# Structure of the thermo-sensitive TRP channel TRP1 from the alga Chlamydomonas reinhardtii

## Abstract

Algae produce the largest amount of oxygen on earth and are invaluable for human nutrition and biomedicine, as well as for the chemical industry, energy production and agriculture. The mechanisms by which algae can detect and respond to changes in their environments can rely on membrane receptors, including TRP ion channels. Here we present a 3.5-Å resolution cryo-EM structure of the transient receptor potential (TRP) channel crTRP1 from the alga Chlamydomonas reinhardtii that opens in response to increased temperature and is positively regulated by the membrane lipid PIP2. The structure of crTRP1 significantly deviates from the structures of other TRP channels and has a unique 2-fold symmetrical rose-shape architecture with elbow domains and ankyrin repeat domains submerged and dipping into the membrane, respectively. Our study provides a structure of a TRP channel from a micro-organism and a structural framework for better understanding algae biology and TRP channel evolution.

## Introduction

Algae contribute to marine food chains (phytoplankton), form symbiotic relationships with other organisms, such as sea sponges, coral reef-forming invertebrates, or lichens, are considered ecological indicators and can be used for pollution control, detoxication, and water filtration (algae scrubber)1. Algae are sources of food rich in vitamins, minerals, and unsaturated fatty acids2,3. They are also sources of agar and alginates for the food and biomedical industries, as well as of polymers and natural pigments for the chemical industry3. In agriculture, algae can be used as fertilizers4. Finally, due to an enormous potential to produce more biomass per unit area than any other organism, algae hold promise to become a future biofuel5.

Algae are guided by multiple sensory cues, many of which are detected by membrane ion channels. Transient receptor potential (TRP) channels are ubiquitous cation-selective sensory ion channels that respond to numerous physical and chemical stimuli and are often considered polymodal signal integrators6,7,8. Several TRP channels have been identified and partially characterized in different species of algae9,10. Correspondingly, a toolkit of mammalian TRP channel agonists and antagonists has been shown to positively and negatively regulate cellular calcium uptake in Ulva compressa11 and Ectocarpus siliculosus12. Multiple TRP channels have been identified in the fresh water, biflagellate alga Chlamydomonas reinhardtii9,10. Similar to its mammalian counterpart expressed in the primary cilia of the kidney, the PKD2 channel of C. reinhardtii was shown to localize to the cell’s flagellar13. The depletion of PKD2 resulted in altered phosphorylation of a cGMP-dependent protein kinase and reduced mating efficiency13. Suppressed expression of TRP11, another TRP channel localized to the flagellar, eliminated the C. reinhardtii avoiding reaction, a reversal in swimming direction as a response to collision10.

Another previously characterized TRP channel from C. reinhardtii9, crTRP1, has not been identified in flagella but exhibited elevated expression in response to deflagellation10. crTRP1 is inhibited by classical TRP channel antagonists BCTC, La3+ and Ruthenium Red, is activated by heat and become less active upon phosphatidylinositol-4,5-bisphosphate (PIP2) depletion9. Although there is a wealth of TRP channel structural information representing multicellular organisms, such information is missing from microbes, limiting our understanding of the structural and functional diversity of this superfamily of ion channels. Therefore, we have decided to structurally and functionally characterize this unique representative.

In this study, we present cryo-electron microscopy (cryo-EM) structures of crTRP1. The crTRP1 architecture is unique; it exhibits overall C2 symmetry and its ankyrin repeat domain (ARD) appears to bend towards and interact with the lipid bilayer. In agreement with a previous study, we found that crTRP1 requires both heat and the lipid PIP2 for its activation.

