TRPV1 channels in sensory neurons are integrators of painful stimuli and heat, yet how they integrate diverse stimuli and sense temperature remains elusive. Here, we show that external sodium ions stabilize the TRPV1 channel in a closed state, such that removing the external ion leads to channel activation. In studying the underlying mechanism, we find that the temperature sensors in TRPV1 activate in two steps to favor opening, and that the binding of sodium to an extracellular site exerts allosteric control over temperature-sensor activation and opening of the pore. The binding of a tarantula toxin to the external pore also exerts control over temperature-sensor activation, whereas binding of vanilloids influences temperature-sensitivity by largely affecting the open/closed equilibrium. Our results reveal a fundamental role of the external pore in the allosteric control of TRPV1 channel gating and provide essential constraints for understanding how these channels can be tuned by diverse stimuli.https://doi.org/10.7554/eLife.13356.001
Humans and other mammals sense elevated heat and other painful stimuli via a sensory ion channel protein called TRPV1. Ion channels create pores in the outer membrane of cells and act as gates that open and close to regulate the flow of ions into and out of cells. This flow of ions generates electrical signals that sensory neurons use to communicate information about the environment to the brain. The TRPV1 channel is opened by heat, but also by venom toxins, acid and the active ingredient in hot chilli peppers.
The fluid that surrounds animal cells often contains high levels of sodium ions, and these ions flow through TRPV1 channels when they are open. Also, when sodium ions are removed from the fluid surrounding a cell, TRPV1 channels will spontaneously open. It is not known why this happens, but it suggests that sodium ions help to regulate the activity of the TRPV1 channel, and despite having been extensively studied, it remains unclear how this channel senses temperature and responds to other harmful stimuli.
Jara-Oseguera et al. have now investigated the role of sodium ions in activating TRPV1 in cells grown in the laboratory. The experiments involved a technique that records the movement of ions through TRPV1 channels in the cell surface membrane while exposing the cell to various stimuli that open or close the channels. The results showed that TRPV1 contains an important site on its outer surface that binds sodium ions and fine-tunes the channel’s properties. This enables the channel to be activated by potentially damaging temperatures. Further analysis revealed that TRPV1 undergoes at least two distinct physical changes in response to heat and that the binding of sodium ions to the channel’s outer structure regulates one of these changes.
Jara-Oseguera et al. went on to discover that the binding of a tarantula toxin to the outer surface of TRPV1 renders the channel insensitive to changes in temperature. These findings suggest that structural changes to the external part of this channel protein are closely associated with its ability to sense temperature, possibly because this region of the protein is directly responsible for detecting changes in temperature.
These findings shed light on how this channel detects and responds to dangerously high temperatures, as well to other harmful stimuli. An aim for future studies is to pinpoint the specific regions of the protein that form the sodium-binding sites and to test the hypothesis that temperature sensors are located on the outer surface of the protein.https://doi.org/10.7554/eLife.13356.002
Transient receptor potential (TRP) channels belong to a large and diverse superfamily of tetrameric cation channels that contain six transmembrane helices per subunit (Liao et al., 2013; Hellmich and Gaudet, 2014), similar to voltage-activated ion channels (Long et al., 2007), ryanodine receptors (Yan et al., 2015) and IP3 receptors (Fan et al., 2015) (Figure 1A). Several TRP channels are exquisitely temperature-dependent, enabling them to serve as biological thermosensors throughout the animal kingdom (Vay et al., 2012). The vanilloid-sensitive TRPV1 channel is a weakly voltage-dependent and cation-selective channel that is expressed in nociceptive sensory neurons, where it acts as a sensor for noxious stimuli (Caterina and Julius, 2001) including heat, extracellular acidic pH, vanilloid compounds (e.g capsaicin), and venom toxins (e.g. double-knot toxin or DkTx) (see [Hilton et al., 2015] for review). The sensitivity of TRPV1 to diverse modulators is fascinating because many stimuli are capable of influencing the responses of TRPV1 to other signals. For example, protons can sensitize the channel to activation by heat (Jordt et al., 2000) and capsaicin (Jordt et al., 2000; Ryu et al., 2003), and both capsaicin (Voets et al., 2004; Matta and Ahern, 2007; Gregorio-Teruel et al., 2014) and protons (Lee and Zheng, 2015) can sensitize the channel to activation by voltage. Conceptually, these observations can be explained by allosteric models wherein distinct stimulus-sensing domains are coupled to each other (Latorre et al., 2007), and to an internal gate within the pore that opens and closes the ion permeation pathway (Salazar et al., 2009; Cao et al., 2013) (Figure 1A).
