Voltage-gated potassium (Kv) channels control the selective flow of potassium (K+) across cell membranes, which is vital for electric signaling1. Kv channels are important therapeutic targets2 and are composed of four identical subunits with six transmembrane segments. The first four segments form the voltage sensor and the two terminal segments the central pore (Fig. 1a). The pore includes the selectivity filter, a conserved molecular gate that governs ion selectivity. The selectivity filter has the canonical signature sequence TVGYG conserved among all K+ channels3 and its backbone carbonyl-groups together with the threonine sidechain line up to form five K+ coordination sites S0-S44,5. The function of Kv channels is regulated by two distinct inactivation mechanisms:1,6,7,8 N-type inactivation, an auto-inhibitory process in which the pore gets blocked by a molecular plug, and C-type inactivation, a regulatory process in which the filter adopts a non-conducting conformation (Fig. 1b)6. Aberrations in C-type inactivation are closely related to neurological disorders such as episodic ataxia or the long QT syndrome9, which makes a structural framework of C-type inactivation in Kv channels desirable. The phenomenon of C-type inactivation was most clearly documented with functional measurements in the case of voltage-activated Shaker K+ channel from Drosophila melanogaster (the Shaker channel)8,10,11,12,13,14,15,16,17.

Fig. 1: C-type inactivation and selectivity filter gating.
figure 1

a Topology diagram of voltage-gated K+ (Kv) channels. Helices S1-S4 form the voltage-sensor, while helices S5-S6 form the pore comprising the selectivity filter. b Slow C-type inactivation renders the selectivity filter of K+ channels non-conductive. c The bacterial KcsA channel is a model for the pore of Kv channels. d, e The selectivity filter (T74-G79 in KcsA) and residues W67, D80 are conserved while the residue corresponding to E71 in KcsA is substituted by a valine in Kv channels.

A molecular mechanism of C-type inactivation considered representative for the central pore of K+ channels (Fig. 1c) has been established for the bacterial channel KcsA on the basis of functional measurements18,19,20, X-ray crystallography5,21,22,23,24, NMR spectroscopy25,26, and molecular dynamics (MD) simulations27,28,29,30. Under inactivating low K+ conditions, the selectivity filter of KcsA sharply constricts at the level of the central glycine (TTVGYGD) caused by a rotation of the V76-G77 plane, which prevents K+ binding at the sites S2 and S35,21. This long-lived constricted conformation is stabilized by the binding of a few water molecules into a cavity behind the filter27,31. The conductive-to-constricted transition of the selectivity filter is allosterically enhanced by the opening of the intracellular activation gate21,22,29. The broad features of a KcsA-like constricted state are recapitulated in a computational study based on homology models of the pore domain of the Shaker channel, but several differences were noted32. Clearly, C-type inactivation does not only depend on the selectivity filter signature sequence, but is exquisitely sensitive to the surrounding residues in the pore domain18,20,33,34, which differ in Kv channels and KcsA (Fig. 1d, e). Of particular interest, the critical glutamic acid E7118 along the pore helix behind the filter, known to dramatically affect inactivation kinetics of the KcsA channel18,20,21, is replaced by a nonpolar valine that is highly conserved in most Kv channels. This raises the question of whether C-type inactivation of Kv channels, by virtue of such a local change in the environment of the selectivity filter, could involve different or additional states than the familiar constriction observed in WT KcsA. Alternative mechanisms have been hypothesized and a number of recent experimental studies with K+ selective ion channel observed disorder or virtually no structural changes in the selectivity filter in inactivating conditions13,35,36,37,38,39. Furthermore, it was reported that interfering with the filter constriction under low K+ conditions does not abolish C-type inactivation40. Altogether, despite the progress, the subject remains controversial41. Putting aside the effect of voltage-sensors, the E71V mutant of KcsA offers a great opportunity to have an incisive look at the molecular environment around the selectivity filter representative to that of a Kv channel. Electrophysiological measurements20 showed that E71V KcsA is functional and exhibits C-type inactivation behavior under experimental conditions under which WT KcsA adopts a constricted selectivity filter18,21. A number of recent experimental studies challenge the canonical constricted conformation as a molecular correlate of C-type inactivation, which might not be necessarily associated with a unique selectivity filter conformation13,35,36,37,38,42. Our knowledge of the structural basis for C-type inactivation in Kv channels still needs to be firmly established.

In this work, we document a series of observations from X-ray crystallography, solid-state NMR (ssNMR), and MD simulations showing how the inactivation process in the Kv-like KcsA mutant could be supported by a mechanism that differs from that of the WT channel (Fig. 1e).


Filter narrowing in the Kv-like channel

To study the molecular mechanism of C-type inactivation in E71V KcsA, we solved X-ray structures with a closed and open intracellular gate, henceforth called closed-gate and open-gate structures (Supplementary Table 1, Supplementary Fig. 1). The E71V channel in its closed-gate conformation was crystallized, and individual crystals were subsequently soaked in low potassium solution (5 mM KCl). The structures were solved by molecular replacement using the 1K4C as a search model4,18. To determine open-gate E71V KcsA structures, the lower ends of the two long transmembrane helices (TM1 and TM2) were cross-linked via disulfide bridges formed between residue C28 of one chain and C118 of the neighboring chain, as previously described for WT KcsA23 (Supplementary Fig. 1a). The structures were solved by molecular replacement using 6W0A as a search model. Well-defined electron density maps were obtained for the transmembrane domain and the pore-loop region including the selectivity filter. Closed-gate E71V KcsA structures have resolutions in the range of 2.7–2.9 Å, whereas the resolutions of the open-gate structures are in the range of 3.0–3.3 Å.

The closed-gate E71V KcsA structure solved with 5 mM K+ (pdb 7MHR) closely matched the so-called closed-conductive structure of WT KcsA (pdb 1K4C), with an overall rmsd (root-mean-square deviation) of 0.3 Å (Supplementary Fig. 1b), displaying a closed intracellular gate together with a conductive selectivity filter, consistent with the filter of the open-conductive structure (pdb 5VK6). Note that pdb 1K4C was obtained in high K+ (150 mM) conditions. The conformation of the closed inner gate of E71V is identical to that in WT KcsA, and the Cα-Cα distance between Thr112 of the TM2 helix is 12 Å for both channels (Supplementary Fig. 1a, b). The E71V selectivity filter is similar to the WT KcsA (rmsdT74-D80 = 0.20 Å) with the exception of a widening of the pore outermost S1 site (Fig. 2a, b), with the Cα-Cα distance between opposing G79 residues being 8.7 Å in E71V and 7.9 Å in WT KcsA.

