SUMMARY
Voltage-gated sodium channels initiate electrical signals and are frequently targeted by deadly gating-modifier neurotoxins, including tarantula toxins, which trap the voltage sensor in its resting state. The structural basis for tarantula-toxin action remains elusive, because of the difficulty of capturing the functionally relevant form of the toxin-channel complex. Here we engineered the model sodium channel NaVAb with voltage-shifting mutations and the toxin-binding site of human NaV1.7, an attractive pain target. This mutant chimera enabled us to determine the cryo-EM structure of the channel functionally arrested by tarantula toxin. Our structure reveals a high-affinity resting-state-specific toxin-channel interaction between a key lysine residue that serves as a ‘stinger’ and penetrates a triad of carboxyl groups in the S3-S4 linker of the voltage sensor. By unveiling this high-affinity binding mode, our studies establish a high-resolution channel-docking andresting-statelockingmechanism for huwentoxin-IV and provide guidance for developing future resting-state-targeted analgesic drugs.
eTOC Blurb
Wisedchaisri et al. report the cryo-EM structure of an engineered bacterial NaV1.7 chimeric channel captured in the resting state by a tarantula toxin. They reveal how the toxin’s ‘stinger’ immobilizes prey at the atomic level and suggest a way to design future resting-state-targeted analgesic drugs.
Graphical Abstract

INTRODUCTION
Voltage-gated sodium channels (NaV) generate and propagate action potentials in nerve and muscle (Hille, 2001; Hodgkin and Huxley, 1952), but the structural basis for their function and pharmacology remains incompletely defined. Upon membrane depolarization, NaV channels transition from the resting state to the activated state, open a Na+-selective transmembrane pore, and then inactivate within a few milliseconds (Hille, 2001; Hodgkin and Huxley, 1952). NaV channels in eukaryotes are composed of a single large polypeptide with 24 transmembrane segments organized in four homologous domains (I-IV) (Catterall, 1984, 1986; Numa and Noda, 1986). Each homologous domain contains six transmembrane segments separated into two functional modules, the voltage-sensing module (VS, segments S1-S4) and the pore-forming module (PM, segments S5-P-S6) (Ahern et al., 2016; Catterall, 1986; Catterall et al., 2017). Each S4 segment contains four to eight repeated motifs of a positively charged amino acid residue (usually Arg) flanked by two hydrophobic residues (Ahern et al., 2016; Bezanilla, 2000; Catterall, 1986; Catterall et al., 2017). Changes in membrane potential exert an electrostatic force on these S4 gating charges, causing inward or outward movement of the S4 segment and coupling these transmembrane movements to conformational changes that open or close the pore (Ahern et al., 2016; Catterall, 1986; Catterall et al., 2017). Prokaryotic NaV channels are simpler in structure, composed of four identical subunits that each is analogous to one domain of a eukaryotic NaV channel (Payandeh et al., 2011; Ren et al., 2001). Thus, this fundamental mechanism of voltage sensing and pore opening is responsible for electrical signaling throughout biology (Gamal El-Din et al., 2018).
The molecular basis for NaV channel function is being progressively elucidated by structural studies of prokaryotic and eukaryotic NaV channels. Many structures of NaV channels with their VS in activated or partially activated conformations have been determined at high resolution, beginning with the bacterial NaV channel NaVAb (Payandeh et al., 2011), and continuing with other bacterial (Shaya et al., 2014; Sula et al., 2017; Zhang et al., 2012b), and mammalian NaV channels (Jiang et al., 2020; Pan et al., 2019; Pan et al., 2018; Shen et al., 2019). In contrast, structural studies of the resting state of NaV channels have been more challenging because the resting state is only present at the negative resting membrane potential of −80 mV in nerve and muscle or −160 mV in bacteria. The structure of the resting state of NaVAb was determined by stabilizing it at 0 mV with a combination of voltage-shifting mutations and disulfide locking (Wisedchaisri et al., 2019). This structure revealed key features of the resting state of the VS and supported a ‘sliding-helix’ mechanism of gating.
Neurotoxins from venomous animals target NaV channels at multiple neurotoxin receptor sites in order to paralyze prey (Catterall, 1980; Hille, 1975, 2001; Lazdunski et al., 1986; Ritchie, 1979; Rochat et al., 1979). Gating-modifier toxins produce their dramatic physiological effects by voltage-sensor trapping; that is, by trapping the VS in either the resting or activated state by binding to it specifically with high affinity (Cestèle et al., 1998; Rogers et al., 1996; Sokolov et al., 2008; Xiao et al., 2008a; Zhang et al., 2012a). Polypeptide toxins from spiders and scorpions target neurotoxin receptor site 4 in domain II of NaV channels and either prevent or inappropriately enhance activation of the VS (Catterall et al., 2007; Cestèle et al., 1998; Couraud et al., 1982; Schmalhofer et al., 2008; Sokolov et al., 2008; Xiao et al., 2008a; Xiao et al., 2014; Zhang et al., 2011, 2012a). Huwentoxin-IV (μ-theraphotoxin-Hs2a; HwTx-IV) from the Chinese bird tarantula Haplopelma schmidti (Peng et al., 2002; Xiao et al., 2008b) and Protoxin-II (β/ω-theraphotoxin-Tp2a; ProTx-II) from the Peruvian green velvet tarantula Thrixopelma pruriens (Middleton et al., 2002) inhibit human NaV1.7 with nanomolar affinity. Structures of NaV1.7 and its bacterial chimera constructs with ProTx-II and HwTx-IV bound to activated or partially activated conformations of the VS have been reported (Gao et al., 2020; Shen et al., 2019; Xu et al., 2019), although it has been suggested that the overall channel could be in the inactivated state (Shen et al., 2019). However, due to the long-standing challenges in isolating NaV channels in their resting state, there is no structure of any inhibitory gating-modifier toxin bound in its high-affinity pose to the resting state of its channel target. The lack of such a structure leaves a major gap in our understanding of the molecular mechanism of action of these deadly toxins.
In these studies, we imported the high-affinity binding site for HwTx-IV from the human neuronal NaV1.7 channel into the ancestral NaV channel NaVAb, introduced voltage-shifting mutations to stabilize the toxin/channel complex in the resting state at 0 mV, and determined its structure at high resolution by cryo-EM. Our results reveal the structure of the resting state of an NaV channel with a gating-modifier bound and define a high-resolution voltage sensor-trapping mechanism through which HwTx-IV opposes the electrostatic force generated by depolarizing stimuli and locks the NaV1.7 in its resting state by inserting a ‘stinger’ Lys into the VS of its prey. Moreover, because NaV1.7 is an actively investigated target for pain therapeutics, our results may offer guidance for future drug discovery efforts to develop much-sought first-in-class analgesic drugs that target the resting state of this key NaV channel.
