The cardiac voltage-gated sodium (Nav) channel Nav1.5 is essential for cardiac excitability and conduction 1. Nav1.5 initiates the rapid influx of sodium ions from the extracellular region into the cytosol during the upstroke of the cardiac action potential. Alteration in Na+ currents has been extensively implicated in the etiology of arrhythmias 9,10. Hundreds of mutations in SCN5A, the gene encoding for Nav1.5, have been linked to arrhythmia syndromes such as Brugada Syndrome (BrS) and Long QT Syndrome type 3 (LQT3) among others 11. Hence, understanding the structure and function of Nav1.5 is pivotal for unraveling the molecular basis of cardiac electrical activity and developing targeted therapies for arrhythmias and other related disorders.
Eukaryotic Nav channels are composed of a pore-forming α subunit and auxiliary β subunits 12. The α subunit consists of four homologous domains (DI to DIV) that share significant similarities yet exhibit different functions. Each domain is composed of six transmembrane segments referred to as S1 to S6. The voltage-sensing domain (VSD, S1 to S4) and the pore-forming domain (PD, S5 to S6) are arranged in a pseudo-tetrameric manner 13,14. The N-terminal domain (NTD) and the C-terminal domain (CTD) are located in the cytosol. During a cardiac action potential, Nav channels get activated and rapidly transition into a non-conductive state known as the fast inactivated state 7. This transition occurs within 2-3 milliseconds following fast activation and it returns to the resting state upon repolarization 7.
Functional studies identified the Isoleucine-Phenylalanine-Methionine (IFM) motif in the linker between DIII and DIV (III-IV linker) as crucial for fast inactivation 15. Published structures of Nav channels showed that the IFM motif gets sequestered into a receptor binding pocket distant from the pore which leads to the proposed ‘door wedge’ model for fast inactivation 8,16-19. It was also shown that mutations that hinder the interactions between the IFM motif and its receptor binding pocket allosterically propagate to the S6 segments 8,20. Another model suggests that residues located at the intracellular end of the pore-forming S6 segment, rather than the IFM motif, cause fast inactivation 21. Published work also implied a role for the CTD in regulating sodium channel function 2,22-25. Indeed, the replacement of the native CTD of Nav1.5 with that of Nav1.4 confers inactivation kinetics that mimics Nav1.4 and vice versa 23,24,26. Additionally, the CTD has been shown to be a hotspot for LQT3 mutations that affect fast inactivation 27. Although electrophysiological and structural studies have identified critical functional elements, the molecular mechanisms underlying fast inactivation and the role of the CTD have yet to be established in the framework of full-length structures of Nav1.5, since these intracellular domains have not been resolved in published structures.
Here, we report three high-resolution cryo-electron microscopy (cryo-EM) structures of human full-length Nav1.5 (hNav1.5) in the open state. Although there has been significant advancement in the understanding of Nav1.5 function over the past three decades, our insights into fast inactivation mechanisms remain limited due to incomplete structural knowledge of the intracellular regions. Our structures show previously unseen intracellular regions of Nav1.5 including the NTD and the CTD. The open state structures feature significant conformational changes in the VSDs and exhibit high plasticity in the positioning of the CTD and the III-IV linker. Site-directed mutagenesis coupled with electrophysiological measurements indicate that disrupting the interaction between the CTD and the III-IV linker can result in compromised fast inactivation mechanisms. In summary, our findings elucidate a mechanism for fast inactivation and the role of CTD in maintaining the open state conformation.
The overall architecture of full-length hNav1.5
We purified recombinant full-length hNav1.5 from Expi293 cells (Extended Data Fig. 1a). Negative stain electron microscopy and SDS-PAGE demonstrated the purity of our protein preparations (Extended Data Fig. 1b,c). We used optimal screened grids for cryo-EM data collection. Analysis of our cryo-EM data showed significant heterogeneity owing to the flexible intracellular regions of hNav1.5. We assessed the structural heterogeneity by establishing a data processing workflow where particles were clustered into three classes (classes 1-3) based on the presence of intracellular features (Extended Data Fig. 2a). Class-1 contained high-resolution features of the core sodium channel. Class-2 and class-3 additionally contained the intracellular regions of hNav1.5 (Extended Data Fig. 2a). The processed data yielded structures of hNav1.5 with overall resolutions of ~3.2 Å for class-1 (Model-I), ~3.3 Å for class-2 (Model-II), and ~3.6 Å for class-3 (Model-III) (Extended Data Figs. 2b and 3a-d). Model-I comprises a total of 1353 residues and contains the transmembrane core, extracellular regions, the III–IV linker, portions of the I-II and II-III linker, and the NTD (Fig. 1a). Model-II and Model-III consist of 1418 residues each and contain the CTD in addition to all structural features observed in Model-I (Fig. 1b,c). The cryo-EM reconstructions show unambiguous densities for the VSDs, the selectivity filter, the pore-lining S6 segments, and the NTD (Extended Data Figs. 4-7). The CTD and other intracellular regions exhibit lower local resolutions due to their flexibility (Extended Data Figs. 2 and 7).