## Results

### Structural and functional characterization

We heterologously expressed the full-length crTRP1 in HEK 293S cells and purified it in the detergent glycol-diosgenin (GDN) or lauryl maltose neopentyl glycol (LMNG) (Methods). Purified crTRP1 was reconstituted in planar lipid bilayers and its function was tested in various lipids and at different temperatures (Fig. 1). We observed no channel openings when crTRP1 was incorporated into the bilayers in the absence of phosphoinositides. Addition of PIP2 readily evoked channel openings. Similar openings were also observed in the presence of phosphatidylinositol-4-phosphate PI(4)P (Fig. 1a), suggesting that the channel activity is regulated by phosphoinositides. Like other TRP channels, crTRP1 demonstrated outwardly rectifying currents, where rectification is a function of both differences in single-channel conductance and open probability (Po). Consistent with previous cellular recordings9, crTRP1 activation was strongly temperature dependent (Fig. 1c–f). Fitting of the Po temperature dependence (Methods, Fig. 1f) yielded a high temperature coefficient, Q10 = 25 ± 1 (n = 15), which closely resembles the Q10 for the temperature sensitive mammalian TRP channels TRPM814 and TRPV115,16. We also examined the effect of TRP1 inhibitors and found that both gadolinium and N-(4-tertiarybutylphenyl)-4-(3-cholorphyridin-2-yl)tetrahydropyrazine-1(2 H)-carbox-amide (BCTC) strongly suppressed crTRP1-mediated currents (Fig. 1g, h), as was found previously9.

To characterize crTRP1 structurally, the protein was subjected to single-particle cryo-EM. The final reconstruction of crTRP1 in GDN exhibited an overall resolution of 3.53 Å, with higher resolution for the molecule’s core (Supplementary Table 1, Supplementary Fig. 1). In an attempt to better mimic a native membrane environment, we also generated a crTRP1 reconstruction in nanodisc (Supplementary Table 1, Supplementary Fig. 2). Although the crTRP1 reconstruction in nanodisc exhibited slightly higher resolution (3.45 Å) and a somewhat better resolved pore-loop (P-loop) region (Supplementary Fig. 2 g, h), the resulting structure was nearly identical to the structure in GDN (Supplementary Fig. 3). The high quality of our cryo-EM maps (Supplementary Fig. 4) allowed de novo building of 901 residue-long crTRP1 tetramer subunits. We could not resolve or build 16 N-terminal and 27 C-terminal residues, 43 residues in the linker domain and 28 residues in the pore domain, presumably because of higher flexibility in these regions.

### crTRP1 architecture

Unlike structures of the majority of mammalian TRP channels15,17,18,19,20,21,22,23,24,25, the rose-shaped structure of the crTRP1 homotetramer has twofold, rather than fourfold rotational symmetry (Fig. 2a–c). The central transmembrane domain of each crTRP1 subunit includes the S1–S4 and pore domains in the canonical domain-swapped arrangement, followed by an amphipathic TRP helix that runs parallel to the membrane (Fig. 2d–f). The periphery of the transmembrane domain includes hydrophobic pre-S1 and post-TRP elbows that both reenter the membrane from its intracellular side and reach toward the middle of the bilayer. Similar elbow domains have been observed in NOMPC23, TRPC3 (refs. 26,27), TRPC4 (ref. 25), TRPC6 (ref. 26), TRPM2 (refs. 19,24), TRPM4 (refs. 20), TRPM7 (ref. 25), and TRPM8 (refs. 21,28).

The large intracellular domain of crTRP1 adopts a unique fold when compared to other TRP channels (Fig. 3a). The distal N terminus (residues 17–50) interacts extensively with the intracellular domain of the neighboring subunit, suggesting its role in stabilizing the channel tetrameric assembly. Following the N-terminal domain is the ARD that is comprised of four ankyrin repeats whose fingers, surprisingly, extend towards and dip into the plasma membrane, a feature unique to crTRP1 that has not been observed in any member of the TRP channel family. This feature defines the distinct crTRP1 architecture and is especially striking when compared to the architecture of TRPC channels, which have otherwise similar domain compositions (Fig. 3b). Similar interactions with the membrane were proposed for the ankyrin-G family proteins29, which regulate the function of various ion channels and transporters30. A linker domain comprised of nine alpha helices connects the ARD with the TM domain, similar to the TRPC channels25,26. Following the post-TRP elbow is a rib helix, a 33 residue-long α-helical segment that runs parallel to TRP helix, and then a 12 residue-long α-helix that, along with similar helices of other subunits, forms a coiled coil, perpendicular to the membrane and in line with the ion conduction pathway. Similar structural elements were observed in TRPC3 (refs. 26,27), TRPC4 (ref. 25), TRPC6 (ref. 26), TRPM2 (refs. 19,24), TRPM4 (ref. 20), TRPM7 (ref. 25), and TRPM8 (ref. 21).