RESULTS
Design, construction, and characterization of a voltage-shifted NaVAb/NaV1.7-VS2 chimera
Chimeric channels in which portions of the VS of NaVAb were replaced by corresponding segments of NaV1.7 yielded a substantial positive shift in the voltage dependence of activation and sensitivity to modulation by the inhibitory gating-modifier toxin ProTx-II (Rajamani et al., 2017). We engineered NaVAb to contain segments of the NaV1.7 VS2 as a receptor site for HwTx-IV. We first aligned the VS sequences of NaV1.7 VS2 and NaVAb and then grafted NaV1.7 VS2 nucleotide sequences encoding the S1-S2 and S3-S4 segments into corresponding segments of a cDNA encoding NaVAb (Figures 1A–1C and S1). Several versions of the NaVAb/NaV1.7 VS2 chimera were constructed and characterized by electrophysiology (STAR Methods). The construct that yielded the largest positive shift in the voltage dependence of activation (V1/2 = +34.6 ± 1.4 mV) was selected for this study (Figures 1D, 1E and S1). Subsequently, a voltage-shifting mutation previously used for stabilizing NaVAb in the resting state (Wisedchaisri et al., 2019) was introduced into the chimera. This mutation (L834A in NaV1.7) caused a further positive shift in the voltage dependence of activation to V1/2 = +83.4 ± 0.9 mV (referred to as NaVAb/NaV1.7-VS2A; Figures 1D, 1E and S1). Most importantly, this chimera remains closed in the resting state at 0 mV at which our structural studies were conducted.
Figure 1. Design of Voltage Shifting NaVAb/NaV1.7-VS2 Chimera.
(A) Topology diagram of substitution. Transmembrane and extracellular portion of human NaV1.7 VS2 S1-S2 and S3-S4 helices (cyan) were grafted onto equivalent region of NaVAb (gold).
(B) Model of substitution. Cyan highlights portions of human NaV1.7 S1-S2 and S3-S4 helices that have been grafted onto NaVAb (gold).
(C) Sequence alignment of S3-S4 region of different human NaV subtypes. Sequence portion including the “LFLAD” motif that interacts with HwTx-IV is highlighted in yellow.
(D) Representative current families of NaVAb/NaV1.7-VS2 chimera (cyan) and with L834A mutation (VS2A) (red). Transiently transfected Sf9 cells were held at −150 mV and stimulated for 50 ms to depolarized voltages in 10 mV increments. Scale bars represent 10 msec × 1 nA.
(E) Normalized conductance-voltage (G/V) relationships and Boltzmann fits for NaVAb (black dash; WT (Gamal El-Din et al., 2013)), NaVAb/NaV1.7-VS2 chimera alone (cyan; V1/2 = 34.6 ± 1.4 mV, k = 10.0, n = 0.1, n = 6) and with L834A mutation (VS2A) (red; V1/2 = 83.4 ± 0.9 mV, k=9.1 ± 0.6, n = 3). Markers and error bars represent average G/Gmax ± standard error of the mean (SEM). Half activation (V1/2) and slope (k) values are averages of individual fits ± SEM. Curves = 1/(1+ê((V1/2-Vm)/k)).
See also Figure S1.
Functional voltage sensor trapping of a NaVAb/NaV1.7-VS2 chimera by an engineered HwTx-IV
The potent gating modifier toxin HwTx-IV has high affinity for NaV1.7 (KD = 26 nM; (Xiao et al., 2008a). Further peptide engineering of this toxin led to the discovery of m3-HwTx-IV with triple mutations of E1G, E4G, Y33W, which has improved affinity (KD = 0.4 to 3.3 nM; (Rahnama et al., 2017; Revell et al., 2013)). We characterized the efficacy of m3-HwTx-IV for voltage-sensor trapping of our NaVAb/NaV1.7-VS2A chimera in its resting state. Perfusion of increasing concentrations of m3-HwTx-IV gave progressive reduction in the sodium current (Figure 2A). At 100 nM, the sodium current was nearly completely blocked at accessible membrane potentials (Figure 2B). The IC50 for the inhibition was 2.6 ± 0.13 nM for the chimera (Figure 2C), similar to values of 0.4 ± 0.1 nM and 3.3 ± 1.1 nM previously reported for intact human NaV1.7 (Rahnama et al., 2017; Revell et al., 2013). Importantly, m3-HwTx-IV at 100 nM completely inhibited sodium current for the chimera (Figure 2B) until long, strong depolarizing pulses were applied (Figure 2D). The voltage-dependent reversal of voltage-sensor trapping was more rapid and complete upon depolarization to 160 mV, intermediate at 120 mV, and slower and incomplete in the time frame we studied at 80 mV (Figure 2D). These results show that the binding of m3-HwTx-IV inhibits the NaVAb/NaV1.7-VS2A chimeric channel by trapping it in the resting state and that this voltage-sensor trapping is reversed by a long, strong depolarization to expel the bound toxin, as observed previously for inhibitory gating-modifier toxins acting on eukaryotic sodium channels (Sokolov et al., 2008; Xiao et al., 2014).
Figure 2. Voltage Sensor Trapping of NaVAb/NaV1.7 VS2A by m3-HwTx-IV.
(A) Representative traces of sodium outward currents and following inward tail currents in Hi5 cells in response to 50-ms pulses from a holding potential of −160 mV in 10 mV steps from 0 mV to +160 mV (Black). Sodium currents measured from the same cell after perfusion with 10 nM m3-HwTx-IV (Red). Tail currents before (black) and after (red) treatment with different concentrations of m3-HwTx-IV (0.1, 1, 10, and 100 nM as indicated).
(B) Normalized Current/Voltage (I/V) plot of NaVAb/NaV1.7-VS2A before (black) and after (red) treating cells with 100 nM m3-HwTx-IV. Tail currents measured after m3-HwTx-IV treatment were normalized to the one measured previously. Conductance was estimated from the tail current amplitude and normalized to the control amplitude at the +160-mV test potential. The solid black line is the fit of the Boltzmann equation to the data. The V1/2 was 107.2 ± 0.5 mV with a slope factor K= 12.5 ± 0.3. Data are represented as mean ± SEM with n = 5 to 8.
(C) Concentration-response curve of m3-HwTx-IV interaction with NaVAb/NaV1.7-VS2A chimera. The solid red line is the best fit using the Hill equation. IC50= 2.6 ± 0.3 nM with a Hill coefficient = 0.7. Data are represented as mean ± SEM with n = 5 to 7.
(D) Time course for recovery of blocked tail current following strong depolarizations in the presence of 250 nM m3-HwTx-IV. Current amplitude was measured at +80, +120, and +160 mV. Different pulse durations were used from 50-ms to 600-ms. Recovered currents were normalized to the peak current elicited from depolarizations to 600-ms. Data are represented as mean ± SEM with n = 3 to 5. Inset. Representative current traces of recovered currents at +120 mV depolarizing potentials.