Fig. 2: X-ray structures of WT and E71V KcsA.
figure 2

a The conductive selectivity filters of WT and E71V KcsA, both with closed lower gates. b Comparison of the constricted selectivity filter of WT KcsA (with a closed lower gate) and the narrowed selectivity filter of the open-gate structure of E71V KcsA. Both structures were obtained in the absence of K+. The Cα-Cα distances between residues of opposing protomers are shown. The closed-state and open-state E71V KcsA structures were obtained with 5 mM and 0 mM K+, respectively. The green mesh shows the difference density map, the orange mesh the anomalous density. The difference (green) map is for the K+ ions and contoured at 8 σ. The orange density map (anomalous) is contoured at 5 σ. An ion cannot be clearly assigned to the density due to the weak signal. c The W67 sidechain flips in the E71V open-state structure, breaking the hydrogen bond with the D80 sidechain that is important for inactivation in Kv channels12,19,44,45.

The open-gate E71V structure (pdb 7MK6) was solved at low K+ (0 mK+/150 mM NaCl), which is an inactivating condition for KcsA5,21,22. The crystal structure globally resembles the previously described open-gate WT KcsA structures22,23,43 (Supplementary Fig. 1b). The opening extent of the inner gate is similar to an open-gate structure of WT KcsA in which TM1 and TM2 were cross-linked43, with a Cα-Cα distance at position Thr112 roughly 22.5 Å for both structures (Supplementary Fig. 1a). Strikingly, the E71V open-gate selectivity filter does not adopt the canonical constricted conformation observed in low K+ WT KcsA (pdb 1K4D) (rmsdT74-D80 = 0.67 Å) and open-gate WT KcsA structures (pdb 3F7V) (rmsdT74-D80 = 0.78 Å). As shown in Fig. 2b, the filter in the open-gate E71V structure is not constricted at the level of V76-G77. Rather, the entire filter-pore appears to be narrower in the open-gate structure compared to the closed-gate structure. The narrowing is most pronounced at the S2 site (Cα-Cα distance of opposing G77 residues reduced by 1.5 Å), and still sizeable at the S4 site (Cα-Cα distance of opposing T75 residues reduced by 0.6 Å), while the S1 site and the pore mouth (Y78-D80) are virtually unaffected. These structural features depart from the constricted filter of WT KcsA, in which the S1 and S4 sites widen as a consequence of the sharp constriction at the level of the central glycine residue. The pore-narrowing in E71V is accompanied by only small structural changes compared to the conductive filter (rmsd T74-D80 = 0.42 Å), and dihedral angles of filter residues alter by 20–25°.

Interestingly, upon opening of the inner gate of E71V, the W67 sidechain adopts an alternative rotamer conformation, breaking the hydrogen bond with D80 (Fig. 2c). Several studies reported on the importance of the W67- D80 hydrogen bond for inactivation in Kv channels12,19,44,45, and breaking this interaction enhances inactivation to different degrees. In Shaker, mutation of the corresponding residue W434 to a F results in near-constitutively inactivated channels44, whereas the corresponding mutation of W366 in Kv1.2 accelerates inactivation19, while the mutation of D317N (D80 in KcsA) in Kv7.1 abolishes ion conductance45. Presumably, the conformational change of W67 is allosterically induced by the opening of the very distant inner gate. This is supported by the observation that the F103 sidechain, an important determinant of the gate-filter allosteric coupling in KcsA22, also changes its conformation upon channel opening and moves closer to T74 (Supplementary Fig. 1c). In addition, we observed changes in the rotameric states of residues in the TM1 helix that contact the pore and TM2 helices, which hints at another layer of modulation in agreement with the allosteric framework previously described by Nimigean, Bernèche, and co-workers36.

Next, we compared inactivation gating in full-length E71V and WT KcsA using ssNMR, which enables high-resolution studies of ion channels in a fluid membrane25,26,46,47,48. High-quality ssNMR data were acquired with [13C,15N]-labeled inversely fractionally deuterated49 channels under high K+/neutral pH conditions (100 mM K+/pH7) at which channels are closed with a conductive filter (closed-conductive), and under low K+/acid pH conditions (0 mM K+/pH3-4) at which channels are open with an inactivated filter (open-inactivated)20 (Fig. 3a, b). Using our previous chemical shift assignments of closed-conductive WT KcsA as reference50, backbone assignments were obtained for all states using 3D (CANH, CONH, CAcoNH, COcaNH) and 2D CC data (Supplementary Figs. 25).

Fig. 3: Comparing inactivation gating by ssNMR.
figure 3

a Superposition of 2D NH ssNMR spectra of (a) closed-conductive (red) and open-inactivated (cyan) WT KcsA channels acquired in membranes. Arrows indicate major signal shifts of key residues. b 2D NH spectra of E71V KcsA in closed-conductive (yellow) and open-inactivated (pink) states. The E71V KcsA filter shows two conformations A and B, highlighted with blue labels, under inactivation conditions. V76, G77, and Y78 of the canonical conductive filter (1K4C) are labeled in brown for clarity. c Schematics of the changes that accompany inactivation in WT and E71V. The inactivated WT filter constricts at sites S2 and S3, accompanied by a rupture of the E71–Y78 interaction and the influx of water into a cavity behind the filter. NMR data also reveal major structural changes at the S1 site and the pore mouth. The inactivated E71V filter does not constrict like KcsA, does not feature structural water in the cavity, and shows two conformations. d Upper panel: 2D NH and 2D CC spectra of the WT filter showing large chemical shift perturbations (CSPs) of key residue Y78 upon constriction. Lower panel: HN and Cα CSPs of the open-inactivated state in reference to the closed-conductive state. Source data are provided as a Source Data file. e Same as d for E71V, which shows only small CSPs upon inactivation. Source data are provided as a Source Data file. f Residue Y82 guards the access to the cavity behind the filter. 2D CC spectra show that Y82 undergoes a conformational change upon constriction of the WT filter but is static during E71V KcsA inactivation. g 2D N(H)H ssNMR spectra to probe structural water behind the conductive (red) and constricted (cyan) WT filter, the conductive (yellow) and inactivated (pink) E71V filter, and the barium-bound E71V filter (magenta). Green stars mark the absence of structural water.

