The selectivity filter is an essential functional element of K+ channels that is highly conserved both in terms of its primary sequence and its three-dimensional structure. Here, we investigate the properties of an ion channel from the Gram-positive bacterium Tsukamurella paurometabola with a selectivity filter formed by an uncommon proline-rich sequence. Electrophysiological recordings show that it is a non-selective cation channel and that its activity depends on Ca2+ concentration. In the crystal structure, the selectivity filter adopts a novel conformation with Ca2+ ions bound within the filter near the pore helix where they are coordinated by backbone oxygen atoms, a recurrent motif found in multiple proteins. The binding of Ca2+ ion in the selectivity filter controls the widening of the pore as shown in crystal structures and in molecular dynamics simulations. The structural, functional and computational data provide a characterization of this calcium-gated cationic channel.
Potassium (K+) channels are tetrameric membrane-spanning proteins that provide a selective pore for the conductance of K+ across the cell membranes1. The X-ray structure of the bacterial channel KcsA from Streptomyces lividans revealed that the permeation pathway comprises a narrow pore lined exclusively by main chain carbonyl oxygens2. Formed by the residues corresponding to the signature sequence TTVGYG, common to all K+ channels3,4, this essential functional element serves as an ion-conducting selectivity filter, allowing only the passage of nearly dehydrated K+ ions. While the X-ray structures of K+ channels determined subsequently greatly expanded our knowledge, these efforts have so far revealed only a small number of possible conformations for the selectivity filter. The conformation that is predominantly observed is the ‘ion conductive state’. First revealed by the X-ray structure of KcsA2, this conformation of the selectivity filter has been subsequently observed in a number of K+ channel pore domains, including KcsA2,5,6,7,8, Kv1.2 (refs 9, 10), MthK11,12, KvAP13, KirBac14, and Kir3.1 (ref. 15). Two additional conformations observed exclusively in crystal structures of the KcsA channel are the ‘constricted’ and the ‘flipped’ conformations. The constricted or pinched conformation is thought to correspond to a C-type inactivated state of the channel. It has been observed at low [K+]5, and in the presence of tetraethylammonium, a classic quaternary amine channel blocker16, as well as in a series of structures in which the intracellular gate of the channel was open17. The flipped conformation has been observed in crystal structures of the non-inactivating mutant E71A7,18. Thus, only three conformational variants of the selectivity filter have been observed, so far, by X-ray crystallography. In contrast, molecular dynamics (MD) simulations suggest that the selectivity filter of K+ channels undergoes considerable thermal fluctuations and can explore a broad range of conformations. Nevertheless, it is difficult to grasp the significance of these computational results because only a limited fraction of the landscape of conformations accessible to the selectivity filter of a K+ channel has been mapped out by X-ray crystallography.
Additional information about the structure of related channels with similar sequences can contribute to a better understanding of the conformational landscape of the pore. Implicit in this view is the assumption that the structural diversity displayed by the members of a family of homologous proteins is representative of the structural dynamics displayed by these proteins19. In this regard, the conformational variants displayed by the non-specific NaK channel, a distant homologue of K+ channels, has helped expand our knowledge of these systems20,21. Its selectivity filter exhibits extensive structural variability20,21,22,23,24, converting in response to specific mutations from a fairly wide hydrated pore20 to a KcsA-like conductive conformation22. An important concept emerging from these studies is that the selectivity filter of tetrameric cationic channels is a complex functional element able to display considerable structural polymorphism and conformational plasticity. While there is an increasing amount of structural data about the broad family of tetrameric 2-transmembrane (TM) pore domains, the extent of the complete conformational landscape of the selectivity filter remains unclear.
Pursuing this strategy, we sought to discover and characterize additional related channels by searching the genomic databases. We specifically focused on 2-TM bacterial channels forming a tetrameric pore domain with a sequence homology below 30% with channels of known structures and with selectivity filters that departed markedly from the highly conserved canonical signature sequence TTVGYGDLMP3,4. One particular channel from the bacterium Tsukamurella paurometabola (Uniprot ID: D5UM26) with an unusual proline-rich selectivity filter sequence, LPMGNGPLSP, attracted our attention. Here, we present a characterization of this cationic channel, hereafter referred to as NaKTs. The crystallographic structure determined at 3.15 Å displays Ca2+ ions bound to the channel tetramer within the selectivity filter. Functional assays and electrophysiological recordings show that it is a non-selective cationic channel and that Ca2+ binding is necessary for channel activation and gating. The key Ca2+ binding motif is formed by an unusual helix-turn structural motif that has not been previously observed in other channels. MD simulations show that Ca2+ ions are stable inside the filter and their presence affects the widening of the pore. The gating mechanism involving Ca2+ binding in the selectivity filter adds to the molecular repertoire of possible machinery that nature uses to turn channels on and off.
Homology to the K+ channel family
The NaKTs channel belongs to the family of channels with fourfold symmetric tetrameric pore domains. The subunits display a simple 2-TM topology, M1-pore-M2, in which a long pore loop is located between two TM helices. The selectivity filter of the NaKTs channel is formed by the uncommon proline-rich sequence, LPMGNGPLSP. A search of the non-redundant database (NCBI and UNIPROT) did not discover other channels with a similar sequence, suggesting that this feature is fairly specific to this particular channel. Despite the difference, the NaKTs ion channel is nonetheless clearly a member of the broad K+ channel family, with a high homology to many important channels, as shown by the multiple sequence alignment of the NaKTs channel and other K+ channel family members (Fig. 1a). The pore region of NaKTs has 30% sequence similarity with that of NaK, a channel that can be mutated into a KcsA-like conductive pore. A phylogenetic tree generated by considering only the sequence of the pore loop region shows the close relationship of NaKTs to the members of the K+ channel family (Fig. 1b). On the basis of this analysis, it appears that the pore region of the NaKTs channel is most similar in terms of primary sequence to that of the CNG, hERG, K2P, MthK and Kir channels. This overall similarity suggests that the conformational variants adopted by NaKTs are likely to be of relevance for the entire K+ channel family.