Structure of NaVAb/NaV1.7-VS2A chimera with m3-HwTx-IV bound
Efforts to crystallize NaVAb/NaV1.7-VS2A with m3-HwTx-IV bound were unsuccessful. Therefore, we generated a fusion protein for cryo-EM imaging by linking the C-terminal alpha helix of maltose-binding protein (MBP)to the N-terminal alpha helix of NaVAb/NaV1.7-VS2A with a rigid Asn-Ala linker (Waugh, 2016). The MBP-NaVAb/NaV1.7-VS2A chimera and m3-HwTx-IV form a high-affinity complex that can be co-eluted during size-exclusion chromatography (Figure S2A), indicating a stable stoichiometric complex suitable for structural study. We assembled an MBP-NaVAb/NaV1.7-VS2A:m3-HwTx-IV complex at 1:8 molar ratio in GDN detergent, flash froze the sample on EM grids, and imaged the sample by cryo-EM using a Titan Krios system (Figures S2B and S2C; Methods). We reconstructed a 3D map to 3.6 Å overall resolution (Figure 3A), as assessed by the Fourier Shell Correlation (FSC) between independently refined half-maps with a criterion of 0.143 (Henderson et al., 2012) (Figure S2D). The density map has local resolution of ∼3.5 Å in transmembrane segments of the VS and pore, and ∼4–4.5 Å in the loops and S4-S5 linker (Figures 3A and S3A). The m3-HwTx-IV density is unambiguously present but the resolution ranges from ∼4Å at the VS aqueous cleft to ∼5 Å near detergent micelles (Figures 3A, S3B and S3C). Using the known structure of m3-HwTx-IV as a guide (Rahnama et al., 2017), we built an atomic model of the NaVAb/NaV1.7-VS2A:m3-HwTx-IV complex in the interpretable part of the map and refined the structure to give a high-resolution image of the toxin/channel complex (Figures 3B and S3).
Figure 3. Cryo-EM Structure of NaVAb/NaV1.7 VS2A Chimera in the Resting State Trapped by m3-HwTx-IV.
(A) Cryo-EM density map colored by local resolution in side and top views. Local resolution was evaluated using ResMap (Kucukelbir et al., 2014). The right panel shows resolution spectrum bar.
(B) Overall structure of m3-HwTx-IV:NaVAb/NaV1.7-VS2A chimera. Side view (left) and top view (right) are shown in the same orientation as in (A). S0 to S3 segments of the VS are colored in teal and S4 in magenta. The S4-S5 linker is highlighted in blue and the pore module in yellow. m3-HwTx-IV is colored in red superimposed with transparent van der Waals surface.
See also Figures S2 and S3, and Table S1.
Resting state conformation of NaV1.7 VS2 with m3-HwTx-IV bound
Transmembrane helices S1-S4 of NaVAb/NaV1.7-VS2A adopt a canonical VS topology (Payandeh et al., 2011) in which the extracellular loops S1-S2 and S3-S4 form helical hairpins that create an aqueous cleft on the extracellular side (Figure 4A, left). Helix S4 adopts a 310 helical conformation, in which all four gating charge Arg’s line up on one side of the helix with their side chains pointing toward helix S2 (Figure 4B, left). The S4 helix markedly assumes an “inward” conformation, in which the hydrophobic constriction site (HCS) residue F776 from S2 is wedged between the side chains of R1 and R2 such that R2-R4 are all on the intracellular side of the HCS. Gating charge R1 interacts with N769 from the ENC of S2, while R2 and R3 make ion-pair interactions with INC residues E779 from S2 and D801 from S3. R4 is located in the cytoplasm and stabilized by conserved W797 on the intracellular side of S3. As S4 partially dips into the cytoplasm in this “inward” conformation, an angle formed between S4 and the S4-S5 linker creates an elbow from which the S4-S5 linker rises toward the inner membrane surface to connect with the intracellular end of S5 and the pore (Figure 4C, left). Together, the S4-S5 linkers from all four subunits form a collar that wraps around S6 to hold the pore closed (Figure 4D, left, blue). The VS and S4-S5 linker conformations observed in the NaVAb/NaV1.7-VS2A:m3-HwTx-IV complex closely resemble the conformations identified previously in the disulfide-locked resting state structure of NaVAb ((Wisedchaisri et al., 2019); RMSD = 0.98 Å over 125 Cα atoms for the S4 helix, S4-S5 linker, and the S5-S6 helices; Figure S4), indicating that m3-HwTx-IV traps VS2 in the same deep resting state in the absence of disulfide-locking.
Figure 4. Structure of NaVAb/NaV1.7-VS2A Trapped by m3-HwTx-IV in the Resting State and Comparison to NaV1.7 VS2 Trapped by HwTx-IV in a Partially Activated State.
(Left panels) NaVAb/NaV1.7-VS2A in the resting state; (Right panels) NaV1.7 VS2 in a partially activated state bound to HwTx-IV + saxitoxin (PDB 6J8G)
(A) Structures of the VS as backbone cartoon superimposed with the molecular surface. S0 to S3 are shown in light teal and S4 in magenta. An aqueous cleft between S1-S2 and S3-S4 helix-loop-helix is indicated.
(B) Gating charge movement. Four Arg gating charges R1-R4 (blue), extracellular negative charge (ENC) cluster of E753 on S1 and N769 on S2, intracellular negative charge (INC) cluster of E779 on S2 and D801 on S3 (red), and F776 in the hydrophobic constriction site (HCS) (green) are shown in sticks. S4 (magenta) moves outward from resting state to partially activated state by ∼7.3 Å, passing nearly two gating charges through the HCS on S2. Part of S3 is omitted for clarity.
(C) Side view of the structures with the S0 to S3 segments shown in gray, S4 in magenta, the S4-S5 linker in blue, and the pore module in yellow. The S4 segment moves outward across the membrane from the resting to the partially activated states while the S1 to S3 segments remain relatively unchanged with respect to the membrane. The S4-S5 linker acts as an elbow that connects the S4 movement to modulate the pore. Three VS and two pore modules are omitted for clarity.
(D) Bottom (intracellular) view of the structures in (C) with complete pore modules. The S4-S5 linker (blue) undergoes a large conformational change that tightens the collar around the S5 and S6 segments (yellow) of the pore in the resting state and loosens the collar in the partially activated state. S0 to S3 are omitted for clarity.
See also Figures S4 and S6.
Comparison of NaVAb/NaV1.7-VS2A trapped in the resting state by m3-HwTx-IV with NaV1.7 VS2 in the activated state could reveal important insights into gating charge movement and mechanical coupling to the pore. Unfortunately, there is no available structure of NaV1.7 apo-VS2 in the fully activated state. We therefore compare our structure with VS2 of human NaV1.7 bound to HwTx-IV in a partially activated state (Shen et al., 2019) (Figure 4, right panels). This partially activated conformation of VS2 is consistent with an inactivated state of the NaV1.7 channel as a whole, as suggested by Shen et al., because partial or full activation of the VS would be required to trigger inactivation. From the resting state of NaVAb/NaV1.7-VS2A, the S4 helix translocates outward by ∼7.3 Å (∼1.2 helical turns) toward the extracellular milieu to reach this partially activated “outward” conformation, which deepens the extracellular aqueous cleft (Figure 4A, right). This distance of movement is significantly less than the 11.5 Å translocation observed in the S4 segment of NaVAb between resting and fully activated states, which corresponds to two complete helical turns (Wisedchaisri et al., 2019), suggesting that this state of the VS in human NaV1.7 is only partially activated. Only side chains of gating charges R1 and R2 have moved outward completely through the HCS, but R3 is located at the same level as F776 in the HCS and R4 is completely on the intracellular side (Figure 4B, right). R1 and R2 interact with ENC while R4 interacts with INC. Evidently, binding of HwTx-IV by itself is not sufficient to move VS2 inward into its resting state at 0 mV without voltage-shifting mutations. Therefore, this complex of HwTx-IV with partially activated VS2 of NaV1.7 is likely to be a low-affinity complex on the pathway to voltage-dependent toxin binding or dissociation (eg., Figure 2).