First, we used ssNMR to show that the WT KcsA selectivity filter and its environment undergo large conformational changes upon inactivation (Fig. 3c, d). As previously reported26, we observed a strong chemical shift perturbation (CSP) for the carbonyl of V76 (+2.99 ppm relative to the conductive WT filter) (Supplementary Figs. 4, 5), which is the signature for the constricted filter of WT KcsA26. In addition, we detected large CSPs for residues 1H- and 13Cα-CSPs for Y78-L81 that report marked conformational changes at the outermost S1 site at the pore mouth (Fig. 3c, d and Supplementary Fig. 6). As shown in the X-ray structure of WT KcsA (1K4D)5, these changes are caused by the loss of the E71–Y78 interaction behind the constricted filter.

Next, we used ssNMR to study selectivity filter gating in the E71V pore. The chemical shifts of the conductive filters of E71V and WT KcsA closely resemble each other except for stark local CSPs of residues W67, Y78 and D80 (Supplementary Fig. 7) that are due to the nonpolar valine residue at position of residue 71. The valine cannot maintain an interaction with Y78/D80 as in WT KcsA, leading to major conformational differences at pore mouth and S1 site in E71V compared to WT KcsA. This reasoning is consistent with the minor CSPs that we observed between conductive and inactivated selectivity filters of E71V KcsA. Since there is no interaction between V71 of the pore helix and Y78 in E71V, the pore mouth and S1 site remain largely unaffected during C-type inactivation (Fig. 3c, e). This appears to be consistent with the minor changes at the S1 site and pore mouth between closed-gate and open-gate E71V in X-ray structures. Note that the ssNMR observations for E71V KcsA are reproduced if residue E71 is replaced by an isoleucine50, encountered in some Kv channels (Fig. 3e).

The entire E71V selectivity filter shows signal splittings (Fig. 3b), which means that the pore adopts either one asymmetric or two different states under inactivating conditions. None of the two E71V filter conformations, henceforth called conformations A and B, appear to adopt the constricted conformation that WT KcsA features at the same experimental conditions5,26. This is evidenced by strong signal difference of the V76CO signature signal (+3.10 ppm in conformation A, +3.60 ppm in conformation B) compared to the constricted WT filter26 (Supplementary Figs. 35). Conformation A of the inactivated E71V filter shows marked CSPs at the S3 and S4 sites for T75CO (−1.2 ppm in reference to the E71V conductive filter) and V76Cα (+0.8 ppm), but otherwise resembles the conductive conformation (see below). Conformation B shows a major CSP for G77CO (+1.95 ppm) at the filter S2/S3 sites. The perturbations observed at T75, V76, and especially G77 appear to be consistent with the open-gate X-ray structure of E71V, which shows a pore narrowing for the S2–S4 sites, which is most pronounced at G77.

The W67 sidechain, critical for inactivation in Kv channels12,19,44,45, also shows two conformations in ssNMR spectra of E71V under inactivating conditions (Fig. 3b). Signal splittings are also observed for V84 and T85, right above the W67 sidechain in the adjacent protomer, that tightly interact51 with the E51 sidechain that plays an important role in C-type inactivation and the coupling between pore and voltage-sensor in Shaker52.

These observations match with structural changes for E51, V84, and T85 observed in the open-gate E71V X-ray structure (Supplementary Fig. 8). We also detected a second conformation for T74 that is part of the allosteric network that couples the inner gate to the filter22. Together, the ssNMR data strongly suggest that the conformations and detailed interactions of W67 and V84/T85 are modulated allosterically. Note that because the asymmetric unit of the E71V KcsA crystals contains only one monomer, the generated tetrameric biological unit is necessarily four-fold symmetric. A conformation departing from the four-fold symmetric tetramer would only be observable by X-ray if the channel crystallized in an asymmetric unit containing more than a single monomer53.

The influx of water into the cavity behind the filter, guarded by lid residue Y8223,27,31, is crucial for the long-lived inactivation of WT KcsA27,31. Using 2D 15N(1H)1H ssNMR experiments54 that monitor the proximity of rigid water to backbone amino-protons, we could confirm the presence of several water molecules behind residues V76-G79 of the WT KcsA constricted filter, while water is confined to G79 behind the conductive filter (Fig. 3g). Moreover, upon inactivation, we observed a marked signal change (+1.29 13Cβ ppm) of the Y82 sidechain, consistent with a conformational change of the lid Y8223,27,31. Conversely, no conformational change of Y82 was observed in E71V KcsA under conditions promoting inactivation (Fig. 3f). We, therefore, hypothesized that water plays a less prominent role behind the filter of Kv channels. Indeed, ssNMR experiments show that the cavity behind the inactivated E71V filter is devoid of rigid water molecules, in line with the hydrophobic nature of the valine 71 sidechain (Fig. 3g). This appears to be another major difference to inactivation in KcsA and suggests that inactivating water is not a universal feature of C-type inactivation, which aligns with observations for C-type gating in the human K2P2.1 (TREK-1) channel55 and the MthK channel56. In line with ssNMR, no water molecule was observed in the cavity behind the selectivity filter of the open-gate E71V X-ray structure. Although our ssNMR setup excludes the presence of rigid water molecules with resistance times in the microsecond range (or longer), transient visits of fast exchanging water behind the filter cannot be ruled out.

Effect of barium

We used barium to further highlight the different conformations adopted by the E71V channel under inactivating conditions compared to the WT channel. Ba2+ can serve as a very useful biophysical probe of the selectivity filter. The cation has a similar crystal radius compared to K+, yet it tightly binds to the filter and blocks ion conduction43,57,58,59,60,61.

In WT KcsA, Ba2+ primarily binds at the S4 site in both closed-gate (pdb 2ITD60 and 6W0I43) and open-gate (pdb 6W0D43) X-ray structures (Fig. 4a,b). The selectivity filter of Ba2+-bound closed-gate WT KcsA is constricted with a G77-G77 distance of 5.4 Å, similar to 1K4D. The Ba2+-bound open-gate WT KcsA corresponds to a semi-constricted filter with a G77-G77 distance of 6.0 Å with some structural deviations that occur at the T75 sidechain.

Fig. 4: X-ray structures of barium-bound WT and E71V KcsA.
figure 4

a Closed-gate and b open-gate structures of WT KcsA with Ba2+ bound at the S4 position of the selectivity filter. The filter is sharply constricted at the level of G77 in both the closed-gate and in the open-gate structures. c Closed-gate and d open-gate structures of E71V KcsA with Ba2+ bound at the S3 position of the selectivity filter. The filter is conductive in the closed-gate structure and narrows in the open-gate structure. Cα-Cα distances between like-residues in opposing protomers are indicated.