Because of tight packing of the coiled coil, there is no straight continuous pathway for permeant ions through crTRP1 (Fig. 4). Instead, the central transmembrane pore opens into a wide intracellular cavity that connects to the cytoplasm via two sets of portals, four upper portals formed by the N-terminal domain and ARD of one subunit and the linker domain of the neighboring subunit, and four lower portals, each between two neighboring rib helices and a linker domain. The central pore includes a large central cavity, which has four pore portals that run perpendicular to the pore axis towards the membrane. The pore portals are unlikely to conduct ions, but similar to voltage-gated sodium channels31, may provide access to the pore for small hydrophobic molecules or lipids.

### Lipid-like densities

We identified twelve (three per subunit) well-resolved, non-protein densities in the crTRP1 cryo-EM map that are buried in the inter-subunit intramembrane interfaces (Fig. 5). Because of the twofold symmetry of crTRP1, these putative lipid densities and corresponding binding sites are slightly different in subunits A and C, when compared to B and D (Supplementary Fig. 4c, d). On the basis of the shapes of the putative lipid densities and the proximity of their apparent head domains to positively charged residues, we have modeled the site 1 and 2 densities as PIP2. The location of site 1 is analogous to the vanilloid binding site in TRPV1 (ref. 32). Site 1 is formed by the C-terminal portion of S4, the N-terminal portion of S5, the S2-S3 linker, and the S5 and S6 helices from the neighboring subunit and contains a positively charged region that can accommodate the negatively charged PIP2 head group.

Site 2, located similarly to the lipid binding sites found or proposed to exist in TRPC3 (ref. 26), TRPC4 (ref. 25), NOMC23 and TRPM8 (ref. 21), is strategically placed and could allosterically couple the pore region, the S4–S5 linker, and the N-terminal portion of S1 and the pre-S1 elbow. Like PIP2 binding to TRPM8 (ref. 21), the negatively charged phosphate groups of PIP2 at site 2 are in proximity to the positively charged R366 from the linker domain, K442 from the pre-S1 elbow, and R759 and K762 from the TRP helix. Homologous to R759, a highly conserved lysine in other TRP channels has been shown to be critical for the PIP2 binding and channel activity33. Supporting the role of site 2 in modulating crTRP1 function, the R759K substitution resulted in slower activation kinetics and a rightward shifted G–V curve9. Furthermore, removal of site 2 by deleting the entire pre-S1 elbow resulted in a greatly reduced Po and loss of activation by PIP2 (Supplementary Fig. 5).

Unique to crTRP1, site 3 is sandwiched between the pre-S1 elbow and the ARD fingers of the neighboring subunit. The head of the site 3 putative lipid, which we modeled as phosphatidylcholine (PC), is surrounded by seven tyrosines, two from the pre-S1 elbow and five from the ARD fingers. The acyl tails of PC fit snugly into a large hydrophobic cavity under the long arcing helix 2 of the pre-S1 elbow. As the pre-S1 elbow deletion eliminates site 3, the altered function of the deletion mutant (Supplementary Fig. 5b–d) suggests that a lipid at site 3 might play both structural and functional roles. We also found a non-protein density in the ion conduction pathway at the level of Y747, in the intracellular mouth of the channel, into which a cholesterol molecule can be roughly fit in different orientations (Supplementary Fig. 4e). Like the other non-protein densities, however, its identity is not unambiguous.