In the activated states of NaVAb (Wisedchaisri et al., 2019) and both VS1 and VS3 of NaV1.7 (Shen et al., 2019), gating charges R1-R3 fully translocate outward from the HCS. In contrast, the partial outward position of S4 in VS2 of the NaV1.7 complex with HwTx-IV can likely be attributed to the association of HwTx-IV with this partially activated conformation of the S4 segment, which prevents VS2 from full activation. The outward movement of S4 also unbends the elbow and brings the S4-S5 linker from the cytoplasm to a position almost parallel to the membrane (Figure 4C, right), and in turn, loosens the collar around the S6 pore-lining helices as if they are poised to open the activation gate with further depolarization (Figure 4D, right).
Neurotoxin receptor site 4 with HwTx-IV bound in resting and partially activated states of the voltage sensor
In the resting state complex revealed by our results, m3-HwTx-IV interacts intimately with VS2 and penetrates into the aqueous cleft between the S1-S2 and the S3-S4 helical hairpins, as observed in a side view (Figure 5A). The penetration of the toxin between these two helical hairpins is seen in more detail in a top view (Figure 5A). These structural results are consistent with a high-affinity interaction between the toxin and its receptor site, which is illustrated in more detail in Figure 5C. m3-HwTx-IV inserts its Loop 4 and its conserved C-terminal “26RK×RWCK32” motif (Figure 6A, underlined) into the outer end of the VS2 aqueous cleft (Figure 5C). There are extensive interactions with amino acid residues in the S3-S4 loop. Negatively charged residues E811, D816, and E818 in the S3-S4 extracellular loop of VS2 interact with positively charged residues K27 and K32 of m3-HwTx-IV (Figure 5C). Remarkably, m3-HwTx-IV inserts K32 with its positively charged amino group like a “stinger” into this triad of negatively charged residues in its prey Figure 5C and S3C. The “812LFLAD816” motif (Figure 1C) in the S3-S4 loop of VS2 provides hydrophobic and van der Waals interactions with I5, F6, T28, W30, K32, and Q34 and nearby residues of m3-HwTx-IV with energy inversely proportional to the sixth power of their distance (Figure 5C). In contrast to these extensive interactions with the S3-S4 loop, residues E753 and N763 are the only residues in S1-S2 loop observed to interact directly with bound m3-HwTx-IV, through their close approach to K27 and R29, respectively (Figure 5C). F813, A815, D816 are unique to NaV1.7 among NaV subtypes (Figure 1C) and may be responsible for NaV1.7 specificity.
Figure 5. Molecular Interactions of HwTx-IV with Neurotoxin Receptor Site 4 in Resting and Partially Activated NaV1.7-VS2.
(A) Binding position of m3-HwTx-IV to the resting state of neurotoxin receptor site 4 of NaVAb/NaV1.7-VS2A in side and top views. Cryo-EM density map filtered to 4.5 Å resolution for m3-HwTx-IV (red) is shown superimposed with the atomic model.
(B) Binding position of HwTx-IV to the partially activated state of neurotoxin receptor site 4 of NaV1.7 in side and top views. Cryo-EM density map (EMD-9781) filtered to 4.5 Å resolution for HwTx-IV (green) is shown in comparison to (A).
(C) Detailed molecular interactions of m3-HwTx-IV with NaVAb/Na1.7-VS2A chimera in the resting state. Residues making contacts within 5 Å are shown as sticks models and highlighted in yellow for residues from VS2 chimera as in Figure 1C. Some parts of the interactions were only partially resolved in the experimentally determined density and were modeled based on rigid-body docking and refinement of the known NMR structure of the toxin.
See also Figure S5.
Figure 6. Detailed Map of Interactions Between m3-HwTx-IV and VS2.
(A) Amino acid sequence of m3-HwTx-IV. Cysteine residues that form disulfide bonds are highlighted in gray. Positive charge and negative charge residues are colored in blue and red letters, respectively. Residues of m3-HwTx-IV that when mutated to alanine resulted in a loss of affinity for NaV1.7 by less than 2-fold are highlighted in yellow, 2–5-fold are in pink, and more than 5-fold in red, or positive gain in affinity in green according to (Revell et al., 2013). The C-terminal “26RKxRWCK32” motif important for binding is underlined.
(B) Close up top view as in Figure 5C right panel with m3-HwTx-IV removed. Surface residues are colored based on changes in affinity when mutated according to (Xiao et al., 2011).
(C) Close up view as in Figure 5C right panel with m3-HwTx-IV turned 180° open face up to show resides making interactions with the NaVAb/Na1.7-VS2A. Surface residues are colored based on changes in affinity when mutated to Ala as in (A).
Comparison with mutational studies reported previously for NaV1.7 further illustrates the close binding interactions with amino acid residues whose mutation has large effects on toxin binding (Figures 6B and 6C). Mutation of residues colored in green to Ala gives an increase in affinity, whereas residues colored in shades of red give decreases in affinity from 2-fold to more than 20-fold as coded in the depth of color (Figure 6B). Mutations of E753Q, E811Q, L814A, D816A, and E818C each decreased HwTx-IV inhibition of NaV1.7 activation (Xiao et al., 2010). Double mutations of D816N/E818Q also greatly diminished HwTx-IV sensitivity for NaV1.7 (Xiao et al., 2008a). On the toxin side, Ala substitutions of F6, W30, and K32 in HwTx-IV all decrease affinity for NaV1.7 while Ala substitutions of I5 and T28 increase the affinity (Figures 6A and 6C) (Revell et al., 2013), which correlate well with our structural findings that these residues make contacts with NaV1.7. Mutations of the ‘stinger’ K32 and its three negatively charged targets, E811, D816, and E818 have particularly strong effects (Figures 6B and 6C). Approximately 480 Å2 of protein surface on each side of this interface interact to form the toxin/receptor complex. These intimately interacting binding surfaces revealed for m3-HwTx-IV and neurotoxin receptor site 4 support a specific high-affinity interaction.
In sharp contrast to this tight interaction of m3-HwTx-IV with VS2 in its resting state conformation, interactions of HwTx-IV with VS2 of NaV1.7 in a partially activated state appear much less extensive in the structures presented by Shen et al (Figure 5B; (Shen et al., 2019)). Outward movement of the S4 segment in the partially activated state of the VS likely impedes tight binding of HwTx-IV to the S3-S4 loop, which is unresolved in this image (Figure 5B, side view; S4, purple; unresolved S3–S4 loop, yellow dashed line). Similarly, bound HwTx-IV does not penetrate into the cleft formed by the S3-S4 helical hairpins (Figure 5C, side view), perhaps because the presence of the S4 segment in an outward conformation would create a clash. The lack of clear molecular interactions between HwTx-IV and partially activated VS2, especially in the S3-S4 loop, is indicative of a low-affinity toxin-receptor complex. Consistent with this conclusion, we estimate that <300 Å2 of protein surface contributes to this interface. The comparison of these two structures illustrates the essence of voltage-sensor trapping. Intimate, high-affinity interactions bind the toxin to neurotoxin receptor site 4 in the resting state and trap VS2 in that state. In contrast, voltage-driven outward movement of the S4 segment destabilizes the toxin-receptor complex by disrupting productive molecular interactions and changing the conformation of the S3-S4 helical hairpin in the partially activated state of VS2. These large differences in binding interactions produce the characteristic, strongly voltage-dependent unblock observed for gating modifier toxins (Figure 2; (Sokolov et al., 2008)). High-affinity binding of HwTx-IV to the resting state of VS2 is the structural basis for its deadly toxic effect, because only this high-affinity toxin/receptor complex can resist the electrostatic force of depolarization, trap the voltage sensor in its resting state, prevent channel activation, and paralyze prey.