To compare the effect of the E71V mutation on the selectivity filter, the crystal structures of closed and open-gate E71V KcsA were determined in the presence of Ba2+ and in the absence of K+ (Fig. 4). In contrast to the WT KcsA, Ba2+ predominantly binds at the S3 site in both E71V structures, which is confirmed by the anomalous x-ray diffraction as shown in Fig. 4. In the Ba2+-bound closed-gate E71V structure, the selectivity filter is similar to the conductive state without Ba2+ (rmsdT74-D80 = 0.15 Å) with a G77-G77 distance of 8.2 Å (Figs. 2a, 4c). On the other hand, the open-gate Ba2+-bound E71V structure is narrowed compared to the closed-gate Ba2+-structure (Fig. 4d). This aligns with the selectivity filter narrowing observed for the open-gate E71V KcsA crystal structure in absence of Ba2+ (Fig. 2b). In addition, the open-gate E71V structures, with and without Ba2+, show the same conformational change of the W67 sidechain if compared to WT KcsA.

Next, we equilibrated E71V and WT KcsA proteoliposomes with 5 mM Ba2+ at neutral (pH7) and acidic (pH3-4) conditions to study Ba2+ binding to the closed-conductive and open-inactivated states by ssNMR. For WT KcsA at pH7, we observed major CSPs for the T75 backbone and sidechain and the V76 backbone (Fig. 5a, e, g) which implies that Ba2+ binds to the S4 site, in line with X-ray studies43,60. The signature CSP of V76CO, which reports on the constriction26, is −2.99 CO 13C ppm for the constricted filter (compared to the conductive WT filter) and only −2.03 CO 13C ppm in the Ba2+-bound filter (Supplementary Figs. 3, 4). This suggests a semi-constricted Ba2+-bound WT filter at pH7, in line with X-ray data43,60. We did not observe signal changes at acidic conditions, which implies that Ba2+ did not bind to the constricted filter. This departs from X-ray data that observe Ba2+ at the S4 site of the constricted filter, however, NMR and X-ray agree that open-gate WT KcsA adopts a fully constricted filter in the presence of Ba2+.

Fig. 5: ssNMR barium-binding studies.
figure 5

2D NH spectra of a closed-conductive WT KcsA (red), b open-inactivated WT (cyan), c closed-conductive E71V KcsA (yellow), and d open-inactivated E71V (pink). Superimposed (in gray) are 2D NH spectra after equilibration with 5 mM Ba2+ solution of the same pH as the original sample. Major Ba2+-caused signal changes are indicated by arrows. The two conformations A and B of the E71V filter under inactivating conditions are highlighted by blue labels. Blue lines show that Ba2+ binds the E71V filter with a conformation similar to conformation B at neutral and acidic pH. e, f Schematics of Ba2+ binding to the WT and E71V selectivity filters. Barium binds at the S4 site of the conductive, however not the constricted WT filter. Barium binds the conductive and the inactivated E71V filter at the S3 or S2 site. g 2D CC spectra show the effect of Barium binding to key residues T75 and G77 of the S2-S4 filter sites. h Backbone carbonyl CSPs in reference to the conductive E71V filter show that the Ba2+-bound states of E71V at pH7 and pH3 closely resemble state B of the inactivated E71V filter. Source data are provided as a Source Data file.

In contrast to WT, Ba2+ binds to the E71V filter at neutral and acidic conditions in ssNMR experiments. The chemical shifts for the Ba2+-bound E71V filter are the same at both conditions and only one filter conformation is observed (Fig. 5c, d, f, g, h) that is not constricted (V76CO = 179.82 ppm compared to 176.1 ppm in the constricted WT filter). In E71V, Ba2+ binding causes a major CSP for G77CO (+1.95 ppm relative to the conductive E71V filter) and V76NH (+1.01 ppm) at the filter S2/S3 sites (Fig. 3g, h), but only minor CSPs at S4 (T75CO = +0.21; T75α CSPs = +0.45 13C ppm). Hence, ssNMR data confirm the X-ray data that Ba2+ binds in the middle of the E71V selectivity filter (Fig. 3f), which again contrasts with WT KcsA. Surprisingly, the signals of the Ba2+-bound E71V filter conformation closely match to filter conformation B that we observed at inactivating conditions (Fig. 3c, d), with the same characteristic perturbation at G77CO (Fig. 3g, h).

While filter residues T75-D80 adopt a single, defined state in the presence of Ba2+, we detected the same peak-splitting for the network T74, W67 sidechain, V84, and T85 in Ba2+-bound open-gate E71V that we observed at inactivating conditions without Ba2+. This strongly corroborates that the break of the W67–D80 interaction is allosterically caused by the opening of the lower gate and not caused by a change in the filter conformation, because peak splittings are not observed for Ba2+-bound closed-gate E71V, and the filter conformation is the same for both Ba2+-bound channels.

Filter rigidification upon inactivation

We probed the impact of the E71V mutation on the channel dynamics in reference to the gating mode with ssNMR relaxation, which is an ideal approach to study the internal dynamics of proteins in membranes50 (Fig. 6a, b). We measured the 15N rotating-frame relaxation (R1rho) that is dominated by motion in the microsecond range62. As we recently showed50, the selectivity filter is the most dynamic membrane-embedded region in closed-conductive WT KcsA. Unexpectedly, the E71 to V substitution enhanced the dynamics of the entire closed-conductive channel, with a pronounced local surge in dynamics at V76 in middle of the filter, in direct vicinity to the V71 sidechain (Fig. 6d, e). Steric clashes between the V71, V76, and M96 sidechains could possibly cause this increase in mobility (Fig. 6c), analogous to the increase in dynamics observed in the E71I mutant caused by clashes between the I71 and W67 sidechains50.

Fig. 6: Dynamics measurements in different gating modes.
figure 6

a 15N rotating-frame ssNMR relaxation rates (R1rho) that report on slow molecular motions in closed-conductive (cc) and open-inactivated (oi) WT KcsA (red, cyan) and E71V (yellow, pink), measured at 700 MHz and 60 kHz MAS. The error bars show the standard error of the fit. Source data are provided as a Source Data file. b R1rho signal decay curves for selected filter residues. Symbols mark data points and lines represent best fits. c The valine behind the E71V filter is in direct contact with the hydrophobic V76 and M96 sidechains. d Plots of the differences in the dynamics between the closed-conductive (cc) states of E71V and WT, and for each WT and E71V the dynamics differences between their open-inactivated (oi) and closed-conductive (cc) states. Source data are provided as a Source Data file. e Illustration of the site-resolved selectivity filter dynamics. The size of the green spheres represents the R1rho relaxation rates.