Structure determined by X-ray crystallography
The crystallographic structure of the NaKTs channel determined at 3.15 Å resolution is shown in Fig. 2. The structural model is complete over all regions, except for residues 1–3 at the N-terminal and residues 107–123 at the C-terminal regions (the latter might have been cleaved by chymotrypsin digestion). In its broad features, the structure of the NaKTs channel is similar to that of other tetrameric pore domains, with a TM helical segment-labelled M1 (residues 21–45), a pore helix (residues 49–62), the selectivity filter (residues Pro63-Met64-Gly65-Asn66-Gly67-Pro68) and a M2 helix (residues 73–101). In addition, an amphipathic helical segment-labelled M0 (residues 5–19) is located at the N-terminal end of the subunit. The channel is in a conformation with an open intracellular gate, with a strong bend of ∼50° near the centre of the M2 helix (Fig. 2b). While the open conformation of NaKTs is similar to that observed in previous X-ray structures of other channels11, the strongest bend in the M2 helix occurs at the level of residue Val87 rather than at the level of a glycine residue proposed to act as a conserved gating hinge in several channels (Supplementary Fig. 1). The narrowest point along the intracellular vestibule occurs at the level of residue Val92, its side chain pointing towards the central channel axis. The diameter is on the order of 10 Å, which is slightly smaller than that observed in other channels in an open conformation, for example, NaK (10.3 Å at Phe92) and MthK (12.9 Å at Ala88)21. The M2 helix also displays a twist of ∼12° with respect to the open conformation of the NaK channel (3E86), but of only ∼3° with respect to the open conformation of the MthK channel (4HYO) (Supplementary Fig. 2). These structural differences regarding the intracellular activation gate suggest that some aspect of the gating mechanism of NaKTs may differ from other channels. Furthermore, an amphipathic helical M0 segment (residues 5–17) docks against the hydrophobic surface of the pore domain. In this configuration, the N terminus of the protein reaches across the membrane region to interact with Phe41 from a neighbouring subunit near the extracellular side. It seems unlikely that M0 affected the overall geometry of the pore, as it is very similar to that of other tetrameric channels. While this orientation is stabilized by a number of interactions (Supplementary Fig. 3), it is probably not representative of a membrane-bound conformation of the channel. In MD simulations including the M0 segment, water molecules rushed into the membrane interior along the pore domain to solvate charged residues (Lys9 and Arg10). Most likely, the amphipathic M0 segment should be parallel to the membrane interface25.
Cation conducting pore
The ion-conducting pore of NaKTs is aligned with the fourfold symmetry axis of the tetramer, consistent with the structure of other channels in the family2. However, the selectivity filter is formed by four extended polypeptide chains, each containing a proline-rich sequence LPMGNGPLSP that is not commonly observed in other homologue channels (Figs 1 and 2d). The overall topology of the pore loop is similar to that of other tetrameric channels (Supplementary Fig. 4) although there are noticeable structural differences with other members of the tetrameric channel family (Supplementary Table 1). A superimposition of the pore region (that is, the pore helix and the filter) of the NaKTs channel with that of the KcsA channel in the conductive state (PDB id 1K4C) yields a root-mean-square deviation (RMSD) of 2.43 Å for the backbone atoms. The RMSD with other K+-selective channels (MthK, Kir2.2, Kir3.2, Kv1.2) is also on the order of 3 Å. For comparison, the RMSD among these various channels is typically much smaller, on the order of 0.5–1.0 Å. This shows that the conformation of the pore region for the NaKTs channel departs from that of other members of the tetrameric channel family. Despite these differences, NaKTs is a non-selective cationic channel according to electrophysiological recordings of the channel reconstituted in lipid membranes. The chymotrypsin-treated form of the channel that was crystallized conducts both K+ and Na+, with a measured conductance of approximately 88 and 110 pS at 200 mM of KCl and NaCl, respectively (Fig. 3a–d).
Presence of Ca2+ in the selectivity filter
A salient difference between the NaKTs channel and other members of the tetrameric channel family is the presence of Ca2+ ions, which are observed in different regions of the selectivity filter. Three different diffraction datasets were analyzed to identify different ion occupancy states (by virtue of the I4 space group symmetry, the six monomers yield three crystallographically related tetramers). A total of nine crystallographically distinct tetramers were considered in the analysis, revealing four different occupancy states, I to IV, with 0, 2, 3 and 6 Ca2+ ions, respectively (Fig. 4).
There are no ions in state I, which serves as the reference for the unoccupied pore. In state II, there are two Ca2+ ions near the extracellular side in locations corresponding to sites S0 and S1 in KcsA. The Ca2+ ion in site S0 is surrounded by four water molecules and does not interact directly with backbone oxygen atoms. The distance between the carbonyl oxygen of Gly67 and the Ca2+ ion at site 1 is about 4.9 Å, suggesting that the ion binds in this site in a hydrated form through bound water molecules.
In state III, two Ca2+ ions are bound diagonally opposite to each other 4.1 Å away from the pore axis at a site in the selectivity filter referred to as SCa (Fig. 2c), where they are coordinated by the backbone carbonyl oxygen atoms of Ser59 (distance of 2.6 Å), Leu62 (distance of 2.5 Å) and the backbone nitrogen atom of Gly65 (distance of 2.9 Å) from one subunit, and the backbone oxygen atom of Pro63 from a neighboring subunit (distance of 2.9 Å). A third Ca2+ is located at the centre of the pore in a site corresponding to S2 in KcsA. The ion is coordinated by the side chain of Asn66, which points towards the pore of the selectivity filter. The OD1 atom of Asn66 interacts with the Ca2+ ion and the ND2 atom of Asn66 interacts with the backbone carbonyl oxygen atom of Leu69. In state IV, there are four Ca2+ ions in SCa and two additional Ca2+ ions, one in the site corresponding to S3 in KcsA near Gly65 and a second ion near Pro63 (a different sub-state is seen with the ion position shifted by 2.1 and 1.1 Å towards the intracellular surface). Lastly, there is a tetramer with a single Ca2+ ion located at the centre of the intracellular vestibule with no ions observed in the pore, as observed in the KcsA and NaK structures, assigned to State I. More details about the locations of Ca2+ ions in the 3.4 Å dataset 3 (3.4 Å resolution) and 3.6 Å dataset 1 (3.6 Å resolution) crystal structures are provided in Supplementary Fig. 5. The Ca2+ ion occupancy along the selectivity filter pore and SCa site were refined using SAD anomalous data and their respective ion occupancy is given in Supplementary Table 2.
Structural and functional response to the binding of Ca2+
The crystallographic and MD data indicate that the diameter of the pore at its inner and outer ends, defined respectively from the backbone Cα–Cα distance of residues Pro63 and Pro68 from diagonally-opposing subunits, is sensitive to occupancy by Ca2+ ions in the pore (Fig. 5). The diameter of the inner pore increases by 1–1.2 Å in response to the binding of a Ca2+ ion at site SCa, in the vicinity of Pro63, Gly65, Ser59 and Leu62. Once a Ca2+ ion binds to this position, Pro63 sways by about 0.5 Å away from the ion-conduction pathway. If one assumes that widening the selectivity filter transforms the channel from a non-conductive (or poorly conductive) state to a conductive state, Pro63 thus appears as a key residue responsible for channel activation upon the binding of Ca2+ at the SCa sites. Of relevance to these observations, functional measurements of the channel reconstituted in lipid bilayers show that Ca2+ is absolutely required for ion-conduction activity, with a K1/2 of ∼4 mM determined from the open-channel probability (Fig. 3e,f). The observed mean open-channel probability appears to be slightly sensitive to the membrane potential (around 0.25 at negative voltages and 0.6 at positive voltages with 2.5 mM [Ca2+]). The average single-channel conductance is not significantly affected by the presence of Ca2+.