DISCUSSION
HwTx-IV traps VS2 in the resting state
Our structure of m3-HwTx-IV bound to the NaVAb/NaV1.7-VS2A chimera in the resting state shows the tarantula toxin occupying the aqueous cleft of VS2 and interacting strongly with the S3-S4 loop to restrict S4 to an inward position projecting into the cytoplasm. This inward position reveals three gating charge Arg on the intracellular side of the HCS and implies exchange of ion-pair interactions from negatively charged residues in the ENC to those in the INC. This position of S4 creates an elbow connecting S4 to the S4-S5 linker, which points into the cytoplasm. The conformation observed here is nearly identical to the resting state conformation in the disulfide-locked resting state (Wisedchaisri et al., 2019), but it is captured here without any chemical modification. This structure verifies that (i) HwTx-IV traps the VS in the resting state to inhibit channel activation; (ii) the resting-state conformations of the VS and S4-S5 linker are likely universal in prokaryotic and eukaryotic NaV channels; and (iii) the disulfide-locked resting state reported previously is not influenced by the disulfide crosslinking used to stabilize it. In this resting-state conformation of NaVAb/NaV1.7-VS2A, the S4 segment is like a cocked gun, ready to shoot out upon depolarization and initiate pore opening. The four S4-S5 linkers form a tight collar to restrict movement of the S6 segments that form the activation gate and keep the channel closed. This conformation reveals the fundamental structural mechanism of voltage-sensor trapping. The binding energy of m3-HwTx-IV imposes an inward resting position of the S4 segment and its gating charges and thereby inhibits voltage-dependent activation.
HwTx-IV binds deeper and with higher affinity in VS2 in the resting state
This structure of the high-affinity complex of m3-HwTx-IV with VS2 in the resting state stands in striking contrast to the previous structure of HwTx-IV bound to VS2 of NaV1.7 in a partially activated state (Shen et al., 2019). In this previously reported structure, the S4 segment is in a partially activated position in VS2, with two gating charges completely outside the HCS, more than 7 Å outward from their resting state position. The S3-S4 loop is unresolved and may not be tightly bound to HwTx-IV in partially activated VS2 (Shen et al., 2019). HwTx-IV appears to make these superficial interactions because the outward position of S4 disrupts the structure of the S3-S4 helical hairpin and prevents access to deeper interaction sites. This comparison suggests that the high-affinity toxin-receptor complex forms only in the resting state, accompanied by unwinding the S3-S4 helical hairpin and deeper and tighter binding of HwTx-IV, which allows the ‘stinger’ Lys to penetrate the triad of negatively charged residues in the S3-S4 loop and lock the voltage sensor firmly in place. This mode of ligand interaction may be more widespread among ion channels, as a Lys residue is also observed to bind tightly in a cage of Trp residues in calmodulin complexes with TRP5 and TRP6 channels (Dang et al., 2019; Singh et al., 2018). Formation of this specific high-affinity complex with HwTx-IV effectively traps the voltage sensor in its resting state. Strong depolarization activates the VS, moves the S4 segment outward, and expels the bound toxin, perhaps through low-affinity intermediate states like the partially activated state of VS2 with HwTx-IV weakly bound (Figure 5; (Shen et al., 2019)). Thus, the essence of voltage-sensor trapping is revealed by the structure of m3-HwTx-IV bound to the resting state of VS2.
A two-step toxin-binding and voltage-sensor trapping mechanism
Our results suggest an unusual voltage-dependent two-step binding and voltage-sensor trapping mechanism, in which only the high-affinity resting state complex is productive in blocking channel activation. We speculate that HwTx-IV can bind loosely and with low affinity to VS2 through weak protein interactions with the S1-S2 and S3-S4 loops, even in a partially activated state of the VS. However, this binding interaction is not functionally significant because it occurs when the VS2 is already partially activated. In sharp contrast, a second step of high-affinity toxin interaction with the resting state is required for voltage-sensor trapping, which is the functionally important step in toxin action. As our structure shows, m3-HwTx-IV binds deeper in the aqueous cleft and forms a tight, high-affinity interaction with the S1-S2 and S3-S4 helical hairpins that thrusts a key positively charged ‘stinger’ Lys amino group into a triad of negative charges in its receptor site. Only this high-affinity toxin interaction covering 480 Å of protein surface on each side has sufficient stability to resist the force of the electrical field acting on the S4 gating charges and therefore is able to trap VS2 in its resting state and prevent sodium channel activation at physiological membrane potentials. We propose that the energy of this protein interaction is the deadly force through which the tarantula immobilizes its prey.
A common mode of action for NaSpTx toxins
Closely related toxins in the NaSpTx family 1 are likely to share a common mode of inhibition with HwTx-IV. Hainantoxin-IV (β-theraphotoxin-Hhn1b; HnTx-IV) from a related Chinese black earth tiger tarantula Haplopelma hainanum shares close sequence similarity to HwTx-IV (80% identical) and also retains the “26RKxRWCK32” motif in Loop 4 and C-terminus identical to HwTx-IV (Klint et al., 2012). HnTx-IV inhibits NaV1.7 with IC50 of 21–34 nM (Cai et al., 2015; Li et al., 2004), similar to that of HwTx-IV, and mutations of positive charge residues K27A and R29A greatly diminished the affinity for NaV1.7 (Li et al., 2004). On the NaV1.7 side, mutations of E753Q, D816N, and E818Q similarly decreased HnTx-IV affinity by 2.0–130 fold (Cai et al., 2015). This indicates that both HwTx-IV and HnTx-IV share the same binding determinants to NaV1.7 and likely bind to NaV1.7 VS2 in a similar manner.
ProTx-II is in NaSpTx family 3 and is much more distantly related to HwTx-IV (Figure S5A). Nevertheless, like HwTx-IV, it binds superficially to neurotoxin receptor site 4 in partially activated states of the VS and does not penetrate deeply into the aqueous cleft in VS2 (Figures S5B–S5D). The surface area of interaction with VS2 is <350 Å2, similar to the low affinity interactions of HwTx-IV with a partially activated state of VS2 (Figure 5). Multiple complexes of ProTx-II with partially activated VS2 have been studied by cryo-EM (Shen et al., 2019; Xu et al., 2019). Although the VS in the structure of Xu et al. were proposed to represent deactivated states, their conformation is consistent with a partially activated intermediate state, as the S4 segment is located substantially outward from its position in the resting (ie., deactivated) state that we report here (Figures S5B–S5D). The structures of VS2 in these complexes form a series of partially activated intermediate states and activated states (Figure S6). The conformations of the voltage sensor in this series fit closely with the predictions of the sliding-helix model of voltage sensing (Catterall, 1986; Catterall et al., 2017; Yarov-Yarovoy et al., 2012). These structures suggest that ProTx-II can form low-affinity complexes with partially activated VS2 in multiple states. However, as we show here for HwTx-IV, it likely requires the resting state to form the high-affinity interactions involving a large surface area of the toxin and its receptor site, which are necessary for effective voltage-sensor trapping.