Both channels are globally more rigid at inactivating conditions (Fig. 6d, e), presumably due to the opening of the lower gate, in line with EPR data that showed a stiffening of open-gate WT63. In WT, we observed a distinct local increase in the mobility of V76 at the S2/S3 sites. This means that the constriction is a flexible structural element, which aligns with computational results28. In contrast to WT, all residues of the S2 and S3 sites in E71V rigidify upon inactivation. Differences are also visible for the pore mouth and the S1 site that rigidify in WT upon inactivation, but are unaffected in E71V, which aligns with the absence of conformational changes at the E71V KcsA pore mouth. These data show that not only the filter structure, but also the filter dynamics differ between E71V and WT KcsA. We also observed a significant difference for G77 between states A (~14 ms−1 R1rho) and B (~20 ms−1 R1rho) of E71V (Fig. 6a). This agrees with G77 being the residue with the most pronounced chemical shift difference between A and B states (Fig. 5h).

Outlook from MD

To expand our perspective of the conformations accessible to the E71V pore, 0.5 μs MD simulations were carried out to examine the effect of various factors. The crystal structures reported in this study were used as starting models to carry out unbiased MD simulations. In addition to the E71V mutation, we probed the effect of different ions in the selectivity filter. In the E71V open-gate, K+ ions were located at the sites S1 and S4 with one water molecule at S2 or S3. The K+ in S1 maintained its position, however, the K+ in S4 was delocalized to S3 after 60 ns and stayed there for the remainder of the simulation. This ion movement was associated with a slight dilation in the middle of the selectivity filter. The starting model was pre-constricted with a Cα-Cα cross-subunit distances at G77 of 6.8 Å, which is used to monitor the width of the selectivity filter. The selectivity filter remained pre-constricted for 60 ns, after which the G77 Cα-Cα cross-subunit distances widened to ~8 Å to resemble the canonical conductive conformation (1K4C) stable until the end of the simulation (Fig. 7a).

Fig. 7: MD simulations for the structures of the KcsA E71V mutant in different conditions.
figure 7

a Open-gate and K+ bound, b open-gate and Na+ bound, c open-gate and Ba2+ bound, d closed-gate and Ba2+ bound, and e closed-gate and K+ bound. The first and last snapshots of the selectivity filter for each MD trajectory are respectively shown (right and left panel) in licorice representation for backbone and in van der Waals representations for K+ (purple), Na+ (orange), and Ba2+ (pink) ions. In the middle panel is the time series of the cross-subunit distance (r) between the Cα atoms of G77 of diagonally opposed monomers A and C (green), and B and D (red). Two levels representing conductive and constricted states are illustrated in black dashed line. The z-coordinate of ions in the selectivity filter are shown as solid dots (with the same colors as the conformation images). The z-coordinates of carbonyl oxygens of G79, Y78, G77, V76, and T75 are respectively shown in red lines to indicate the position of ion binding sites.

When K+ is substituted by Na+ of open-gate E71V, the sites S1-S4 of the selectivity filter were occupied interchangeably by Na+. After 320 ns, the filter adopted a constricted conformation with one Na+ still bound at the site S4 (Fig. 7b). In contrast to the simulation of the open-gate E71V with K+ ions, the selectivity filter gradually converted from a canonical conductive to a constricted filter when K+ is substituted by Na+, similar to the constricted X-ray structure of KcsA previously observed at low K+ (1K4D)5. The G77 Cα-Cα cross-subunit distances decreased from ~8 Å to ~5.4 Å at 320 ns, which coincides with the unbinding of a Na+ ion from site S1 (Fig. 7b). Remarkably, unlike the constricted form of WT KcsA, the selectivity filter of the E71V mutant constricts in an asymmetric fashion. This is shown by the green and red traces illustrating the cross-subunit distances from the opposite pairs of the monomers (Fig. 7b). Additional studies reported similar asymmetrically constricted conformation in other K+ channels64. A previous computational study of the pore domain of Shaker also provides indications of a structural heterogeneity associated with the constricted state of E71V;32 the free energy minimum in the 2D-PMF is an elongated basin covering both symmetrical and asymmetrical conformations (see Fig. 6 and S3 of ref. 32. and the methods for details of the 2D-PMF calculations).

We report crystal structures with Ba2+ binding at S3 of the selectivity filter of E71V KcsA in the open and closed gate E71V KcsA, which is not commonly observed. Therefore, it is of interest to gauge the conformation of the selectivity filter under those conditions using MD simulations. In open-gate E71V, Ba2+ stably binds to the selectivity filter at site S3 for 500 ns with Na+ (from the bulk solution) briefly binding to the outer sites of the selectivity filter (Fig. 7c). The selectivity filter adopts a conductive state, but notably this conformation was not stable throughout the 500 ns simulation. The G77 Cα-Cα cross-subunit distances show that the filter cross-subunit distances fluctuate between 6 and 9 Å (Fig. 7c, maximum near 400 ns) due to the conformational instability and deviation of the upper filter (Y78 to D80) in some subunits. Moreover, the selectivity filter is slightly narrower when compared with the canonical conductive filter (1K4C)5. For the closed-gate E71V with Ba2+ or K+ ions, the conformation of the selectivity filter is highly stable during 500 ns MD simulations. In both trajectories, Ba2+ or K+ ions predominantly bound at the same sites as the initial conformation (Fig. 7d, e). In comparison with the other simulations, the selectivity filter of the closed-gate E71V bound with Ba2+/K+ was very stable with a G77 Cα-Cα cross-subunit distance of ~8 Å, indicative of a canonical conductive filter5,65.