To probe the functional significance of the SCa binding site on channel activation, a chimera of the NaKTs channel with its selectivity filter (PMGNGP) replaced by the corresponding residues from the KcsA channel (TVGYGD) was engineered and purified for functional assays. Whereas no channel activity can be observed with the wild-type NaKTs unless Ca2+ is present (Fig. 3e), it is observed that this chimeric NaKTs-SFKcsA channel conducts K+ in the absence of any Ca2+ (Fig. 3g). This observation strengthens the conclusion that the binding of Ca2+ at the site SCa is directly implicated in the activation of the NaKTs channel.
Comparison with other channels shows some similarities but also important differences. A Ca2+-dependent gating located within the selectivity filter was also shown to control the K+ conduction in the MthK channel26. However, while the sequence similarity of NaKTs and MthK is high (Fig. 1a), the latter does not possess the proline (Pro63) that forms part of the SCa binding site observed in NaKTs and the filter gating observed in the MthK channel is believed to be allosterically triggered by the binding of Ca2+ to the cytoplasmic RCK domains at the intracellular side26. A recent study based on chimeric channels that replaced the selectivity filter of the bacterial non-selective cation channel NaK, TVGDGNFS, with a cyclic-nucleotide gated channel filter sequence, TIGETPPP also displayed Ca2+ block (∼14 μM)27. However, there are important differences because the key prolines in those chimeras were located toward the extracellular end of the filter, whereas the SCa binding site in NaKTs is located at its intracellular end.
Structural similarity of the SCa site with other systems
The unusual helix-turn Ca2+-binding motif forming the SCa site is a structural feature that has not been previously observed in other crystallographic structures of tetrameric ion channels. Interestingly, a large number of similar helix-turn Ca2+-binding motifs could be identified from a search via the Metal3 webserver28 (Fig. 6). Interestingly, Ca2+ appears to be functionally important for several systems where the helix-turn motif is found, for example, it triggers the assembly process of SbsB, a layer-forming component of the cell-wall in archaea and many bacteria29, it is essential for the enzyme activation of human transglutaminase 3, and it is required for the toxin activity of Clostridium botulinum neurotoxins30. It should be noted, however, that a large fraction of the structures with a helix-turn binding motif include coordination by negatively charged side chains, which are absent from the SCa site of the NaKTs channel. As a result, the ion binding affinity to SCa is likely to be weak. Weak ion binding affinity is generally thought to be consistent with the function of a channel, as strong binding would oppose rapid conduction. While the role of Ca2+ in NaKTs is not as a permeant ion but rather to activate the channel, low binding affinity for the site SCa is nonetheless reasonable, as it is accessible via the selectivity filter. In the case of the layer-forming protein SbsB (PDB id 4AQ1), the measured K1/2 falls within a range of 0.9–110 μM, a value that is considerably smaller than the K1/2 of ∼4 mM determined for the NaKTs channel on the basis of the open-channel probability (Fig. 3f).
To gain further insight about the structural sensitivity of the selectivity filter to the Ca2+ ions in the SCa binding sites, MD simulations of the NaKTs channel tetramer (ABDE) embedded in fully hydrated POPC bilayer membranes were carried out. Four different systems were simulated (0, 1, 2 and 4), comprising respectively zero, one, two and four Ca2+ ions bound at site SCa in the selectivity filter using the polarizable Drude force field31,32,33,34,35 with recently refined parameters for Ca2+ ions36. Equivalent simulations carried out using the nonpolarizable additive CHARMM36 (C36) force field37,38 were unstable (See METHODS for details). The system with two Ca2+ at the SCa site is shown in Fig. 7a,b. The simulations with double Ca2+ occupancy display relatively small deviation from the crystal structure when compared with the other systems (Supplementary Fig. 6b) and also retain a water-filled selectivity filter (Fig. 7a,d). In the simulations, the number of Ca2+ ions bound at the SCa sites in the selectivity filter appears to control the opening of the pore. This is observed from the distance (Dinner and Douter) between the Cα atoms (Fig. 5) and the radius profile of the pore restriction zone (Rmin), which is near residue Pro63 at the intracellular end of the filter (Supplementary Fig. 6c). In the simulations, the diameter measured across the pore between the diagonally placed Pro63 (Dinner in Fig. 5) increases as the SCa sites become occupied by Ca2+. This trend continues until two of the SCa sites are filled with Ca2+. Further increasing the number of Ca2+ at the SCa sites does not lead to a more open pore. Instead, it causes structural distortions of the filter and closure of the intracellular gate formed by M2 (Supplementary Fig. 6a). The Rmin profiles in Supplementary Fig. 6c corroborate the notion that Ca2+ binding at the SCa sites promotes the opening of the selectivity filter. Increasing the number of Ca2+ ions in the selectivity filter from zero to two leads to more and longer incidents of transient pore openings (Supplementary Fig. 6c). The correlation offers one explanation from a structural point of view for the relationship between [Ca2+] and the channel open probability Po determined from single-channel recordings (Fig. 3f). However, no ion-conduction events were observed during the MD simulations with an applied voltage. Further analysis indicates that the unfavourable electrostatic repulsion resulting from Ca2+ ion bound in the sites Sca likely blocks the passage of other cations through the selectivity filter.
Knowledge of the landscape of conformations accessible to the selectivity filter of tetrameric K+ channels remains limited. To make further progress, we present here a first characterization of a novel tetrameric ion channel, referred to as NaKTs, with an unusual proline-rich selectivity filter sequence using X-ray crystallography, electrophysiology and MD simulations. Sequence comparison suggests that, despite the differences, this channel is closely related to the members of the broad family of tetrameric 2-TM channels. The NaKTs channel was crystallized with its intracellular gate in an open state. The X-ray structures revealed the presence of Ca2+ binding sites, SCa, formed by main chain atoms of residues Pro63, Gly65, Ser59 and Leu62, near the intracellular end of the selectivity filter. A database search reveals that similar helix-turn Ca2+-binding motifs are found in multiple proteins, with a broad variation in the type of coordinating ligands involved. Single-channel recordings demonstrate that the NaKTs channel is a Ca2+-activated non-selective cation channel. Analysis of crystallographic data indicates that the presence of bound Ca2+ at diagonally-opposing sites inside the selectivity filter controls the diameter of the conducting pore. Pro63, which contributes to the SCa binding site, appears to be a key residue responsible for the channel activation triggered by the binding of Ca2+. The direct functional implication of the SCa binding site on channel activation is confirmed by engineering a chimera protein in which the classic selectivity filter of the KcsA channel has been inserted in the NaKTs channel. While no channel activity is observed with the wild-type NaKTs unless Ca2+ is present (Fig. 3e), the chimeric NaKTs-SFKcsA channel conducts K+ in the absence of any Ca2+ (Fig. 3g). The importance of Pro63 is supported by the results from MD simulations with a polarizable force field. The results from MD strengthen the view that the Ca2+ binding motif located at the base of the selectivity filter may act as an activating switch.