Implications for human NaV1.7
Neurotoxin site 4 ligands like HwTx-IV and ProTx-II inhibit NaV1.7 by trapping VS2 in the resting state, thereby preventing channel activation until a more positive membrane potential is reached. Our NaVAb/NaV1.7 VS2A chimera provides a structural basis for resting state trapping by HwTx-IV action. However, due to the tetrameric nature of the chimera, all voltage sensors are trapped in the resting state in a homogeneous fashion. This arrangement contrasts with eukaryotic sodium channels, which contain four homologous, but nonidentical, domains in a single polypeptide. HwTx-IV targets only VS2 in eukaryotic sodium channels (Xiao et al., 2014). Based on our results, we propose a mechanism for NaV1.7 inhibition by HwTx-IV as follows. First, HwTx-IV approaches NaV1.7 embedded in the plasma membrane at a negative resting membrane potential and binds tightly to the S1-S2 and S3-S4 helical hairpins and the aqueous cleft on VS2 in the resting state. Next, when the membrane potential is depolarized, the S4 helices in VS1, 3, and 4 move outward, priming the channel for opening. However, since VS2 is trapped in the resting state, the DII S4-S5 linker blocks S6 from moving, incapacitating pore opening. As long as HwTx-IV stays bound on VS2, the channel remains closed at physiologically accessible membrane potentials, and the action potential cannot be initiated or propagated.
Design and potential therapeutic significance of resting-state inhibitors of NaV1.7
The mechanism for voltage-sensor trapping of NaV1.7 in the resting state by gating-modifier toxins has significant implications for physiology and medicine. NaV1.7 plays a key role in transmission of nociceptive information from the periphery to the spinal cord (Dib-Hajj et al., 2013). Gain-of-function mutations cause hyperalgesic syndromes, whereas loss-of-function mutations cause congenital indifference to pain (Dib-Hajj et al., 2013). Chronic pain is an unmet medical need that causes much loss of human potential and has driven the epidemic of opiate abuse. Drug discovery efforts have focused on sodium channel inhibitors that target activated states (Ahuja et al., 2015; Jarvis et al., 2007), but these compounds have not yet been successful in clinical use. Even in nociceptive afferents that are firing action potentials at maximal frequency, NaV1.7 channels spend more than 90% of the time in the resting state between action potentials. Drugs that lock NaV1.7 in the resting state would be powerful analgesics. Our results show that the resting state has a unique structure that can be in principle be effectively targeted by structure-based drug design, just as evolution has targeted this state-dependent structure by high-affinity neurotoxins. The binding surface we have revealed (Figure 6) is an excellent target for structure-based drug design, as it has a rigid array of positive, negative, and hydrophobic residues to mediate specific, high-affinity drug binding. We hope that our resting-state structure may provide guidance for future drug discovery efforts in targeting the resting state of sodium channels.
Limitations
Our conclusions are limited by the resolution of our cryo-EM structures. The resolution of the majority of the NaVAb/NaV1.7 chimera in its resting state is 3.5–4.0 Å (Figure 3). The resolution of m3-HwTx-IV is ∼4.0 Å at the interface of m3-HwTx-IV with VS2A but declines to nearly 5 Å on the backside of the toxin away from the interface (Figure 3). In fitting the toxin into our cryo-EM density, we overcame these limitations by using the known NMR structure of m3-HwTx-IV, which is rigidly fixed by three disulfide bonds. The key amino acid side chains of the m3-HwTx-IV toxin and its target site on VS2A are well fit by the local cryo-EM density, as illustrated in Figures 5 and S3, which allowed us to build an accurate molecular model of the toxin/receptor interaction.
STAR METHODS
RESOURCE AVAILABILITY
Lead contact
Further information and requests for resources and reagents should be directed to and will be fulfilled by the Lead Contact, William A. Catterall (wcatt@uw.edu).
Materials Availability
Reagents generated in this study will be made available on request, but we may require a payment and/or a completed Materials Transfer Agreement if there is potential for commercial application.
Data and Code Availability
Cryo-EM map has been deposited in the Electron Microscopy Data Bank (EMDB) under accession code EMD-22661. The coordinates of the atomic model have been deposited in the PDB under accession code 7K48.
EXPERIMENTAL MODEL AND SUBJECT DETAILS
Microbe strains
E. coli GC10 was cultured at 37°C in LB medium supplemented with 100μg/ml of ampicillin for plasmid DNA extraction. E. coli DH10Bac was cultured at 37°C in LB medium supplemented with 50 μg/mL kanamycin sulfate, 7 μg/mL gentamicin and 10 μg/mL tetracycline for bacmid production.
Cell lines
Sf9 (Spodoptera frugiperda) insect cells were maintained in Grace’s Insect Medium and supplemented with 10% FBS and penicillin/streptomycin at 27°C and passaged at 80–95% confluence for electrophysiology. Sf9 and Hi5 (Trichoplusia ni) insect cells were maintained and infected in Grace’s Insect Medium supplemented with 7.5% FBS and glutamine/penicillin/streptomycin at 27°C for baculovirus production and protein expression, respectively.
METHOD DETAILS
Construction of NaVAb/NaV1.7-VS2 chimera
NaVAb/NaV1.7-VS2 cDNAs with a wide range of voltage-shifting mutations and combinations were constructed in order to explore the range of positive shifts in the voltage dependence of activation that are possible. These NaVAb/NaV1.7-VS2 chimeras were generated by grafting nucleotide sequences of S1-S2 and S3-S4 segments of NaV1.7 VS2 into homologous regions in NaVAb. The cDNA encoding an initial chimera was gene synthesized, amplified by PCR, cloned into the pIZT vector, and modified by site-directed mutagenesis to generate different various chimera constructs that were then characterized by electrophysiology in Sf9 cells as described previously (Wisedchaisri et al., 2019). For more experimental details on construction and functional characterization of these constructs, see McCord, E., Broadband tuning the voltage dependence of a sodium channel. PhD Dissertation, University of Washington: https://digital.lib.washington.edu/researchworks/handle/1773/45249. The most positively shifted chimera (NaVAb/NaV1.7-VS2A), which contains the L834A mutation (equivalent to NaVAb L109A (Wisedchaisri et al., 2019)), was selected for structural and functional studies with m3-HwTx-IV (Figures 1 and S1A).
DNA fragments of NaVAb/NaV1.7-VS2A were amplified by PCR from the pIZT NaVAb/NaV1.7-VS2A plasmid and fused to DNA fragments encoding maltose-binding protein (MBP) by overlap extension PCR (Heckman and Pease, 2007) to generate a gene encoding an N-terminal fusion of MBP-NaVAb/NaV1.7-VS2A with a rigid Asn-Ala linker and cloned into pFastBac Dual vector as described (Wisedchaisri et al., 2019). Baculoviruses containing the chimera were prepared using the Bac-to-Bac protocol according to the manufacturer with Sf9 insect cells (Life Technologies).
