (PerkinElmer), and 2.5% glycerol. After
30 min, 200-µl aliquots were diluted 5-fold into ice-cold quench buffer
(50 mM HEPES/Tris-base, pH 7.4, 200 mM ChCl, and 2.5% glycerol), followed by
immediate filtration and wash on nitrocellulose 0.22-µm filters
(Millipore). Radioactivity was quantified by liquid scintillation using a
Tri-Carb 3110TR counter (PerkinElmer). For the UCPH101 titrations,
proteo-liposomes were both pre-incubated for 20 min at room temperature, and
assayed in the presence of UCPH101. Background radioactivity was
estimated from protein-free liposomes, and subtracted from the uptake data. Data
was fitted to a Hill equation of the form:F=F∞ +
ΔF∞/(1+(IC50/[UCPH101])n)Where F∞ is the final level of inhibition,
ΔF∞ is the final amplitude of the
UCPH101 effect, and n is the Hill coefficient.To titrate the rate of L-glutamate transport by EAAT1cryst,
proteo-liposomes were assayed in the presence of 0, 5, 50 or 200 μM
L-glutamate supplemented with 1, 5, 5, or 5 μM
[14C]-L-glutamate, respectively. At each substrate concentration, the
initial rate of transport was calculated by a linear fit to 120 s and 180 s
uptake measurements with origin fixed at zero. Background radioactivity was
estimated from protein-free liposomes, and subtracted from the uptake data.For the cell-based transport uptake, cells were collected 36 h
post-transfection, and washed three times and resuspended at a density of 50 x
106 cells ml-1 in 11 mM HEPES/Tris-base, pH 7.4, 140
mM ChCl, 4.7 mM KCl, 2.5 mM CaCl2, 1.2 mM MgCl2, and 10 mM
D-glucose, for immediate use. The uptake assay was performed similarly to the
one described for the proteo-liposomes, but using a reaction buffer containing
11 mM HEPES/Tris-base, pH 7.4, 140 mM NaCl, 4.7 mM KCl, 2.5 mM CaCl2,
1.2 mM MgCl2, 10 mM D-glucose, 50 µM L-glutamate, and 5
µM [14C]-L-glutamate, and 0.8-µm nitrocellulose
filters. Background radioactivity was estimated from cells transfected with
empty vector, and subtracted from the uptake data.
Hydrogen-deuterium exchange mass spectrometry
HDX-MS experiments were performed with transporters purified as
described in the proteo-liposome section, and using a Superose 6 5/150 gel
filtration column equilibrated with 50 mM HEPES/Tris-base, 200 mM NaCl, pH7.4, 1
mM L-asp, 0.5 mM TCEP, 0.0632% DDS, 0.01264% CHS, and 5% glycerol.The purified EAAT1cryst was incubated in ice for 30 min with
2.2% DMSO at a monomer concentration of 5.2 µM, in the presence and
absence of 102 µM UCPH101, respectively. Prior to labeling, 10
µL of the unbound and UCPH101-bound EAAT1cryst
solution was equilibrated for 10 min at room temperature. Deuterium exchange was
initiated by adding 40 µL of D2O buffer (50 mM HEPES, pD 7.3,
200 mM NaCl, 1 mM L-asp, 5% glycerol, 0.0632% DDS, 0.01264% CHS, 0.5 mM TCEP)
supplemented or not with 101.2 µM UCPH101. Assuming that the
KD and IC50 values of UCPH101 are similar,
~96% of the transporters would remain bound during deuterium labeling.
Aliquots of 10.4 pmols of protein were removed at defined deuterium exchange
time points (from 10 sec to 60 min) and quenched upon mixing with an ice-cold
acidic solution (0.75% formic acid, 5% glycerol) to decrease the pH to 2.6.