Paradoxically, even though the Ca2+ bound in the site SCa kept the selectivity filter in the crystallographic open state, no ion-conduction events were observed during the MD simulations with an applied voltage due to the unfavourable electrostatic repulsion from the bound Ca2+. It is also possible that the binding of Ca2+ could induce additional conformational changes not yet observed, or that the X-ray structure obtained from a chymotrypsin-treated truncated form of the protein is not fully representative of the channel probed by the electrophysiological experiments. For example, the intracellular gate of KcsA truncated is more wide-open than KcsA full-length17,39. The situation may be different in the case of the NaKTs channel, as the conductance of the truncated channel (Fig. 3a) is smaller than that of the full-length channel (Supplementary Fig. 7a). To be as consistent as possible with the crystal structure, the functional experiments were carried out with the truncated chymotrypsin-digested form of the NaKTs channel. However, additional experiments with the full-length channel NaKTs channel indicate that it exhibits a complex functional behaviour, with two major conductance levels. Furthermore, the full-length channel undergoes some degradation over time at room temperature, which may partly explain its complex functional behaviour. The smaller conductance level is observed more frequently with the truncated form of the channel while the larger level occurred more frequently with the full-length form of the channel (Supplementary Fig. 7a). Nonetheless, while the truncated form of the channel displays a more reliable functional behaviour than the full-length form, it remains somewhat complex (Supplementary Fig. 7b). It is also noticeable that the kinetic behaviour of the full-length channel is slower than that of the truncated channel. These observations suggest that there might be two open-channel conformations, and their relative probability is different in the chymotrypsin-digested and full-length form of the channel.
While Ca2+ binding at the site SCa is key for channel activation, a complex interplay between gating and conduction might take place because the permeating cations and Ca2+ must translocate through the same passageway. This suggests various mechanistic scenarios whereby the occurrence of ‘open’ conformations of the pore could be simultaneously promoted by the reversible binding of Ca2+ as well as blocked for ion conduction. In other words, the channel could display sustained periods of conduction if the lifetime of the open state persists for sufficiently long time after the dissociation of the activating Ca2+ ion(s). The intriguing mechanism by which Ca2+-activation and ion conduction are interrelated in the NaKTs channel will require further investigation.
In closing, while the primary objective of the present study was to characterize the structure and function of a novel tetrameric 2-TM cationic channel in relation to other K+ channels, the striking structural differences presented by the pore of the NaKTs channel (its uncommon proline-rich sequence LPMGNGPLSP is not found in human channels) could potentially offer a useful target for the discovery of specific inhibitors that may be of therapeutic interest. Tsukamurella species are Gram-positive bacilli that have been isolated from environmental samples and sludge, that can lead to human diseases40. Catheter related bloodstream infections (CR-BSI), the most common presentation of Tsukamurella species infections, primarily occur in patients with indwelling central lines and/or immune suppression41. Additional clinical malfunctions include bacteremia42,43, meningitis44, peritonitis45, and cutaneous, lung and knee prosthesis infection43,46. Tsukamurella species is also recognized as a potential pathogen in immunocompromised patients47.
Expression and purification
Genomic DNA from T. paurometabola (DSM 20,162) was obtained from the DSMZ (German Collection of Microorganisms and Cell Cultures, Braunschweig, Germany). The genomic databases search leading to the identification of a 2-TM tetrameric channel from T. paurometabola used PsiBlast48, followed by manual analysis to focus on the sequence in the selectivity filter region. The Tpau_1687 gene encoding residues 1–123 of an ion transport two domain protein was amplified by PCR and cloned into the pQE60 expression vector (Qiagen). The primers used to clone the full-length NaKTs channel into pQE60 used the NcoI and BamHI sites of pQE60. The forward primer is 5′-CGTATAAC ATGT TGGGTCTCACATTGATGTTCAAGAGATTC-3′ and the reverse primer is: 5′-CTTGTAGGATCC GTCCTCCGCCTCGGCCGAAC-3′ (restriction sites highlighted in bold and the NaKTs coding sequence is underlined). The NaKTs ion channel protein was expressed in E. coli strain XL-1 Blue cells on induction with 0.5 mM isopropyl-β-D-thiogalactopyranoside (IPTG) at 37 °C for 3 h at an OD600 of 0.6–0.8. Cell pellets were resuspended in buffer A (20 mM Tris, pH 8; 0.2 M NaCl) plus 1 mM PMSF and DNase I. Cells were lysed by homogenization. The cell lysate was clarified by centrifugation at 107,000g for 35 min at 4 °C. and the membrane pellet was solubilized by incubation at 4 °C in Buffer B (Buffer A plus 10 mM DDM (n-Dodecyl-β-D-maltoside) or 40 mM DM (n-Decyl-β-D-maltoside). The supernatant was then purified using a cobalt metal affinity column pre-washed with buffer A and 0.5 mM β-DDM. The affinity-bound protein was eluted with Buffer A containing 500 mM imidazole and 0.5 mM β-DDM. The 6 × His C-terminal tag along with the unstable cytoplasmic domain was removed from the eluted protein by incubation with chymotrypsin for 2 h at room temperature. The cleaved protein was further purified by gel filtration (buffer: 20 mM HEPES pH 8, 200 mM NaCl and 0.3 mM β-DDM). The peak fraction was concentrated to 8–25 mg ml−1 and used for crystallization. To confirm the role of the SCa binding site, a chimera NaKTs-SFKcsA channel was engineered and purified, where the selectivity filter of NaKTs (PMGNGP) was replaced by the corresponding residues from the selectivity filter of KcsA (TVGYGD) using QuikChange Site-Directed Mutagenesis (Agilent Technologies). The primers used to make the NaKTs-SFKcsA chimera are as follow. To first make a NaKTs without a selectivity filter (NaKTS-noSF), the forward primer is 5′-CTCGGTGGGATTGCTCAGCCCCACGC-3′ and the reverse primer is 5′-GCGTGGGGCTGAGCAATCCCACCGAG-3′. To insert the KcsA selectivity filter into NaKTs-noSF, the forward primer is 5′-CTCGGTGGGATTGACCGTCGGCTACGGCGACCTCAGCCCCACGC-3′ and the reverse primer is 5′-GCGTGGGGCTGAGGTCGCCGTAGCCGACGGTCAATCCCACCGAG-′3 (insertion in bold). The NaKTs-SFKcsA chimera was expressed and purified according to the same protocol as the wild-type protein.