### Ion channel pore

Similar to other tetrameric ion channels, the pore of crTRP1 is lined by the S6 helices and the extended portions of the P-loops. For crTRP1 in GDN, the density for the P-loops was completely invisible, presumably due to their higher flexibility, while for crTRP1 in nanodisc, the purported helical portions of the P-loops were poorly resolved and modeled as poly-alanine helices (Supplementary Fig. 2g, h). The selectivity filter and the region between the pore helix and the S6 helix were not built in the structure of TRPM8 due to a lack of interpretable cryo-EM density, and the region connecting S5 and S6 of PKD1 also could not be built in the structure of the PKD1/PKD2 complex28,34. In the case of crTRP1, it is possible that in a lipid bilayer the P-loops are more flexible than those of other TRP channels, however, it is also possible that the disordered P-loops are the product of our experimental methods and are not flexible during, for example, planar bilayer recordings or in a cell membrane. Nevertheless, the P-loops must have an important functional role in crTRP1 as their deletion resulted in substantially impaired gating and reduced single-channel conductance (Supplementary Fig. 5a, c, d). Preceding the helical portions of the crTRP1 re-entrant pore loops, the extracellular turret-forming S5-P-loops contain a disulfide bridge (Supplementary Fig. 6). An analogous disulfide bridge is present in the S5-P-loops of TRPC4, while in the TRPM4 turret, it is incorporated in the P-S6-loop instead. Substitution of the bridge-forming cysteines in TRPC4 results in altered channel function25. Similarly, we show that crosslinking of the extracellular turret cysteines could be important for crTRP1 function; the presence of 100 μM dithiothreitol (DTT) drastically reduces the crTRP1 Po (Supplementary Fig. 7a, b). The formation of such a disulfide bond could be important for the behavioral responses of C. reinhardtii. Indeed, it has been shown that thermotaxis in C. reinhardtii is controlled by redox conditions35.

Of all domains, the ion channel pore reflects the twofold symmetry of crTRP1 most distinctly. Apart from the pore-forming and coiled coil helices, the overall crTRP1 symmetry is close to fourfold (Fig. 6a–c). While deviation from the fourfold symmetry at the coiled coil region is accommodated by a simple swing of the coiled coil helices in subunits A/C relative to subunits B/D, the pore-forming S6 helices in B/D undergo one helical turn (~100°) rotation with respect to the S6 helices in A/C, exposing a different set of residues to the pore. Superposition of subunits A and C onto ~90° rotated B and D subunits show that the C termini of TRP helices in the two subunit pairs overlap (Supplementary Fig. 8). The N-terminal ends of the TRP helices from subunits B and D move up (toward the extracellular side of the protein) and rotate in the plane of the membrane, when compared to subunits A and C. Superposing subunits A and B based on their TRP helices reveals that the linker, pre-S1 and S1–S4 domains do not move much in subunit A relative to subunit B, while S5 and S6 move away from the S1–S4 helices (Supplementary Fig. 8d). Also, the S4–S5 linker moves closer to the TRP helix in subunit B relative to subunit A. Different relative positioning of domains in subunit B is accompanied by rearrangement of the side chains of Q632 and R761 but the overall interaction between the TRP helix and the domains surrounding it does not change very much between subunits. As the TRP helices maintain the same overall conformation in A/C and B/D subunits, the S6 rotation also results in subunit-specific conformations of the S6-TRP helix hinge (Fig. 6d–e, Supplementary Fig. 8b–d). Similar rotation in only two of four pore-forming subunits was observed in the twofold symmetrical structure of TRPV2RTx-ND36. In TRPV2, however, only the C-terminal portions of S6 underwent ~100° rotation, yielding an α-to-π transition in only two diagonally opposed subunits. In contrast, the S6 helices in all four crTRP1 subunits are entirely α-helical and rotate in their entirety.

The twofold symmetrical arrangement of the pore-lining S6 helices results in different contributions to the S6 bundle crossing gate; the B/D subunits appear to adopt a more closed conformation while the A/C subunits are more open. Indeed, L743 in the B/D S6 helices form the narrowest (6.1 Å) crTRP1 pore constriction (Fig. 6e), which is intermediate in diameter when compared to the constrictions formed by I679 in the TRPV1 pore in the apo (5.3 Å) and capsaicin-bound (7.6 Å) states32. In contrast, the narrowest crTRP1 pore constriction contributed by subunits A/C (8.2 Å) is formed by I740 (Fig. 6d) and is intermediate in diameter when compared to the TRPV1 pore constrictions in the capsaicin- and RTX/DkTx-bound (9.3 Å) states32. While the minimal radius of the twofold symmetrical crTRP1 pore (Fig. 6f) is large enough for ion permeation, it may represent an intermediate gating state, similar to the state of the twofold symmetrical TRPV32-APB structure or the TRPV2RTx-ND structure36,37. TRPV3, and likely TRPV2, can adopt twofold symmetric structures while transitioning between states that exhibit fourfold symmetry. That twofold symmetrical structures have been determined for distantly related channels indicates that four- to twofold symmetry transitions might be a conserved component of the gating mechanisms of TRP channels and could be more prevalent than currently known. Regardless of its symmetry, the crTRP1 ion conduction pathway is occluded in both the GDN and nanodisc structures, as evidenced by a strong density in the middle of the ion channel pore (Fig. 6d, e). The hydrophobic environment at this narrow, gate-forming region of the pore suggests that the density may belong to a lipid. Given its flat shape, this density might represent differently oriented molecules of cholesterol that plug crTRP1 pore (Supplementary Fig. 4e, f).