Quenched samples were immediately snap-frozen in liquid N2 and stored
at -80°C until analysis.Prior to mass analysis, quenched samples were rapidly thawed and
immediately injected into a cooled nanoACQUITY UPLC HDX system (Waters corp.)
maintained at 0°C. 8.6-pmol protein samples were on-line digested for 2
min at 20 °C using an in-house packed immobilized pepsin cartridge (2.0 x
20 mm, 66 µL bed volume). The resulting peptides were trapped and
desalted onto a C18 Trap column (VanGuard BEH 1.7 µm, 2.1 x 5 mm, Waters
corp.) at a flow rate of 100 µL/min of 0.15% formic acid, and then
separated in 10 min by a linear gradient of acetonitrile from 5 to 40% at 40
µL/min using an ACQUITY UPLC™ BEH C18 analytical column (1.7
µm, 1 x 100 mm, Waters corp.). After each run, the pepsin cartridge was
manually cleaned with two consecutive washes of 1% formic acid, 5% acetonitrile,
1.5 M guanidinium chloride, pH 2.5. Blank injections were performed between each
run to confirm the absence of carry-over.Mass spectra were acquired in resolution and positive mode on a Synapt
G2-Si HDMS mass spectrometer (Waters corp.) equipped with a standard
electrospray ionization source, as described previously57. Peptides were identified from undeuterated protein
samples acquired in MSE mode by database searching in ProteinLynX
Global Server 3.0 (Waters corp.). Each fragmentation spectrum was manually
inspected for assignment validation. Deuterium uptake values were calculated for
each peptide using DynamX 3.0 (Waters corp.). Only one unique charge state was
considered per peptide and no adjustment was made for back-exchange. HDX-MS
results are reported as relative deuterium uptake values expressed in mass unit
or fractional exchange57. A statistical
analysis was performed with MEMHDX58
using a False Discovery Rate of 1%.
Alignment of human SLC1 transporters.
Amino acid sequences of EAAT1-5, ASCT1-2 and EAAT1cryst
are compared. The boundaries of the α-helices (cylinders) in the
TranD (orange) and the ScaD (teal) seen in the EAAT1cryst
structure are shown. In order to confer crystallizability, the region
between TM3 and TM4c (arrows) from ASCT2 was transferred to a thermally
stabilized EAAT1. To further improve crystal formation in the absence of
UPCH101, mutations M231I and F235I (circles) were introduced
to generate EAAT1cryst-II. These substitutions are found in
EAAT2. Other residues involved in UPCH101 coordination are more
conserved (triangles). Sequences were aligned with Jalview59.
EAAT1cryst and EAAT1 glutamate uptake.
a, Initial rates of L-glutamate uptake from purified
EAAT1cryst reconstituted in liposomes. The solid line is the
fit of a Michaelis-Menten equation to the data with KM=21
± 10 μM and Vmax= 13 ± 1 pmol
μg-1 protein min-1. The graph is the mean
of three independent experiments, and error bars represent s.e.m..
b, L-glutamate uptake was measured in HEK293 cells
expressing WT EAAT1 (black circles) and a truncated mutant beyond E501 (red
symbols). The initial rate of uptake decreased by ~2-fold in the
EAAT1 truncated mutant. Data were normalized to the asymptotic level of
glutamate uptake based on a monoexponential function. The rates obtained
from the fits were 0.16 ± 0.03 and 0.08 ± 0.03
min-1 for EAAT1 and the truncated mutant, respectively. The
graphs are means of 4 independent experiments done in duplicates. Error bars
represent the s.e.m..
EAAT1cryst and GltPh structural comparison.
a-b EAAT1cryst aligns to a monomer of GltPh
(PDB 2NWL) with α-carbon r.m.s.d. of 1.4 Å. The ScaDs
(EAAT1cryst teal, and GltPh purple, a), and
TranDs (EAAT1cryst orange and GltPh, purple, b) are
shown separately for clarity of display.
EAAT1cryst trimeric interface.
a-b, Interface of three ScaDs of the
EAAT1cryst UCPH101-bound structure viewed from the
extracellular side (a) and from the membrane (b).