Crystallization and data collection
Trials were carried out in the presence and absence of 5 mM CaCl2 in sitting drop 96 well, 3 drop crystallization plates (Hampton Research), using various commercially available crystallization kits (JCSG+ suite (Qiagen), Wizard I&II (Emerald Bio), HR2 110, HR2 112, HR2 136, PEG I & II (Hampton Research), HTS Screen II (Jena Biosciences)). Crystals were obtained in JCSG+ suite conditions 18 (50% PEG 200/5% PEG 1,000; 0.1 M phosphate/citrate, pH 4.2) and 22 (50% PEG 200, 0.2 M MgCl2, 0.1 M sodium cacodylate, pH 6.5). More than 150 crystals obtained at varying conditions were screened at −180 °C under a nitrogen stream. All datasets were collected on the Northeastern Collaborative Access Team beamline NECAT 24-ID-C at Advanced Photon Source (APS) of the Argonne National Laboratory (ANL) on a PILATUS 6MF detector at a wavelength of 0.97920 Å. Chymotrypsin-digested NaKTs ion channel crystals obtained in JCSG+ suite condition 18 diffracted only to 7 Å resolution. The best achievable diffraction data (3.15 Å resolution) were obtained in JCSG+ condition 22. Three different crystallographic datasets were obtained at 3.15 Å (dataset 2), 3.36 Å (dataset 3) and 3.6 Å (dataset 1) resolution and the data were processed using the HKL2000 suite49; see Table 1. NaKTs ion channels crystallized in the I4 space group and contained 6 molecules per asymmetric unit.
Three datasets were collected, labelled chronologically 1, 2 and 3, at 3.6, 3.15 and 3.4 Å resolution, respectively. For each dataset, the asymmetric unit contains six distinct subunits (monomers labelled A, B, C, D, E, F), which can be used to generate three complete tetramers: Tetramer 1 is formed by subunits A, B, D and E; tetramer 2 is formed by chain C and chains G, H and I generated by crystallographic fourfold symmetry from chain C; tetramer 3 is formed by chain F and chains J, K and L generated by crystallographic fourfold symmetry from chain F. For dataset 2 (PDB ID: 5CBG), the structure solution was determined by molecular replacement with PHASER in the PHENIX program50 using the pore helix (residues 49–61) of NaK (PDB ID: 2AHY) structure as an initial model. Automated model building was performed using the PHENIX-Autobuild program and repeated cycles of model building were done using COOT51. Structure refinement was done using REFMAC 5.5 in the CCP4 suite of programs52. Calcium ions were located based on Fo−Fc difference map peak at 4.5σ cutoff and water molecules at 3σ cutoff. The water molecules were also located based on the Coot:find water facility in REFMAC (CCP4 6.5.001) and finally checked manually using the electron density map in COOT51. The N-terminal residues 1–4 and C-terminal residues 107–123 were disordered. The final model contains six monomers (A, B, C, D, E and F) of residues 5–106 and 8 Ca2+ ions refined to Rcryst and Rfree of 23.6 and 29.3%, respectively, with no outliers in disallowed regions of the Ramachandran plot. Two additional crystal structures, at 3.4 Å (dataset 3) and 3.6 Å (dataset 1) resolution, were determined by molecular replacement, using the NaKTs 3.15 Å crystal structure as an initial search model followed by repeated cycles of model building in COOT and refinement with REFMAC 5.5 in the CCP4 suite of programs. For dataset 3 (PDB ID: 5CBH), the N-terminal residues 1–4 and C-terminal residues 107–123 were disordered in the crystal structure. The final model contains six monomers (A, B, C, D, E and F) of residues 5–106 and 8 Ca2+ ions refined to Rcryst and Rfree of 23.2 and 26.2%, respectively, with no outliers in disallowed regions of the Ramachandran plot. Tetramer 1 (Chain ABDE) contains four Ca2+ ions located at site SCa and two Ca2+ ions at sites 2 and 3. Tetramer 2 (Chain CGHI) has no ions in the pore. Tetramer 3 (Chain FJKL) contains two Ca2+ ions located at sites S0 and 1. For dataset 1 (PDB ID: 5CBH), the N-terminal residues 1–4 and C-terminal residues 107–123 were disordered in the crystal structure. The final model contains six monomers (A, B, C, D, E and F) of residues 5–106 and three Ca2+ ions and refined to Rcryst and Rfree of 23.87 and 27.9%, respectively, with no outliers in disallowed regions of the Ramachandran plot. Tetramer 1 (Chain ABDE) contains two Ca2+ ions bound diagonally opposite to each other at site SCa and 1 Ca2+ ion bound at site 2. Tetramer 2 (Chain CGHI) and Tetramer 3 (Chain FJKL) have no ions in the pore.
Determination of calcium ions
Calcium ions (Ca2+) were identified based on the Fo−Fc map at 4.5σ cutoff. A cluster of Ca2+ ions was observed at the centre of the hexamer of tetramer assembly (overall molecular packing). Calcium positions in all of the three crystal structures were initially identified based on the Fo−Fc difference map peak at 4.5σ cutoff and confirmed by calculating an anomalous density map using SAD phasing in CNS program53,54. Anomalous maps were calculated by calcium anomalous scattering values (f′=0.3002 and f″=0.5654) at λ=0.9792 Å using calcium positions obtained from the refined NaKTs ion channel structures at 3.15, 3.4 and 3.6 Å resolution and further confirmed by random anomalous peak search procedure. Anomalous density peaks >10.0σ cutoff were also observed for the cluster of calcium ions located at the centre of the hexamer of tetramer assembly. The calcium ion sub-structure occupancy refinement was performed using SAD data in REFMAC 5.5 in the CCP4 suite of programs. The calcium ion occupancy along the ion-conduction pathway and their corresponding B-factor values are reported in Supplementary Table 2. All structure figures were generated in PyMOL (http://www.pymol.org/).