### crTRP1 structure and evolution

The distinct pore structure and overall architecture of crTRP1 emphasizes its unique evolutionary niche. crTRP1 has evolved from common ancestors of plants and animals, the most recent of which existed ~1.6 billion years ago38,39. Combined with functional and sequence analysis9, the structure of crTRP1 expands our understanding of TRP channel diversity and evolution. Compared to its mammalian counterparts19,20,25,26,27, crTRP1 includes domains that remain structurally conserved throughout evolution and include the canonical six-helix transmembrane domain, linker domain, TRP helix, rib helix, and coiled coil domains, exhibiting the close structural homology to the TRPC channels (Fig. 3). The TRP helix is homologous to those of mammalian TRP channels and contains conserved residues in the TRP-box signature sequence “WKFQR”, including two positively charged residues at positions 2 and 5 that have been proposed to be important for PIP2 binding (Supplementary Fig. 8a). The highly conserved tryptophan at position 1 is replaced by phenylalanine 758, as was noted previously9.

Other domains of crTRP1, however, show diverged structural features that are likely to be important for crTRP1 function (Fig. 7). Compared to other TRP channels, the crTRP1 pre-S1 elbow domain evolved to a larger than average size and harbors a unique lipid binding site (site 3), which is located strategically to link the ARD with the pre-S1 and post-TRP elbow domains (Fig. 5). The hydrophobic surfaces of the elbow domains (Fig. 7b) facilitate their submersion into the membrane and suggest their possible role in sensing the composition of the membrane and perhaps the environmental temperature32. Linked to the elbow domains by the site 3 lipid-like density, the crTRP1 ARDs adopt a similar overall architecture to the ARDs from the TRPC sub-family, but with uniquely organized fingers (Supplementary Fig. 9). Indeed, the tips of the crTRP1 ARD fingers contain triplets of hydrophobic residues, capable of dipping into the lipid bilayer (Fig. 7c). At the bases of the fingers, the triplets are surrounded by polar and charged residues, capable of interacting with the polar heads of membrane lipids. We speculate that the ARDs function as a part of the crTRP1 scaffold, relative to which the elbow domains move in response to changes in their environment (Fig. 7d). As the TRP helix directly links the post-TRP elbow to the channel gate, the distinct arrangement of the crTRP1 domains might reflect a unique molecular mechanism utilized by C. reinhardtii to sense temperature and chemical composition of the environment.

## Methods

### Cryo-EM sample preparation and data collection

We purchased C-flat (Protochips) CF-1.2/1.3-2Au mesh holey carbon grids and prepared Au/Au grids as described in the literature41. Briefly, ~50 nm of gold was deposited onto the grid surface using an Edwards Auto 306 evaporator. The grids were then flipped and placed into a Gatan Solarus (model 950) Advanced Plasma Cleaning System for an Ar/O2 treatment (4 min, 50 watts, 35.0 sccm Ar, 11.5 sccm O2) to remove carbon. The grids were plasma treated for the second time (H2/O2, 20 s, 10 watts, 6.4 sccm H2, 27.5 sccm O2) prior to 3 µl sample application. A Vitrobot Mark V1 was used to plunge-freeze the crTRP1-nanodiscs grids at 22 °C and 100% humidity using a 2 s blot time, the blot force set to 3, a 20 s wait time. The crTRP1-GDN grids were prepared in the same way, except that Vitrobot was set to 4 °C.