The a-subunit of the hNav1.5 shows a pseudo-tetrameric structure consisting of the DI to DIV domains in a domain-swapped manner (Fig. 1a-c), consistent with the overall architecture observed in published structures of Nav channels 6,8,16-18,28,29. The NTD and the CTD emanate from the transmembrane portion of the channel on the intracellular side. The NTD is located at the base of VSDI. The CTD is a compact domain that is connected to the S6-helix of the DIV via a flexible linker. The position of the CTD is variable with respect to the core transmembrane domain (Fig. 1b,c). Model-I exhibits a root-mean-square deviation (RMSD) of 0.6 Å to 0.8 Å over about 1050 Cα residues when compared to Model-II and Model-III. The RMSD between Model-II and Model-III is 0.7 Å for 1113 Cα residues. The transmembrane cores of Models-I to -III have an RMSD of 1.6 Å to 1.8 Å over nearly 1100 C-α residues compared to the human Nav1.5-E1784K structure (PDB ID: 7DTC) and show an outward movement of ~2 Å of the individual VSDs (Fig. 2a and Supplementary Video 1). This structural change is accompanied by the expansion of the pore domain (Fig. 2a and Supplementary Video 1).
Sequential activation of gating charges is coupled with fast inactivation
Capturing VSDs in different confirmations is necessary to understand the precise activation and inactivation mechanisms of Nav1.5. The VSDs in the previous open and inactive state structures of Nav1.5 show similar conformations (Extended Data Fig. 8) 17,20,30. The superposition of our models showed a gradual upward movement of gating charges (GCs) in VSDII and VSDIV caused by altered sidechain conformations (Extended Data Figs. 9 and 10). Specifically, multiple salt bridge interactions were rearranged, and two unique p-cation interactions were established between occluding residue (OR) and R4 of Model-III (Extended Data Fig. 9). Only three GCs in VSDII and VSDIV with minimal outward translocation are positioned above the OR, indicating a partially depolarized state. VSDI and VSDIII are in the depolarized conformation with three and four GCs positioned above the OR, respectively. This suggests a hierarchical pattern (S4III > S4I > S4II > S4IV) of VSD activation states as predicted in previous functional studies 31,32.
Classification of our open state structures based on the conformational spectrum of the VSDs revealed that Model-III represents a late activated state, while Models II and I represent early inactivated states of hNav1.5. Comparison of our structures with that of Nav1.5-E1784K (PDB ID: 7DTC; intermediate inactivated state) revealed a sequential shift in the side chains of GCs as they transition from the open to the fast inactivated state (Fig. 2a and Extended Data Figs. 10 and 11). This observation provides a structural framework for fast inactivation in the order of Model-III > Model-II > Model-I > Nav1.5-E1784K.
The III-IV linker and interaction with CTD
The positioning of the CTD with respect to the III-IV linker and the transmembrane core is crucial for the working mechanisms of hNav1.5. The IFM motif is loosely docked into the hydrophobic receptor pocket formed by the S4III-S5III linker and the intracellular ends of S5IV and S6IV (Fig. 2c). This positioning differs from other mammalian Nav1.5 structures as follows. First, the short α-helix that immediately follows the IFM motif and the IFM receptor exhibits a downward displacement (Fig. 2c). The IFM motif is mostly engaged in hydrophobic interactions within the receptor binding pocket (Fig. 2d). The stability of the pocket is primarily maintained by a cluster of hydrophobic residues and polar contacts (Fig. 2d,e). Altered side chain conformations of N1765, F1473, and Q1476 cause a downward shift in the IFM motif without fully displacing it from the receptor (Fig. 2f). This structural rearrangement is further stabilized by the interaction between D1484 and K1492, located in the short α-helix (Fig. 2e). Second, we observed a significant change in the conformation of the S0IV helix and the connecting loop of the III-IV linker. The N-terminal end of the S0IV moved ~4 to 6 Å outward which caused a significant displacement of the flexible loop of the III-IV linker (Fig. 3a,b). A consequence of this transition is that the IFM motif is repositioned but not displaced from the receptor despite the channel being in the open state (Supplementary Video 1).