All single-channel recording and analysis experiments were carried out using Port-a-Patch patch clamp system (Nanion Technologies GmbH, Munich, Germany). Planar lipid bilayers were obtained from GUVs prepared by using the electroformation method55 in an indium tin oxide (ITO) coated glass chamber connected to the Nanion Vesicle Prep Pro setup (Nanion Technologies GmbH, Munich, Germany). A mixture of 10 mM DPhPC (2-diphytanoyl-sn-glycero-3-Phosphocholine, Avanti Polar Lipids Inc.) and 1 mM cholesterol, dissolved in chloroform, was deposited on the ITO-coated glass surface and air-dried. After complete evaporation of the solvent, the lipid film was rehydrated with 210 μl of 1 M sorbitol. GUVs were formed by electroswelling using an alternating electric field of amplitude 3 V, 5 Hz for 2 h. GUVs were collected and used directly for the reconstitution of the ion channel. Purified chymotrypsin-treated NaKTs channel was reconstituted into the GUVs solution to a final concentration of 40 μg ml−1. Giga-ohmic seals were formed within a few seconds by pipetting 5 μl of the protein-GUVs on the micro-structured glass patch clamp NPC-1 Chips by Nanion. Channel activity was recorded under symmetric conditions (unless otherwise stated) using 20 mM HEPES, pH 7.5, 0.2 M NaCl/KCl as the internal solution and 20 mM MOPS, pH 4, 0.2 M NaCl/KCl, as the external solution. The channel is active only at pH 4 (MOPS & HEPES); no current was detected at pH 7.5 (HEPES). The data were filtered at 3 kHz (Bessel filter, HEKA amplifier) digitized at a sampling rate of 50 kHz and analyzed with ClampFit (Axon Instruments, part of Molecular Devices, USA). Ionic currents were observed only after adding Ca2+ in the external solution. All I/V curves were determined using a voltage sweep procedure in which the membrane potential was changed from −40 to +40 mV in steps of 20 mV lasting 20 μs. Open-channel probability was measured as a function of Ca2+ concentration, with internal solution containing 20 mM HEPES, pH 7.5, 0.2 M NaCl and the external solution containing 20 mM MOPS, pH 4, 0.2 M NaCl. External CaCl2 was applied using a multichannel perfusion system linked to the Port-a-Patch. The membrane potential was held at −40 mV and the current recordings were measured using CaCl2 concentrations of 1, 2, 3, 4, 5, 7.5, 10, 12.5 and 15 mM. Single-channel currents were recorded from multiple patches for 1–3 min per Ca2+ concentration using continuous acquisition mode. The Po were calculated as the fraction of open time over a total time interval during which there is channel activity. For each Ca2+ concentration, about 3–5 separate time intervals of ∼200 ms were analyzed and the error on the Po was estimated as the mean-square deviation from the average. Single-channel recordings on the chimeric NaKTs-SFKcsA channel were carried out according to the same procedure.
Building the NaKTs channel–membrane systems
The POPC bilayers systems for MD simulations were built from the crystal structure of NaKTs using the Membrane Builder module56 in CHARMM-GUI57. The N-terminal M0 helix was not included; its inclusion resulted in water penetrating the lipid bilayers according to preliminary simulations (5 ns). The protein-membrane complex was solvated by an equal molar mixture of KCl and NaCl solutions with a cation concentration of 1 M (that is, [K+]=[Na+]=0.5 M). Each of the four protein subunits was patched with an acetylated N terminus and an amidated C terminus. The resulting system comprises ∼50,000 atoms (80 × 80 × 78 Å3). The ABDE tetramer in dataset 2 has two Ca2+ placed diagonally against each other at the SCa site. It was used to generate the double SCa occupancy system while also serving as the prototype for making the zero, single and full (that is, Ca2+ at all four SCa sites) SCa occupancy systems.
Equilibration of the NaKTs channel systems
Initial equilibration simulations were performed in the NPT ensemble with constant pressure (1 atm along the Z axis) and temperature (300 K) with the NAMD program58 version 2.9. The time duration for each equilibration simulation is 10 ns. The pressure of the system was controlled by the hybrid Nosé–Hoover Langevin piston method. Langevin dynamics thermostat with a 1 ps−1 damping coefficient was used to keep the temperature constant. The van der Waals interactions were smoothly switched off at 10–12 Å by a switching function and the electrostatic interactions were calculated using the particle-mesh Ewald method with a mesh size of ∼1 Å. Harmonic positional restraints were applied to the protein backbone atoms and the bound Ca2+, keeping the structural deviation from the crystal structure to a minimum. This was necessary because it prevents the channel from closing. The force constant of the harmonic potential was set to 5 kcal mol−1 Å−2 Further equilibration of 100 ns for each system was performed on Anton with the volume and temperature of the system kept constant. Harmonic positional restraints with a force constant set to 5 kcal mol−1 Å−2 were applied to the backbone and the SCa Ca2+ atoms to prevent the filter from collapsing. The Nosé–Hoover thermostat was used to maintain the system temperature at 300 K59. The lengths of all bonds involving hydrogen atoms were constrained using M-SHAKE60. The cutoff of the van der Waals and short-range electrostatic interactions was set to 16.21 Å as suggested by the guesser script. Long-range electrostatic interactions were evaluated using the k-space Gaussian split Ewald method61 with a 64 × 64 × 64 mesh. The r-RESPA integration method62 was employed and long-range electrostatics were evaluated every 6 fs. The additive C36 force field37,63 was used in both the NAMD and Anton equilibration simulations.
Simulation of the Drude model systems
After equilibration, each system was then converted to its Drude model representation using the Drude Prepper module in CHARMM-GUI57 with the TIP3P water molecules replaced by the polarizable water SWM4-DNP (ref. 32). The generated Drude model systems of the NaKTs channel were equilibrated using the input scripts provided in the CHARMM-GUI Drude Prepper module. The production afterwards was carried out using NAMD2.9 with the Drude polarizable model implemented64. The simulation protocols were analogous to those during the initial equilibration with constant pressure (1 atm along the Z axis) and temperature (300 K), except that a dual Langevin thermostat was used to keep the Drude particle at 1 K (ref. 64). The first 2.5 ns of each production was TM potential (Vmp) free. Following it was a 30 ns production run with a Vmp of either 500 or −500 mV to investigate ion permeation. The MD simulations based on the polarizable force field were stable within a 30-ns duration. This is in stark contrast with the restraint-free NaKTs channel simulations based on the nonpolarizable force field, in which the Ca2+ ions at the SCa site started to dissociate in a much shorter time scale, leading to a rapid collapse of the selectivity filter.
Simulating the hydration of pore Ca2+ ions
To examine the hydration structure of Ca2+ ions within the selectivity filter pore, four additional systems were constructed starting from the crystal structures showing four occupancy states (I to IV in Fig. 4). The setup procedure was the same as described above. Each system was equilibrated for 375 ps with reducing harmonic restraints asserted on protein heavy atoms and the Ca2+. At the end of the equilibration, the force constant of the harmonic restraints was 2 kcal mol−1 Å−2. It was kept the same in the 30-ns production simulations. A Langevin thermostat and a Monte Carlo barostat were used to maintain the system temperature and pressure at 300 K and 1 atm. Both the equilibration and the production were performed with the OpenMM6.2 program65 on GeForce GTX 780 Ti GPU processors.
Coordinates and structure factors have been deposited in the Protein Data Bank under accession codes 5CBF (dataset1), 5CBG (dataset2) and 5CBH (dataset3). Remaining data are available from the corresponding author upon reasonable request.
How to cite this article: Dhakshnamoorthy, B. et al. Structural and functional characterization of a calcium-activated cation channel from Tsukamurella paurometabola. Nat. Commun. 7:12753 doi: 10.1038/ncomms12753 (2016).