The crTRP1-GDN data were collected on a Titan Krios TEM (FEI) operating at 300 kV equipped with a Gatan K2 Summit direct electron detection (DED) camera using a post-column GIF Quantum energy filter. 2342 micrographs were collected using Leginon42 with a pixel size of 1.06 Å in a counting mode across the defocus range of −1.0 to −3.0 µm. The total dose, ~61 e Å−2, was attained by using a dose rate of ~8.0 e pixel−1 s−1 across 40 frames for 8 s total exposure time.

The crTRP1-nanodisc data were collected on a Tecnai F30 Polara operating at 300 kV equipped with a Gatan K3 DED camera. 6272 micrographs were collected using Leginon in a counting mode with the pixel size of 0.95 Å across the defocus range of −1.0 to −3.0 µm. The total dose, ~71 e Å−2, was attained either by using the dose rate of ~16 e− pixel−1 s−1 across 40 frames for 4 s total exposure time or by using the dose rate of ~8 e− pixel−1 s−1 for 8 s total exposure time.

### Image processing

All data was processed using Relion 3.0 (ref. 43). The crTRP1-nanodiscs dataset was processed as follows. Initially, ~2000 particles were manually picked to generate 2D classes that were subsequently used to automatically pick 1,714,216 particles. The particle images were subjected to 2D classification and then 3D classification using an ab-initio model as a reference. Two classes, comprising ~550,000 particles, were combined and refined with C1 and C2 symmetry, at which point it was determined that the channel exhibited the overall C2 symmetry. Nevertheless, because of structural ambiguity in the upper-pore region, the C1 reconstruction was used as a reference for the next round of 3D classification, which was also done without imposing symmetry. Five classes were chosen, combined and refined with C2 symmetry, and post-processed to generate the final ~3.5 Å reconstruction.

The crTRP1-GDN dataset was processed in a similar manner to that described above and the reported resolutions were estimated using the Fourier shell correlation (FSC) = 0.143 criterion. The local resolutions were estimated with unfiltered half maps using ResMap44 and EM density visualization was done in UCSF Chimera45.

### Model building

The data was of sufficient quality to build the structures de novo. The models were tested for overfitting (Supplementary Figs. 1 and 2) by shifting their coordinates by 0.5 Å (using shake) in PHENIX46, refining each shaken map against a corresponding unfiltered half map, and generating densities from the resulting models in Chimera45. FSC was calculated between the densities generated in Chimera and both unfiltered half maps and the sum maps, using EMAN247. The local resolutions in our reconstructions were estimated using ResMap44. Structures were visualized and figures were prepared in Pymol46.

### Planar lipid bilayer measurements

Planar lipid bilayers measurements were performed as described previously48. Briefly, planar lipid bilayers were formed from a solution of synthetic 1-palmitoyl-2-oleoyl-sn-glycero-3-phospho-(1′-rac-glycerol) (POPG), 1-palmitoyl-2-oleoyl-glycero-3-phosphocoline (POPC) and 1-palmitoyl-2-oleoyl-glycero-3-phosphoethanolamine (POPE; Avanti Polar Lipids) at a 3:1:1 ratio in n-decane (Sigma-Aldrich). The solution was used to paint a bilayer in an aperture of 150 µm diameter in a Delrin cup (Warner Instruments) between symmetric aqueous bathing solutions of 150 mM KCl, 0.02 mM MgCl2, 1 μM CaCl2, and 20 mM HEPES (pH 7.2). Unless specified otherwise, all experiments were performed in the presence of 2.5 μM 1-(1,2R-dioctanoylphosphatidyl)inositol-4,5-bisphosphate, trisodium salt (DiC8-PIP2, Cayman Chemical) added to both compartments. To assess the effect of a reducing agent on crTRP1-mediated currents, after obtaining heat-induced crTRP1 activity, 100 μM DTT was added to both compartments of the bilayer, and the channel activity was then continuously recorded for up to 5–6 h. All reagents (Sigma-Aldrich) were ultrapure (>99%). Bilayer capacitances were in the range of 50–75 pF.