W67 as a molecular switch

In the open-gate E71V crystal structures, the W67 sidechain is flipped 180o compared to WT KcsA, consistent with the ssNMR data (Fig. 3b). To understand this conformational difference from a dynamical perspective, the orientation of W67 was monitored in all the trajectories. Based on the analysis, W67 in the open-gate E71V accessed multiple rotamer conformations (Fig. 8). Starting from the equilibrated crystal structure and throughout the 500 ns simulation, the side chain of W67 in the open-gate E71V was very dynamic in nature. This dynamic behavior was observed in the simulations of open-gate E71V with K+, Na+ or Ba2+ (Fig. 8a–c). Unlike the crystal structure, the conformation of W67 sidechain in the simulations of open-gate E71V was not confined to a certain conformation throughout the MD simulation. Rather, the side chain of W67 adopted multiple rotamer configurations. The high mobility of W67 in the open-gate E71V could be attributed to the orientation of W67 side chain. The 180o flipping of W67 side chain prevents its Nε1-Hε1 group from forming a hydrogen bond with the carboxylate group of D80, which is needed to stabilize the configuration of W67 and D80, as well as for maintaining the structural integrity of the whole selectivity filter. In closed-gate E71V with Ba2+, the conformation of W67 in the crystal structure is identical to that in the WT KcsA of previous structures (1K4C, 1K4D). In the simulation, it is observed that the mobility of the W67 is significantly less than in the open-gate E71V simulations due to the stability of the hydrogen bond between W67 and D80 (Fig. 8d). The range of observed conformations of W67 in the crystal structures and ssNMR, indicates that this sidechain may access multiple rotameric states in the open-gate E71V. However, this is not the case in the closed-gate KcsA, presumably because the hydrogen bond restrains the mobility of W67.

Fig. 8: The dynamics of the W67 and D80 side chains in MD simulations.
figure 8

a Open-gate and K+ bound, b open-gate and Na+ bound, c open-gate and Ba2+ bound, d closed-gate and Ba2+ bound, and e closed-gate and K+ bound. The crystal structures are shown as reference (labeled with their PDB ID) in licorice representation and carbon atoms in white with multiple snapshots from simulations. The side-chain conformations are shown in red licorice, and these snapshots are selected for every 100 ns in all four subunits.

Unbiased MD simulations provide a powerful albeit limited way to explore the conformations accessible to a molecular structure; a 0.5 μs trajectory is likely to sample mainly the conformations around a meta-stable free energy basin. To more quantitatively assess the conformational preferences of the selectivity filter, free energy landscapes PMFs were calculated. The results shown in Fig. 9 represent extensions of previous calculations29,32. The computations are designed to allow a comparison of the WT and E71V mutant channels with fully open gate (23 Å measured by Cα-Cα distance between T112). To obtain the free energy landscape, two-dimensional potential of mean force (2D-PMFs) were performed using US/H-REMD simulations as a function of the Cα––Cα cross-subunit distance of G77 in the filter (coordinate r) and the position of the external K+ ion along the pore axis (coordinate z). To compare the propensity between the conductive conformation with K+ ion bound at S2 site and constricted structure with K+ at S1 site, two most typical occupancy observed in previous structures, the 2D PMFs only focus on the region covering the outer binding sites S1 and S2 (between 0 and 6 Å along the z coordinate).

Fig. 9: Free energy landscapes to assess the conformational preferences of the selectivity filter of WT and the E71V KcsA mutant as a function of intracellular gate opening.
figure 9

a 2D PMF depending on two coordinates. The horizontal reaction coordinate r describes the width of the selectivity filter and is defined as the average cross-subunit pinching distance between the Cα atoms of G77. The vertical reaction coordinate z indicates the position of the external K+ ion along Z axis relative to the center of the selectivity filter. Extensions of previous calculations29,32. b 1D PMF projected along the horizontal reaction coordinate r (after Boltzmann integration of the vertical reaction coordinate z).

The calculated 2D PMFs clearly show the relative population differences for the conductive and constricted conformations between WT and E71V mutant (Fig. 9a). For WT, there is a deep free energy minimum around r = 5.4 Å corresponding to a stable constricted state, but no clear free energy basin in the conductive structural region (r ≈ 8.2 Å). It is reasonable to imagine that the selectivity filter would tend to spontaneously interconvert from the conductive to the constricted conformation for WT with an open intracellular gate, going downhill on the free energy surface (Fig. 9b). For E71V mutant, there is a clear minimum in the conductive region (r ≈ 8.2 Å), and the free energy difference is only 1.5 kcal/mol between the conductive and constricted minima. These features are broadly consistent with previous computational results obtained using a homology model of the pore domain of the Shaker channel32. The comparison of these two free energy landscapes (WT vs E71V) indicates that, although the constricted conformation is favorable for both E71V and WT in the open structure, there is a higher probability to capture a conductive conformation for E71V mutant than WT. The presence of a single inactivating water near the bottom of the filter frees the backbone of Y78 and G79 from hydrogen bonding constraints, which reduces the stability of the constricted state compared to the canonical constricted conformation of the WT (1K4D). This is consistent with a previous functional study showing that E71V is less inactivated than WT19. It is also consistent with ssNMR data showing a shift of the V76CO signal in the conductive E71V filter (179.8 13C ppm in E71V; 179.0 13C ppm in WT KcsA) (Supplementary Fig. 5), which, as we recently showed50, relates to a stabilization of the conductive filter. Interestingly, the free energy basin of constricted states is shallower and broader for E71V than WT, suggesting that the constricted state in E71V could represent a larger set of heterogeneous ensemble than WT.


Using a combination of X-ray, ssNMR, and MD simulations the behavior of the E71V KcsA mutant was investigated. While the overall sequence identity between KcsA and the pore of mammalian Kv channels is on the order of 40%, the valine along the pore helix behind the filter is highly conserved among Kv channels suggesting that it is an important molecular determinant of function. X-ray crystallographic structures show that the filter of the open-gate E71V KcsA channel is narrowed but not constricted. This observation is in line with our ssNMR data, which also does not reveal the presence of the constricted filter conformation in inactivating conditions. In contrast with the canonical constricted state, the absence of bound water molecules behind the narrowed filter is noteworthy. Both X-ray and ssNMR unambiguously show the absence of the constricted state for the E71V KcsA whereas the MD simulations indicate that this conformation is possible. While a constricted state for the E71V filter is not captured by our experiments, it is difficult to rule out this possibility: a conformation extensively documented in the case of the WT KcsA should be physically accessible to the E71V mutant.