Hille, B. Ion Channels of Excitable Membranes 3rd edn (Sinauer, 2001).
Doyle, D. A. et al. The structure of the potassium channel: molecular basis of K+ conduction and selectivity. Science 280, 69–77 (1998).
Heginbotham, L., Abramson, T. & MacKinnon, R. A functional connection between the pores of distantly related ion channels as revealed by mutant K+ channels. Science 258, 1152 (1992).
Heginbotham, L., Lu, Z., Abramson, T. & Mackinnon, R. Mutations in the K+ channel signature sequence. Biophys. J. 66, 1061–1067 (1994).
Zhou, M., Morais-Cabral, J. H., Mann, S. & MacKinnon, R. Potassium channel receptor site for the inactivation gate and quaternary amine inhibitors. Nature 411, 657–661 (2001).
Zhou, M. & MacKinnon, R. A mutant KcsA K(+) channel with altered conduction properties and selectivity filter ion distribution. J. Mol. Biol. 338, 839–846 (2004).
Cordero-Morales, J. F. et al. Molecular determinants of gating at the potassium-channel selectivity filter. Nat. Struct. Mol. Biol. 13, 311–318 (2006).
Uysal, S. et al. Crystal structure of full-length KcsA in its closed conformation. Proc. Natl Acad. Sci. USA 106, 6644–6649 (2009).
Long, S. B., Campbell, E. B. & Mackinnon, R. Crystal structure of a mammalian voltage-dependent Shaker family K+ channel. Science 309, 897–903 (2005).
Long, S. B., Tao, X., Campbell, E. B. & MacKinnon, R. Atomic structure of a voltage-dependent K+ channel in a lipid membrane-like environment. Nature 450, 376–382 (2007).
Jiang, Y. et al. The open pore conformation of potassium channels. Nature 417, 523–526 (2002).
Ye, S., Li, Y. & Jiang, Y. Novel insights into K+ selectivity from high-resolution structures of an open K+ channel pore. Nat. Struct. Mol. Biol. 17, 1019–1023 (2010).
Jiang, Y. et al. X-ray structure of a voltage-dependent K+ channel. Nature 423, 33–41 (2003).
Kuo, A. et al. Crystal structure of the potassium channel KirBac1.1 in the closed state. Science 300, 1922–1926 (2003).
Nishida, M., Cadene, M., Chait, B. T. & MacKinnon, R. Crystal structure of a Kir3.1-prokaryotic Kir channel chimera. EMBO J. 26, 4005–4015 (2007).
Lenaeus, M. J., Vamvouka, M., Focia, P. J. & Gross, A. Structural basis of TEA blockade in a model potassium channel. Nat. Struct. Mol. Biol. 12, 454–459 (2005).
Cuello, L. G., Jogini, V., Cortes, D. M. & Perozo, E. Structural mechanism of C-type inactivation in K(+) channels. Nature 466, 203–208 (2010).
Cheng, W. W., McCoy, J. G., Thompson, A. N., Nichols, C. G. & Nimigean, C. M. Mechanism for selectivity-inactivation coupling in KcsA potassium channels. Proc. Natl Acad. Sci. U S A 108, 5272–5277 (2011).
Sali, A. Modeling mutations and homologous proteins. Curr. Opin. Biotechnol. 6, 437–451 (1995).
Shi, N., Ye, S., Alam, A., Chen, L. & Jiang, Y. Atomic structure of a Na+- and K+-conducting channel. Nature 440, 570–574 (2006).
Alam, A. & Jiang, Y. High-resolution structure of the open NaK channel. Nat. Struct. Mol. Biol. 16, 30–34 (2009).
Sauer, D. B., Zeng, W., Canty, J., Lam, Y. & Jiang, Y. Sodium and potassium competition in potassium-selective and non-selective channels. Nat. Commun. 4, 2721 (2013).
Derebe, M. G. et al. Tuning the ion selectivity of tetrameric cation channels by changing the number of ion binding sites. Proc. Natl Acad. Sci. USA 108, 598–602 (2011).
Liu, S. & Lockless, S. W. Equilibrium selectivity alone does not create K(+)-selective ion conduction in K(+) channels communications. Nature 4, 2746 (2013).
Cortes, D. M., Cuello, L. G. & Perozo, E. Molecular architecture of full-length KcsA: role of cytoplasmic domains in ion permeation and activation gating. J. Gen. Physiol. 117, 165–180 (2001).
Posson, D. J., Rusinova, R., Andersen, O. S. & Nimigean, C. M. Calcium ions open a selectivity filter gate during activation of the MthK potassium channel. Nat. Commun. 6, 8342 (2015).
Lam, Y. L., Zeng, W., Derebe, M. G. & Jiang, Y. Structural implications of weak Ca2+ block in Drosophila cyclic nucleotide-gated channels. J. Gen. Physiol. 146, 255–263 (2015).
Valasatava, Y., Rosato, A., Cavallaro, G. & Andreini, C. MetalS(3), a database-mining tool for the identification of structurally similar metal sites. J. Biol. Inorg. Chem. 19, 937–945 (2014).
Baranova, E. et al. SbsB structure and lattice reconstruction unveil Ca2+ triggered S-layer assembly. Nature 487, 119–122 (2012).
Eswaramoorthy, S., Kumaran, D., Keller, J. & Swaminathan, S. Role of metals in the biological activity of Clostridium botulinum neurotoxins. Biochemistry 43, 2209–2216 (2004).
Lamoureux, G. & Roux, B. Modeling induced polarization with classical Drude oscillators: theory and molecular dynamics simulation algorithm. J. Chem. Phys. 119, 3025–3039 (2003).
Lamoureux, G., Harder, E., Vorobyov, I. V., Roux, B. & Mackerell, A. D. Jr. A polarizable model of water for molecular dynamics simulations of biomolecules. Chem. Phys. Lett. 418, 245–249 (2006).
Yu, H. et al. Simulating monovalent and divalent ions in aqueous solution using a drude polarizable force field. J. Chem. Theo. Comp. 6, 774–786 (2010).
Chowdhary, J. et al. A polarizable force field of dipalmitoylphosphatidylcholine based on the classical drude model for molecular dynamics simulations of lipids. J. Phys. Chem. B 117, 9142–9160 (2013).
Lopes, P. E. et al. Force field for peptides and proteins based on the classical drude oscillator. J. Chem. Theo. Comp. 9, 5430–5449 (2013).
Li, H. et al. Representation of ion–protein interactions using the drude polarizable force-field. J. Phys. Chem. B 119, 9401–9416 (2015).
Klauda, J. B. et al. Update of the CHARMM all-atom additive force field for lipids: validation on six lipid types. J. Phys. Chem. B 114, 7830–7843 (2010).