Electrophysiology
For initial characterization of cDNAs encoding NaV1.7/NaVAb-VS2 chimeras (Figures 1D and 1E), Sf9 insect cells (Spodoptera frugiperda) were transiently transfected with NaVAb/NaV1.7-VS2 containing the mutations indicated. Glass pipettes 1.5–3 MΩ were used to patch-clamp fluorescent cells, and currents were recorded via whole-cell voltage clamp (EPC10, Pulse, HEKA), sampled at 250 kHz, and filtered at 3 kHz. Membrane capacitance ranged from 5–25 pF. Rs was below 10 MΩ, with a 2 μs lag and at least 70% compensation, and voltage error was below 10 mV. A P/4 leak subtraction protocol was used. Standard recording solutions were as follows: Intracellular (in mM), NaCl (35), CsF (105), EGTA (10), HEPES (10), pH 7.4 (CsOH); Extracellular (in mM), NaCl (140), MgCl2 (2), CaCl2 (2) HEPES (10), pH 7.4 adjusted with NaOH ([Na]Out = 146 mM). As the G/V curves for the chimeras run through the reversal potential of sodium for these solutions (35 mV), these recordings were verified in solutions where NMDG-Cl (pH 7.0; HCl) was substituted for NaCl to move the reversal potential of sodium to 0 mV (35 NaCl/35 NaCl) and 100 mV (2.8 NaCl/140 NaCl). The pH for both intracellular and extracellular solutions was adjusted with NMDG+ for these solutions. Osmolarity was adjusted with sucrose to match that of the cell growth media each day. Pulse data was analyzed using IGOR Pro (6.37).
For detailed voltage clamp studies of NaVAb/NaV1.7-VS2 chimeras (Figure 2), Hi5 insect cells (Trichoplusia ni) were infected with Baculovirus containing the chimera MBP-NaVAb/NaV1.7-VS2A. After 24–48h, whole-cell sodium currents were recorded using an Axopatch 200 amplifier (Molecular Devices) with glass micropipettes (1.5–3 MΩ). Capacitance was subtracted and 80–90% of series resistance was compensated using internal amplifier circuitry. I/V relationships of tail currents were recorded in response to steps to voltages ranging from −160 mV to 160 mV in 10-mV increments from a holding potential of −160 mV. Pulses were generated and currents were recorded using Pulse software controlling an Instrutech ITC18 interface (HEKA). Data were analysed using Igor Pro 8 (WaveMetrics). Sample sizes were chosen to give standard error of the mean (SEM) values of less than 10% of peak values based on prior experimental experience. Synthetic C-terminally amidated m3-HwTx-IV (>98% purity) was purchased from Alomone Laboratories.
Protein expression and purification
Third passage (P3) baculoviruses for MBP-NaVAb/NaV1.7-VS2A chimera were used to infect Hi5 cells in single-layer culture dishes, and the cells were incubated at 27°C for ∼72 h. Cells were harvested by centrifugation. Cell pellets from ∼20 dishes were resuspended in Buffer A (50 mM TrisHCl pH 7.5 and 200 mM NaCl) supplemented with 1 mM PMSF, 2X SigmaFast protease inhibitor cocktails, benzamidine HCl, and DNase I. Cells were lysed by sonication and membranes were solubilized with 1% high purity digitonin (Calbiochem) for 1 h at 4°C with gentle mixing. The mixture was centrifuged at 15,000×g for 30 min at 4°C, and the supernatant was incubated with amylose resin (NEB) for 1 h at 4°C with gentle mixing. The resins were washed with Buffer B (Buffer A supplemented with 0.06% w/v glycol-diosgenin (GDN; Anatrace)) and bound protein was eluted with Buffer C (Buffer B supplemented with 10 mM maltose). Eluted protein was concentrated to 1 ml using Vivaspin20 100kDa MWCO (Cytiva) and further purified with Superose 6 Increase size-exclusion chromatography (Cytiva) using 10 mM Tris HCl pH 7.5, 100 mM NaCl, and 0.006% GDN as a column running buffer. Elution fractions were evaluated using SDS-PAGE and peak fractions were combined and concentrated using Vivaspin6 100 kDa MWCO (Cytiva). m3-HwTx-IV was added to the chimera at 8:1 stoichiometric molar ratio of toxin to channel (8 molecules of toxin per 4 binding sites per channel), which corresponds to ∼0.2–0.3 mM of m3-HwTx-IV to ∼10 mg/ml of channel to ensure full binding occupancy. The mixture was incubated on ice for at least 30 min before grid preparation. Using this protocol, m3-huwentoxin-IV is co-eluted with MBP-NaVAb/NaV1.7-VS2A chimera on Superose 6 size-exclusion column (Figure S2A).
Cryo-EM sample preparation and data acquisition
Cryo-EM grids were prepared by applying m3-HwTx-IV: MBP-NaVAb/NaV1.7-VS2A complex in GDN detergent to glow-discharged holey carbon grids (Quantifoil Au R1.2/1.3, Quantifoil Micro Tools GmbH, Germany). Grids were blotted for 2.5 to 4.0 s using Vitrobot Mark IV (Thermo Fisher Scientific) and immediately plunge-frozen in liquid ethane cooled by liquid nitrogen. Cryo-EM data were recorded on a Titan Krios microscope (Thermo Fisher Scientific) operated at 300 kV, equipped with a GIF-quantum energy filter (Gatan) at 20 eV slit width and a K2 Summit direct detector (Gatan). LEGINON (Suloway et al., 2005) was used for automated data collection. Movies were collected at a nominal magnification of 130,000x in super-resolution mode resulting in a pixel size of 0.528 Å, with a small defocus range of −0.5 to −2.5 μm. The dose rate on the camera was set to be ∼8 counts per physical pixel per second. The total exposure time was 8.6 s (0.2 s/frame), leading to a total accumulated dose of 60 electrons per Å2 on the specimen (Table S1).
Cryo-EM image processing
Movie frames were aligned and 2x binned to a pixel size of 1.056 Å using MotionCor2 (Zheng et al., 2017), and the contrast transfer function parameters for each motion-corrected image were estimated using Gctf (Zhang, 2016). Subsequent image-processing steps were performed using RELION (Scheres, 2012) on an NVIDIA GPU-accelerated workstation. Particles were auto-picked using templates derived from 2D class averages that were initially generated from manually picked particles from ∼50 images. A total of ∼1.47 million particles from 7,168 good images were extracted into 256 × 256-pixel boxes and subjected to several rounds of 2D classification to remove bad particles (Figure S2C). 3D classification and refinement were carried out in RELION from 849,942 particles after 2D classification using the cryo-EM structure of NaVAb that had been low-pass filtered to 60 Å as an initial model. The resulting 3D reconstructions were routinely better than 4.5 Å resolution. Subsequently, ∼500k particles from a homogeneous class after RELION 3D classification and refinement were subjected to cycles of global and local refinement in cisTEM (Grant et al., 2018) using a reconstruction from RELION as a starting reference with the resolution limit set to 7.5 Å for particle alignment, and using a 3D mask that included the transmembrane and toxin regions while low-pass filtered the region outside (e.g. MBP, NaVAb C-terminal tail, and detergent micelles) to 20 Å. The resolution was estimated using the Fourier shell correlation (FSC) between independently refined half-maps with a criterion value of 0.143 (Henderson et al., 2012) to be 3.6 Å (Figure S2D). Local resolution was evaluated using ResMap with two half maps as inputs (Kucukelbir et al., 2014) (Figure 3A).