X-ray data with bound Ba2+ confirm that the substitution of E71 by a nonpolar valine alters the local selectivity of the cation binding sites and filter gating. The open-gate WT filter is constricted in the presence of Ba2+, which then either binds at the S4 site43 or, as shown by ssNMR, cannot bind at all to the filter. By contrast, the filter of open-gate E71V accommodates Ba2+ at the S3 site without constriction. The binding in the middle of the filter seems consistent with studies reporting that Ba2+ tightly binds to C-type inactivated Shaker and becomes trapped in its selectivity filter66,67. In line with our data, Ba2+ binding in the middle of the filter was observed for the MthK68 and NaK2K69 channels that both have a valine at the position corresponding to E71 in KcsA. A structure of the MthK channel with constricted filter could never be captured37, although this appears to be explained by differences in ion binding affinity38. In a similar vein, recent ssNMR studies show that NaK2K under low K+ conditions (0 mM K+) adopts a disordered selectivity filter and not the constricted filter of WT KcsA39. The ssNMR studies of NaK2K also reported a marked change in the filter dynamics under inactivation conditions. Interestingly, the selectivity filter of NaK2K seems more dynamic in the disordered (perhaps inactivated) than in the canonical state, while the filter in open-inactivated E71V KcsA becomes more rigid.

X-ray, ssNMR, and MD simulations show that the W67-D80 interaction behind the filter, critical for inactivation in Kv channels12,19,44,45, breaks in E71V KcsA under inactivating conditions upon opening of the inner gate, consistent with the allosteric coupling between the activation gate and the selectivity filter21,22,29. On the other hand, the W67-D80 interaction is intact in the constricted conformation of WT KcsA (1K4D), which aligns with the diverging role of W67: replacing W67 slows down inactivating in WT KcsA, whereas it promotes inactivation in Kv channels19. Another interesting observation is that ssNMR data unambiguously show, based on Cαβ chemical shifts (Fig. 3e), that the Y78 sidechain changes its conformation in E71V KcsA upon inactivation. Changes in the sidechain of F627 in hERG, equivalent to Y78 in KcsA, were suggested to modulate the inactivation mechanism42,70 and emulate the role of structural water molecules behind the filter. Consistent with this observation, we also recently showed that Y78 exhibits strongly enhanced dynamics if residue E71 in KcsA is replaced by an isoleucine50, which is representative for channels like Kv2.1. Against this background, it generally seems that there is more to learn on the role of the sidechains behind the selectivity filter environment, given that the of substitution of a glutamic acid to a nonpolar valine at position 71 in the channel (Fig. 6d) drastically increases the overall dynamics of the pore by a mechanism that we do not yet fully grasp.

Strikingly, ssNMR data show that the E71V selectivity filter can adopt two conformations under inactivating conditions (Figs. 3b, 5h). This could either mean the presence of two different symmetric conformations, or alternatively, a single asymmetric conformation. Non-symmetric filter conformations have been related to inactivation gating in the KcsA G77dA28, TREK-155, hERG42,64, and KcsA channels71. The MD trajectories of open-gate E71V KcsA display a filter that departs from 4-fold symmetry (Fig. 7) and the calculated 2D-PMF shows a lower energy barrier in between constricted and conductive filter than in WT KcsA (Fig. 9). Both of these factors could promote a more heterogeneous sampling of the conformational space in E71V. The heterogeneity of the inactivated E71V filter also aligns with a previous computational study32, and could be caused by the absence of inactivating water molecules behind the filter or by the rupture of the W67-D80 interaction. A potential reason why a second conformation in open-gate E71V KcsA was not observed by X-ray could be due to the presence of the stabilizing Fab fragments bound in the pore mouth vicinity which could impair some of the natural conformational sampling18, as recently shown by ssNMR50.

In pondering the different pieces of information, one should make clear that asking whether the E71V mutant can adopt or not the constricted filter conformation, and what is the true molecular mechanism of inactivation of this mutant are two distinct questions. With respect to the first question, the small magnitude of the energy difference between conductive and inactivated state in E71V KcsA must certainly be taken into consideration. The macroscopic current in E71V KcsA after a stimulus decays to about 57% from the peak current20, corresponding to a free energy difference between the conductive and non-conductive functional states of about 0.17 kcal/mol. The ssNMR experiments are carried out with the full-length channel, which inactivates less deeply than the truncated form used for X-ray crystallography and MD simulations29. The intracellular gate of the full-length opens only up to 19 Å whereas the truncated form used to calculate the 2D-PMF has a gate opening of 23 Å (Fig. 9), which allosterically promotes inactivation (a smaller gate opening would allosterically shift the equilibrium toward the conductive state). Moreover, the channel crystals include the presence of Fab antibodies that destabilize the inactivated state18. With respect to the second question, it seems likely that there exists some non-constricted state of the E71V filter that is functionally non-conductive—a state that is associated with the functional phenotype of inactivation observed in the electrophysiological experiments. Strengthening this interpretation is the fact that the sample probed by ssNMR, with a full-length KcsA E71V channel incorporated into a fluid membrane, reflects faithfully the conditions imposed by the functional electrophysiological measurements (apart from the non-equilibrium ion current that perhaps promotes entry into C-type inactivation), including natural channel–channel interactions that seem to affect the gating of WT KcsA72,73. Ultimately, the existence of a nonconductive (inactivated) state associated with the flipping of a filter-lining carbonyl group cannot necessarily be ruled out for all K+ channels with a valine at position 71. In particular, a computational study from Thompson et al.74 concluded that in the MthK channel, which has a valine at the position corresponding to E71 in KcsA, the rotation of the filter-lining carbonyl group in a K+-depleted filter results in a non-conductive (perhaps inactivated) state.

Choosing to wander on the side of caution, we conclude that there seems to exist at least two conformational states of C-type inactivation in the case of the Kv-like E71V mutation of KcsA. There is the familiar conformation in which the filter is constricted at the level of the central glycine, and there is a second conformation in which the filter is not constricted but slightly narrowed over its entire length. Such a non-conductive and non-constricted conformation was recently buttressed by some experimental studies with Kv channels13,35,36,37,38. While it is generally non-trivial to imagine how a non-constricted filter could act to robustly inhibit K+ current, the concept has been discussed previously by Nimigean, Bernèche, and co-workers36. Although this scenario is not captured by MD simulations (the narrowed pore can rapidly relax in the presence of K+), the concept of a non-conductive narrowed filter in the Kv-like channel is supported here by a transition from a highly dynamic conductive filter to very rigid filter under inactivating conditions, as indicated by ssNMR. Like in a bench vise, the four rigidly and compactly packed E71V protomers would block the passage of K+ through the filter. Coupling between pore helix and transmembrane helices could modulate the packing of the filter36. The presence of the voltage-sensor may further affect the packing of the pore-domain and the relative stability of different inactivated states.