After the bilayers had formed, the micellar solution of crTRP1 protein (0.02 μg/ml) was added by painting. Unitary currents were recorded using the Axopatch 200B patch-clamp amplifier (Molecular Devices). The trans solution (command voltage side) was connected to the CV 201A head-stage input, while the cis solution was held at a virtual ground via a pair of matched Ag-AgCl electrodes. Currents through the voltage-clamped bilayers (background conductance, <1 pS) were filtered at the amplifier output (low pass, −3 dB at 10 kHz, 8-pole Bessel response). Data were filtered at 100 Hz through an 8-pole Bessel filter (950 TAF; Frequency Devices) and digitized at 1 kHz with an analog-to-digital converter Digidata 1322A controlled by pClamp10.3 software (Molecular Devices). Single-channel conductance events, all-points histograms, open probability (Po), and other parameters were identified and analyzed with Clampfit10.3 software (Molecular Devices). The experiments were performed in the temperature range from 22 to 30 °C. For the temperature-dependence measurements, the bilayer recording chamber was fitted onto a conductive stage containing a pyroelectric heater/cooler that was controlled by a temperature controller (CL-100; Warner Instruments). Deionized water was circulated through the stage and pumped into the system to remove the generated heat. The temperature of the bath was constantly monitored using a thermoelectric device in the cis chamber (the ground side) and was reliably controlled within ±0.5 °C. The temperature coefficients (Q10) for Po were calculated using Eq. 1:

$$Q_{10} = \left( {\frac{{X_2}}{{X_1}}} \right)^{\frac{{10}}{{T_2 - T_1}}}$$
(1)

where X1 and X2 are Po values obtained at T1 and T2 temperatures measured in Kelvins. Statistical analysis was performed using Origin 9.0 (Microcal Software Inc.). Statistical significance was calculated using One-way ANOVA followed by Fisher’s least significant difference test. All data are presented as mean ± SEM.

### Reporting summary

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

## Data availability

Cryo-EM density maps have been deposited to the Electron Microscopy Data Bank (EMDB) under accession numbers EMD-20499 for crTRP1-nanodiscs and EMD-20498 for crTRP1-GDN. Model coordinates have been deposited to the Protein Data Bank (PDB) under accession numbers 6PW5 for crTRP1-nanodiscs and 6PW4 for crTRP1-GDN. The source data underlying Fig. 1b, d, f, h and Supplementary Figs. 5c, d and 7b are provided as a Source Data file. All other data are available from the corresponding authors upon request.

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## Acknowledgements

We thank R. Grassucci for assistance with microscope operation, U. Baxa and T. Edwards for help with data collection, and H. Kao for computational support. L.L.M. is supported by the NIH (F31 CA232391-01). A.I.S. is supported by the NIH (R01 CA206573, R01 NS083660, R01 NS107253), NSF (1818213), and the Irma T. Hirschl Career Scientist Award. Data were collected at the Frederick National Laboratory for Cancer Research National Cryo-EM Facility (NIH) and at the Simons Electron Microscopy Center and National Resource for Automated Molecular Microscopy (New York Structural Biology Center) supported by grants from the Simons Foundation (349247), NYSTAR, and the NIH (GM103310).

## Author information

L.L.M., A.K.S., E.Z., and A.I.S. designed the project and analyzed data. L.L.M., A.K.S., T.-Y.L., and R.G.C. made constructs and prepared protein samples. L.L.M. and A.K.S. carried out cryo-EM data collection and processing. L.L.M., A.K.S., and A.I.S. built molecular models. L.D. carried out bilayer experiments. L.L.M., A.K.S., L.D., T.-Y.L., E.Z., and A.I.S. wrote the manuscript.

Correspondence to Eleonora Zakharian or Alexander I. Sobolevsky.

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### Competing interests

The authors declare no competing interests.

Peer review information Nature Communications thanks Sebastian Brauchi and Tingliang Wang for their contribution to the peer review of this work.

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McGoldrick, L.L., Singh, A.K., Demirkhanyan, L. et al. Structure of the thermo-sensitive TRP channel TRP1 from the alga Chlamydomonas reinhardtii. Nat Commun 10, 4180 (2019). https://doi.org/10.1038/s41467-019-12121-9