The TranDs are not shown. The ScaD of one monomer (black) buries 3,000
Å2 in the trimerization interface through extensive
contacts with the two other subunits (teal and purple surfaces), including
six intermolecular salt bridges (shown as green sticks for the monomer in
black). The surface area in the other two monomers is colored in light pink.
Only residues that contribute ≥ 10 Å2 of buried
surface area are highlighted.
TranD-ScaD interface.
a-b, EAAT1cryst monomer viewed from the
membrane (solid black line). Residues in the TranD (colored black) bury
1,760 Å2 at the interface with the ScaD (a).
This interface extends to the extracellular side of the transporter through
interactions between HP2-TM4 (sticks and pseudo-transparent spheres)
(b). c, Cytoplasmic view of the monomer
displaying the salt bridge between TM7 and TM5.
Superposition of EAAT1cryst and EAAT1cryst-II
structures.
a-b, The transport domains of EAAT1cryst
(teal) and EAAT1cryst-II (pink) UCPH101-bound
structures superimpose accurately after aligning their scaffold domains
(a). The overall α-carbon r.m.s.d. was 0.3 Å.
However, the same alignment done with EAAT1cryst-II
UCPH101-bound and -unbound structures shows a small but
global movement of the transport domain (b), with a small
increase in the overall α-carbon r.m.s.d. of 0.1 Å.
c,d Anomalous difference Fourier maps contoured at the
2.8σ (pink mesh), from data collected at low
energy X-rays (1.77 Å), show the correct sequence registry in both
the TranD (orange, a) and the ScaD (teal, b).
Peptide coverage map of EAAT1cryst.
A total of 111 peptides covering 76.3% of the EAAT1cryst
sequence were identified by data independent MS/MS acquisition after 2 min
digestion with immobilized pepsin. Each bar below the EAAT1cryst
sequence corresponds to a unique peptide. The 57 peptides colored in blue
were further selected for HDX-MS data extraction and analysis. The two
additional N-terminal residues (i.e., GP) that remain after
protein purification are also shown. The transmembrane helices (TM) of the
TranD (orange) and the ScaD (cyan) are indicated above the sequence.
UCPH101 effect on the local hydrogen exchange behavior of
EAAT1cryst.
a, HDX profiles of EAAT1cryst (see Methods) in the apo (upper panel) and
UCPH101-bound state (middle panel). The relative fractional
uptake determined for each peptide and at each time point is plotted as a
function of peptide position. The black to red lines correspond to data
acquired from 10 sec up to 1h, respectively. b, The fractional
uptake difference plot was generated by subtracting the deuterium uptake
values in the UCPH101-unbound from those in the bound state.
Negative uptake difference indicates UCPH101-induced decrease in
amidehydrogen exchange. Each dot corresponds to an average of three
independent HDX-MS experiments. The four regions (labeled 1 to 4) showing a
statistically significant modification (p <0.01) of
deuterium uptake upon binding of UCPH101 are highlighted in
grey.
HDX-MS results mapped on the crystal structure of ScaD and TranD of
EAAT1cryst in the unbound and UCPH101-bound
state.
The color code at the bottom shows the average relative fractional
uptake measured in both domains after 10 sec (upper panel), 10 min (middle
panel) and 1h (lower panel) labeling. Missing regions in the crystal
structure are represented by dashed lines. Peptides showing a statistically
significant (p <0.01) modification of deuterium
uptake upon UCPH101 binding are labeled. Uncovered regions are
colored in light blue.One crystal was used to collect diffraction datasets for each
structure, except in the EAAT1cryst UCPH101 and
TFB-TBOA bound structure, where datasets from three crystals were
merged.5% of reflections were used for calculations of
Rfree, except for the EAAT1cryst UCPH101-TBOATFB
bound structure where 10% was used due to the lower number of total reflections.Values in parentheses are for the highest-resolution shell.The anisotropy directions where computed with AIMLESS.
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