Crystallization and structure determination

The open-gate E71V KcsA was expressed as reported in Cuello et al.23. The pQE32 expression vector containing the coding sequence for E71V closed-gate KcsA channel was transformed into E. coli strain XL-1 Blue cells. Fresh LB media was inoculated from an overnight culture and grown at 37 °C with shaking until reaching an OD600 of 0.8–1.0, after which expression was induced by adding 0.5 mM isopropyl-β-D-thiogalactopyranoside (IPTG). Growth was continued for 3 h at 37 °C. After this step the open- and closed-gate KcsA were treated similarly. Cell pellets were resuspended in lysis buffer (20 mM Tris, pH 8.0; 0.2 M NaCl) supplemented with 1 mM PMSF and 20 μg/ml of DNase I. The resuspended cells were lysed by homogenization using an Avestin Emulsiflex C5. The cell membranes were collected by centrifugation at 100,000 × g at 4 °C for 1 h. The membrane pellet was resuspended in 20 mM Tris, pH 7.5, 0.15 M KCl and solubilized by incubation with 40 mM DM (n-Decyl-β-D-maltoside) overnight at 4 °C. The sample was centrifuged at 100,00 × g for 1 h and the supernatant was loaded on a HisTrap FF 5 ml nickel metal affinity column previously equilibrated with buffer A (20 mM Tris, pH 7.5, 0.15 M KCl, 5 mM DM, 20 mM imidazole) and eluted with buffer B (buffer A + 300 mM imidazole). The C-terminal tail was removed by incubation with 1 μg/ml chymotrypsin for 1 h at room temperature. The chymotrypsin-treated protein was further purified by size exclusion chromatography using a Superdex 200 HR 10/30 column with an AKTA FPLC system (GE Healthcare) in buffer C (50 mM Tris, pH 7.5, 0.15 M KCl, 5 mM DM). The peak fraction was collected and incubated with KcsA-Fab and size exclusion chromatography was repeated to remove excess Fabs. To obtain KcsA under Ba2+ conditions, the purified KcsA-Fab complex was incubated with 5 mM BaCl2 prior to crystallization and the KCl is replaced by 0.15 M NaCl in the final size exclusion chromatography buffer.

The KcsA-Fab complex was concentrated to 15 mg/ml and crystallized in 50 mM magnesium acetate, 50 mM sodium acetate pH 5.5 and 25% PEG 400 at 20 °C. After 5 days, crystals were harvested and soaked in a cryoprotectant solution containing 40% PEG 400 for 1 min at room temperature. This step was repeated three times followed by flash-freezing in liquid nitrogen. X-ray diffraction datasets were collected at the NECAT 24-ID-C beamline at the Advanced Photon Source. Crystal structures were determined by molecular replacement using the structures 1K4C and 6W0A as search models. The anomalous difference Fourier maps were calculated using Phenix. The structure refinements were performed using REFMAC. The electron density map and KcsA models were inspected by COOT.

Solid-State NMR spectroscopy

Inversely Fractionally deuterated49 WT KcsA and E71V mutant channels were expressed in E. coli M15 cells (Qiagen) using H2O-based M9 medium supplemented with 15NH4Cl and D-glucose-13C6-d7. Cells were subsequently harvested, treated with lysozyme, and lysed via French press. The membranes containing the channels were collected by centrifugation (100,000×g) and proteins were extracted with 40 mM DM75. Channels were purified using Ni-NTA agarose beads (Qiagen). Liposome reconstitution was performed using E. coli polar lipids (Avanti) at 1:100 protein:lipid molar ratio co-solubilized in DM, in which the detergent was removed using polystyrene beads (Bio-Beads SM-2)75. Before the ssNMR measurements, reconstituted samples were suspended in phosphate buffer (pH 7.4, 100 mM K+) or citrate buffer (pH 3-4, 0 mM K+). Ba2+-binding studies were conducted with HEPES buffer (pH 7, 5 mM BaCl2) and citrate buffer (pH 4, 5 mM BaCl2) to probe closed-gate and open-gate states, respectively. Samples were incubated in the buffers for 2 days.

3D ssNMR experiments50 (CANH, CONH, CAcoNH, COcaNH) for sequential backbone assignments were performed at 800 MHz (1H-frequency) using 60 kHz magic angle spinning (MAS) frequency and a real temperature of ~305 K. 2D 13C–13C PARISxy76 experiments for side chain chemical shift assignments were performed at 700 MHz using 42 kHz MAS and a 13C–13C mixing time of 110 ms. 15N T1rho relaxation experiments were run at 700 MHz and 60 kHz MAS using a 15N spin lock amplitude of 17.5 kHz50. PISSARRO77,78 decoupling was used in all detection dimensions. 2D 15N(1H)1H ssNMR experiments54 using 1.5 ms 1H1H spin diffusion transfer was used to probe the presence of structural water behind the filter.

MD simulations

The open and closed-gate crystal structures of the KcsA E71V mutant obtained in the present study were used as the starting model for MD simulations. The channel was embedded in a bilayer of 3POPC:1POPG lipids and solvated in 150 mM NaCl using the web service CHARMM-GUI79. Most residues were assigned their standard protonation state at pH 7. The total number of atoms in the atomic model is on the order of 41,000. The all-atom CHARMM force field PARAM36 for protein80,81,82,83, lipids84, and ions85 was used together with the TIP3P water model86. The atomic channel models were refined using energy minimization for at least 2,000 steps, and the ions and backbone atoms (except those from the selectivity filter) were kept fixed throughout the minimization procedure. All the simulations were performed under NPT (constant number of particle N, pressure P, and temperature T) conditions at 310 K and 1 atm, and periodic boundary conditions with electrostatic interactions were treated by the particle mesh Ewald method87,88 and a real-space cutoff of 12 Å. The simulations use a time step of 2 fs, with bond distances involving hydrogen atoms fixed using the SHAKE algorithm89. After minimization, positional restraints on all the Cα atoms were gradually released after which a trajectory of 500 ns was generated using NAMD version 2.1390,91. The biased simulations to calculate the two-dimensional (2D) potential of mean force (PMF) surfaces were generated with Hamiltonian replica-exchange MD (US/H-REMD)92 using the multiple-copy facility of NAMD93 and were unbiased using the weighted histogram analysis method (WHAM)94,95. Analysis was carried out using the program VMD96.

Reporting summary

Further information on research design is available in the Nature Research Reporting Summary linked to this article.