Model building and refinement
Crystal structure of NaVAb/NaV1.7-VS2 with ProTx-II bound in the activated state (PDB 6N4I) was cleaned up to remove ProTx-II and small molecule ligands from the coordinates and subsequently docked into cryo-EM density map using Chimera (Pettersen et al., 2004). The atomic model was then rebuilt and locally refined using Coot (Emsley et al., 2010). NMR structure of m3-HwTx-IV (PDB 5T3M) (Rahnama et al. 2017) was docked into density for toxin on each voltage sensor initially by manual fitting, followed by rigid body fitting in Coot. The atomic model was subsequently refined using real space refinement in Phenix (Adams et al., 2010) with secondary structure restraints, noncrystallographic symmetry restraints, and reference model restraints of both main chains and side chains from the NMR structure of m3-HwTx-IV (Figure S3D and Table S1).
Structural analysis
Molecular contacts with distances within 5 Å were analyzed using program Contact in CCP4 Interface program suite (Potterton et al., 2003). Protein interfaces were analyzed using the program PISA (Krissinel and Henrick, 2007). Structure figures were made with Pymol (Schrodinger) and UCSF Chimera (Pettersen et al., 2004).
QUANTIFICATION AND STATISTICAL ANALYSIS
Analysis of electrophysiological data
Peak current at each voltage was averaged and plotted as a function of the stimulus voltage to yield a current vs. voltage (I/V) relationship. When the I/V curves contained only outward current, the reversal potential (Vrev) was verified with a separate protocol measuring the tail currents at peak activation. The instantaneous current of the tail current family was plotted as a function of voltage, fit with a line near 0 mV, and the X-intercept was used as Vrev to generate the conductance vs. voltage (G/V) curve from the I/V curve by calculating G=I/(Vm-Vrev). Normalized G/V curves were fit with a simple two-state Boltzmann equation, 1/(1+exp(V1/2-Vm)/k), in which Vm is the stimulus potential, V1/2 is the half-activation voltage, and k is a slope factor. I/V plots of inward currents were fit with (Vm-Vrev)*(Imin/(1+exp((Vm-V1/2)/k)) to generate the Boltzmann curve fit to normalized G/V. Points within 10 mV of the reversal potential were omitted for the fit.
Estimation
Protein concentrations were estimated using an A280 extinction coefficient of 33,920 M−1 cm−1 on a spectrophotometer.
Global resolution estimation of cryo-EM density map is based on the 0.143 Fourier Shell Correlation criterion.
Supplementary Material
KEY RESOURCES TABLE.
| REAGENT or RESOURCE | SOURCE | IDENTIFIER |
|---|---|---|
| Bacterial and Virus Strains | ||
| E. coli BL21(DE3) | NEB | Cat# C2527I |
| E. coli DH10Bac | ThermoFisher Scientific | Cat# 10361-012 |
| Chemicals, Peptides, and Recombinant Proteins | ||
| Amylose resin | NEB | Cat# E8021S |
| Digitonin, High Purity | Millipore Sigma | Cat# 300410 |
| Glycol-diosgenin (GDN) | Anatrace | Cat# GDN101 |
| m3-huwentoxin-IV (m3-HWTX-IV) | Alamone Labs | Cat# STH-102 |
| Deposited Data | ||
| Coordinates of NaVAb/NaV1.7-VS2A: m3-HwTx-IV | This study | PDB: 7K48 |
| Cryo-EM Map of NaVAb/NaV1.7-VS2A: m3-HwTx-IV | This study | EMDB: EMD-22661 |
| Experimental Models: Cell Lines | ||
| Spodoptera frugiperda (Sf9) | Life Technologies | B825-01 |
| Trichoplusia ni (High Five) | Life Technologies | B855-02 |
| Oligonucleotides | ||
| EcoRI-MBP forward primer: CGCGCGGAATTCATGAAAATCGAAGAAGGTAAACTGG | Integrated DNA Technologies (IDT) | N/A |
| MBP-NA1-NaVAb reverse primer: GTAATTGCAAGATACATAGCATTAGTCTGCGCGTCTTTCAGGGC | Integrated DNA Technologies (IDT) | N/A |
| MBP-NA1-NaVAb forward primer: GCGCAGACTAATGCTATGTATCTTGCAATTACAAATATTGTAG | Integrated DNA Technologies (IDT) | N/A |
| NaVAb-HindIII reverse primer: CGACAAGCTTTTATTAGTTTTTTAAACTAGTTTTTATTAATTCTTTAAG | Integrated DNA Technologies (IDT) | N/A |
| Recombinant DNA | ||
| pFastBacDual MBP-NaVAb/NaV1.7-VS2A | This study | N/A |
| pIZT GFP-P2A-NaVAb/NaV1.7-VS2 | This study | N/A |
| pIZT GFP-P2A-NaVAb/NaV1.7-VS2A | This study | N/A |
| Software and Algorithms | ||
| CCP4i 7.0.068 | CCP4 | http://www.ccp4.ac.uk |
| Chimera 1.11.2 | UCSF | https://www.cgl.ucsf.edu/chimera |
| CisTEM 1.0.0-beta | CisTEM | https://cistem.org |
| Coot 0.8.9.1 | MRC | https://www2.mrc-lmb.cam.ac.uk/personal/pemsley/coot |
| Gctf | MRC | https://www.mrc-lmb.cam.ac.uk/kzhang |
| IGOR Pro 6.37 | WaveMetrics | https://www.wavemetrics.com |
| Leginon 3.3 | NRAMM | http://leginon.org |
| MotionCor2 | UCSF | https://msg.ucsf.edu/software |
| Phenix 1.14-3260 | Phenix consortium | https://www.phenix-online.org |
| Pymol 1.7.2 | Schrödinger | https://pymol.org |
| Relion 3.0 beta | MRC | https://www2.mrc-lmb.cam.ac.uk/relion |
| ResMap | Kucukelbir et al., 2014 | http://resmap.sourceforge.net/ |
Highlights.
Tarantula toxin and voltage-shifting mutations trap resting state of NaV1.7 chimera
The toxin forms a high-affinity complex with the S3-S4 linker of the voltage sensor
Huwentoxin inserts a key lysine like a ‘stinger’ into a triad of negative charges
The structure vividly illuminates the molecular mechanism of voltage-sensor trapping
The results offer an initial molecular template for future design of analgesic drugs
ACKNOWLEDGEMENTS
We thank Joel D. Quispe and Quinton Beedle (University of Washington Cryo-EM Facility) for technical assistance on cryo-EM, and Dr. Jin Li (Department of Pharmacology, University of Washington) for technical and editorial support. This research was supported by National Institutes of Health research grants R01 NS015751 (W.A.C.), R35 NS111573 (W.A.C.), and R01 HL112808 (W.A.C. and N.Z.), research training grant T32 GM007750 (E.M.), and by the Howard Hughes Medical Institute (N.Z.).
Footnotes
DECLARATION OF INTERESTS
The authors declare no competing interests.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Data Availability Statement
Cryo-EM map has been deposited in the Electron Microscopy Data Bank (EMDB) under accession code EMD-22661. The coordinates of the atomic model have been deposited in the PDB under accession code 7K48.