Notably, we have resolved 100 residues of the previously unseen CTD in Model-II and Model-III in two different conformations. The CTD is positioned closer to the III-IV linker in Model III and away from the III-IV linker in Model II. The superimposition of Model-II and Model-III shows that the position of the CTD differs by ~9° (Fig. 3c,d and Supplementary Video 2). To understand the direction and magnitude of CTD flexibility, we performed normal mode analysis (NMA) on Model-II and Model-III. This analysis revealed similar dynamics of the CTD in both structures (Supplementary Video 3). The comparison with the CTD in NavPaS and NavPas-Nav1.7 chimera revealed significant differences in the positioning of the III-IV linker. In our structures, the CTD interacts with the flexible loop of the III-IV linker rather than being positioned on the short α-helix of the III-IV linker. This results in the bending of the flexible loop of the III-IV linker at residues K1504 and K1505 and causes an inward movement of the S0IV helix and the short α-helix of the III-IV linker (Fig. 3b,e and Supplementary Video 2). In Model III, both residues are positioned proximate to the negatively charged surface residues, specifically E1788 on the αI helix and E1867 on the αV helix, within the CTD (Fig. 3b). Site-directed mutagenesis coupled with electrophysiological measurements were used to assess the importance of this interface in the inactivation kinetics of hNav1.5. Our data revealed that charge reversal mutations K1540E and K1505E in the III-IV linker and E1788K and E1867K in the CTD altered hNav1.5 inactivation parameters. Mutations K1504E, K1505E and E1867K resulted in a faster time course of inactivation compared to WT (Fig. 3f, Extended Data Fig. 12a and , and Extended Data Table 2). Additionally, all four mutants produced destabilization in inactivation as illustrated by a significant hyperpolarized shift in steady-state inactivation (Fig. 3g and Extended Data Table 2). We also assessed the recovery from inactivation and one of the mutants, E1788K, displayed a slower recovery (Fig. 3h and Extended Data Table 2). While none of the mutants significantly affected current densities (Extended Data Fig. 12b), K1504E and E1867K exhibited a depolarized shift in the conductance curve (Fig. 3g and Extended Data Table 2), suggesting delayed activation. Our results show that the dynamics between the CTD and the III-IV linker are crucial for the transition of hNav1.5 from the open state to the inactivated state during the kinetic cycle.
Conformation of the two-tier hydrophobic activation gate in the open state
The opening and closing of the activation gate regulate the influx of sodium ions into the cells. In our structures, the activation gate is open. We used the position of two hydrophobic rings at the lower part of the S6 helices as a reference for the comparison of the activation gate in our three structures with the Nav1.5-E1784K (PDB ID: 7DTC, intermediate inactive state) and rNav1.5c/QQQ (PDB ID: 7FBS, open state) structures 21. The residues on the top layer are L409, L935, I1466, and I1768. The bottom layer residues are A413, L938, I1470, and I1771. In the open state structure of rNav1.5c/QQQ, the average pore diameter is 10.2 Å at the top layer and 10.3 Å at the bottom layer (Fig. 4, A and C). The average pore diameter in the upper and lower layer of Nav1.5-E1784K is 8.4 Å and 8.7 Å (Fig. 4a,c) indicative of an intermediate state. Comparison with Model-I showed that our average pore diameters at the top and bottom layer are 10.5 Å and 10.2 Å and closely resemble those of rNav1.5c/QQQ (Fig. 4a-c) 20. In Model-II, the diameter of the top layer decreased to 10.2 Å and the diameter of the bottom layer increased to 10.8 Å in Model-II (Fig. 4a and Extended Data Fig. 13). We observed an even larger activation gate diameter in Model-III, measuring 10.9 Å at the top layer and 11.0 Å at the bottom layer (Fig. 4a-c). Thus, we propose that Models I to III represent open state conformation of hNaV1.5. Notably, in all our structures, we observed a synchronized movement of the S6 helices, leading to an equivalent pore diameter of the activation gate (Supplementary Video 1). A van der Waals space-filling model shows that hydrated Na+ fits through the orifice of the activation gate in our open state structures (Extended Data Fig. 14). In summary, our structures show activation gates with average pore diameters that exceed those of published Nav1.5 structures. We attribute this characteristic to the presence of untruncated, native intracellular regions.
Distributions of disease-causing mutations in the NTD and CTD
Previous Nav1.5 structures have not resolved intracellular regions that contain the majority of Nav1.5 disease-causing mutations. However, our cryo-EM structures include the previously unresolved NTD and the CTD of hNav1.5. This allowed us to systematically map the disease-causing mutations linked to LQT3 and BrS in these regions. Analysis of mutations in the NTD and its interacting S6I helix, as well as in the CTD and its interacting III-IV linker, showed a distinct pattern of distribution in the structures (Fig. 5a and Extended Data Fig. 15). We found that mutations associated with LQT3 and BrS are dispersed evenly in the NTD (Extended Data Fig. 15) while a cluster of mutations is present in the III-IV linker and the adjacent region of the CTD (Fig. 5a,b).
Mutations in the bending region of the III-IV linker, specifically at K1505 and P1506 of the KPQ sequence, can lead to LQT3 and BrS (Figs. 3b and 5b) 3-5,33,34. P1506 is crucial in shaping the curvature of the III-IV linker, which enables the interaction between K1504-K1505 and the CTD (Supplementary Video 2). Our structures further revealed an important mutational hotspot at the C-terminal end of the III-IV linker and its connecting S0IV helix where residue R1512 engages in a p-cation interaction with F1522 in Model-III (Fig. 5c and Supplementary Videos 1 and 2). This interaction is disrupted in both Model-II and Model-I, suggesting that the p-cation interaction is transient and reliant on the conformation of the S0IV helix. Mutation R1512W can lead to a robust p-stacking interaction with F1522 that limits the flexibility of the S0IV helix and its connecting III-IV linker and leads to the reported changes in hNav1.5 kinetics in BrS 35,36. It is well-established that mutations leading to LQT3, found in regions with inactivation, often present with an increase in persistent current. Here, we observed that the introduction of mutant E1867K resulted in a significant increase in late current (Fig. 5d), further supporting the contribution of this region to cardiac channelopathies.