MacKerell, J. A., Feig, M. & Brooks, C. 3rd Improved treatment of the protein backbone in empirical force fields. J. Am. Chem. Soc. 126, 698–699 (2004).
Uysal, S. et al. Mechanism of activation gating in the full-length KcsA K+ channel. Proc. Natl Acad. Sci. USA 108, 11896–11899 (2011).
Collins, M. D., Smida, J., Dorsch, M. & Stackebrandt, E. Tsukamurella gen. nov. harboring Corynebacterium paurometabolum and Rhodococcus aurantiacus. Int. J. Syst. Bacteriol. 38, 385–391 (1988).
Liu, C. Y. et al. Clinical characteristics of infections caused by Tsukamurella spp. and antimicrobial susceptibilities of the isolates. Int. J. Antimicrob. Agents 38, 534–537 (2011).
Woo, P. C., Ngan, A. H., Lau, S. K. & Yuen, K. Y. Tsukamurella conjunctivitis: a novel clinical syndrome. J. Clin. Microbiol. 41, 3368–3371 (2003).
Maalouf, R., Mierau, S. B., Moore, T. A. & Kaul, A. First case report of community-acquired pneumonia due to Tsukamurella pulmonis. Ann. Intern. Med. 150, 147–148 (2009).
Bouza, E. et al. Tsukamurella: a cause of catheter-related bloodstream infections. Eur. J. Clin. Microbiol. Infect. Dis. 28, 203–210 (2009).
Elshibly, S. et al. Central line-related bacteraemia due to Tsukamurella tyrosinosolvens in a haematology patient. Ulster Med. J. 74, 43–46 (2005).
Sheridan, E. A. et al. Tsukamurella tyrosinosolvens intravascular catheter infection identified using 16S ribosomal DNA sequencing. Clin. Infect. Dis. 36, e69–e70 (2003).
Maertens, J. et al. Catheter-related bacteremia due to Tsukamurella pulmonis. Clin. Microbiol. Infect. 4, 51–53 (1998).
Boratyn, G. M. et al. BLAST: a more efficient report with usability improvements. Nucleic Acids Res. 41, W29–W33 (2013).
Otwinowski, Z. & Minor., W. in Method in Enzymology, Macromolecular Crystallography Part A, Vol. 276 (eds Jr. Carter, C.W. and Sweet, R.M.) 307–326 (Academic, 1997).
Adams, P. D. et al. PHENIX: a comprehensive Python-based system for macromolecular structure solution. Acta Crystallogr. Sect. D Biol. Cryst. 66, 213–221 (2010).
Emsley, P. & Cowtan, K. Coot: model-building tools for molecular graphics. Acta. Crystallogr. D Biol. Cryst. 60, 2126–2132 (2004).
Potterton, E., Briggs, P., Turkenburg, M. & Dodson, E. A graphical user interface to the CCP4 program suite. Acta Crystallogr. Sect. D Biol. Cryst. 59, 1131–1137 (2003).
Brunger, A. et al. Crystallography & amp; NMR system: a new software suite for macromolecular structure determination. Acta Crystallogr. D Biol. Cryst. 54, 905–921 (1998).
Brunger, A. T. Version 1.2 of the Crystallography and NMR System. Nature Protocols 2, 2728–2733 (2007).
Angelova, M. I. in Liposome Electroformation, in Perspectives in Supramolecular Chemistry: Giant Vesicles Vol. 6 (eds P. L. Luisi and P. Walde) 26–36 (John Wiley & Sons, Ltd., Chichester 1999).
Wu, E. L. et al. CHARMM-GUI Membrane Builder toward realistic biological membrane simulations. J. Comp. Chem. 35, 1997–2004 (2014).
Jo, S., Kim, T., Iyer, V. G. & Im, W. CHARMM-GUI: a web-based graphical user interface for CHARMM. J. Comp. Chem. 29, 1859–1865 (2008).
Phillips, J. C. et al. Scalable molecular dynamics with NAMD. J. Comput. Chem. 26, 1781–1802 (2005).
Martyna, G. J., Klein, M. L. & Tuckerman, M. Nose-Hoover chains—the canonical ensemble via continuous dynamics. J. Chem. Phys. 97, 2635–2643 (1992).
Krautler, V., Van Gunsteren, W. F. & Hunenberger, P. H. A fast SHAKE: Algorithm to solve distance constraint equations for small molecules in molecular dynamics simulations. J. Comp. Chem. 22, 501–508 (2001).
Shan, Y., Klepeis, J. L., Eastwood, M. P., Dror, R. O. & Shaw, D. E. Gaussian split Ewald: A fast Ewald mesh method for molecular simulation. J. Chem. Phys. 122, 054101 (2005).
Tuckerman, M., Berne, B. J. & Martyna, G. J. Reversible multiple time scale molecular-dynamics. J. Chem. Phys. 97, 1990–2001 (1992).
Best, R. B. et al. Optimization of the additive CHARMM all-atom protein force field targeting improved sampling of the backbone phi, psi and side-chain chi(1) and chi(2) dihedral angles. J. Chem. Theo. Comp. 8, 3257–3273 (2012).
Jiang, W. et al. High-performance scalable molecular dynamics simulations of a polarizable force field based on classical Drude oscillators in NAMD. J. Phys. Chem. Lett. 2, 87–92 (2011).
Eastman, P. et al. OpenMM 4: a reusable, extensible, hardware independent library for high performance molecular simulation. J. Chem. Theo. Comp. 9, 461–469 (2013).
This research was supported by NIH-NIGMS through Grant R01-GM062342. This work is based on research conducted at the Advanced Photon Source (APS) on the Northeastern Collaborative Access Team beam lines, which are supported by a grant from the National Institute of General Medical Sciences (P41 GM103403) from the National Institutes of Health. Use of the Advanced Photon Source, an Office of Science User Facility operated for the U.S. Department of Energy Office of Science by Argonne National Laboratory, was supported by the U.S. DOE under Contract No. DE-AC02-06CH11357. We wish to express the gratitude to the staff at NE-CAT-24-ID-C and E beam lines at the Advanced Photon Source in the Argonne National Laboratory. Anton computer time was provided by the National Center for Multiscale Modeling of Biological Systems (MMBioS) through Grant P41GM103712-1 from the National Institutes of Health and the Pittsburgh Supercomputing Center (PSC). The Anton machine at PSC was generously made available by D.E. Shaw Research.
The authors declare no competing financial interests.
About this article
Cite this article
Dhakshnamoorthy, B., Rohaim, A., Rui, H. et al. Structural and functional characterization of a calcium-activated cation channel from Tsukamurella paurometabola. Nat Commun 7, 12753 (2016). https://doi.org/10.1038/ncomms12753
This article is cited by
Frontiers of Environmental Science & Engineering (2021)
In silico assessment of the conduction mechanism of the Ryanodine Receptor 1 reveals previously unknown exit pathways
Scientific Reports (2018)