The regions of TRPV1 targeted by some activating stimuli have been identified, including the vanilloid binding site within internal regions of the S1-S4 domain (Jordt and Julius, 2002; Cao et al., 2013), and both proton- (Jordt et al., 2000) and DkTx-binding sites within the external pore (Bohlen et al., 2010; Cao et al., 2013; Bae et al., 2016) (Figure 1A). However, we currently do not understand the structural basis by which the binding of protons, capsaicin or DkTx promotes opening of the internal pore. Moreover, there is no consensus about the site and mechanism of temperature sensitivity. Mutations throughout TRPV1 alter the temperature sensitivity of the channel (Feng, 2014), and distinct models have been proposed to explain temperature sensitivity in these channels (Voets, 2012). For example, in the conventional allosteric model, a specialized temperature-sensitive transition is coupled to a temperature- and voltage-insensitive opening transition (Brauchi et al., 2004; Matta and Ahern, 2007). In contrast, others have suggested that temperature sensitivity arises from a weakly voltage-sensitive opening transition (Voets et al., 2004). Indeed, one recent study on voltage-activated potassium (Kv) channels suggests that the opening transition in these related channels can be made steeply temperature-dependent when the coupling between the voltage-sensing and pore domains is weakened (Yang et al., 2014). It has also been suggested that TRP channels may not contain localized temperature-sensors, but that their steep temperature-dependence results from changes in solvation of hydrophobic residues throughout the protein (Clapham and Miller, 2011).
Recent landmark near-atomic resolution structures of the TRPV1 channel confirm the presence of an internal gate related to that present in Kv channels (Liu et al., 1997; del Camino and Yellen, 2001). In addition, the external pore and selectivity filter change conformation in the combined presence of DkTx and the vanilloid resiniferatoxin (RTx) (Cao et al., 2013; Liao et al., 2013). Given our limited understanding of the temperature-sensitivity of TRPV1, it is unclear whether these structures provide insight into the mechanisms of heat activation. However, the structural rearrangements within the external pore are intriguing because mutations in this region have been reported to alter activation of the channel by protons (Jordt et al., 2000) and heat (Grandl et al., 2010; Cui et al., 2012; Yang et al., 2014). In addition, external Na+ ions have been reported to inhibit the TRPV1 channel at room temperature (Ohta et al., 2008), raising the possibility that an external cation binding site may regulate these channels. In the present study, we demonstrate the presence of a critical external Na+ ion-binding site that must be occupied for the channel to remain closed at room temperature, and to be available for opening by noxious heat. Our results also show that multiple steeply temperature-dependent transitions are allosterically coupled to an opening transition, and that binding of Na+ or DkTx to the external pore strongly influences the activity of the temperature-sensor and opening of the pore.
To investigate the influence of external Na+ on TRPV1 channels, we obtained whole-cell patch clamp recordings of cells expressing rat TRPV1 using internal and external solutions containing Na+ (130 mM) as the sole charge carrier, and then exchanged the external Na+ solution with one containing N-methyl-D-glucamine (NMDG+; 130 mM) (Figure 1B). At room temperature, this simple manipulation produced a rapid and reversible increase in outward currents at positive voltages (Figure 1B), consistent with previous results (Ohta et al., 2008). Subsequent application of a saturating concentration of capsaicin further increased the outward currents independently of whether external Na+ or NMDG+ was present (Figure 1B). At moderate TRPV1 expression levels, where outward Na+ currents could be accurately measured, the inward currents with external NMDG+ were negligible even in the presence of capsaicin (Figure 1B), indicating that TRPV1 has a relatively low permeability to large cations. Although large outward currents induced by exchanging external ions were observed in all cells in which capsaicin evoked measurable currents, this manipulation also produced a variable and irreversible rundown of the channel that increased with time in Na+-free solutions (Figure 1—figure supplement 1). Exchanging external Na+ with NMDG+ also produced large outward currents in human, mouse and chicken TRPV1 orthologues (Figure 1—figure supplement 2), which together with the previous report on porcine TRPV1 (Ohta et al., 2008), suggest that this phenomenon is a conserved feature of TRPV1 channels. Given the robust effects of exchanging external Na+ with NMDG+, we set out to explore the underlying mechanism.
To investigate the extent to which the large outward currents in external NMDG+ result from a change in driving force when exchanging external solutions, we obtained current-voltage (I-V) relations using rapid voltage ramps (Figure 1C) or voltage steps in cells exhibiting minimal rundown at room temperature (Figure 1—figure supplement 3). I-V relations for fully activated channels (10 µM capsaicin) in the presence of external Na+ or NMDG+ superimpose at positive voltages (Figure 1C and Figure 1—figure supplement 3), suggesting that the unitary conductance of TRPV1 channels is similar under these conditions. In addition, theoretical I-V relations calculated from the Goldman-Hodgkin-Katz equation predict little change in unitary conductance at positive voltages (Figure 1—figure supplement 4), and we confirmed that exchanging external solutions does not affect the single-channel current amplitude (i) at positive voltages in outside-out patches containing a few channels (Figure 2A). From these results, we conclude that exchanging external Na+ with NMDG+ leads to spontaneous opening of the TRPV1 channel at room temperature.
To distinguish whether channel activation results from the removal of Na+ or the addition of NMDG+, we obtained voltage ramps in 130 mM NMDGo in the additional presence of 130 mM Nao (with 260 mM internal Na+) and observed only small outward currents at positive voltages that superimposed with those obtained in the presence 260 mM Nao (Figure 2B). This result indicates that NMDG+ does not activate the channel in the presence of Na+, but rather removal of external Na+ leads to channel activation. Removal of internal Na+ in recordings using inside-out patches produced no channel activation (Figure 2C, left panel), whereas removing external Na+ using outside-out patches led to robust activation (Figure 2C, right panel), demonstrating that the inhibitory influence of Na+ is limited to the external side of the TRPV1 channel. We also measured the concentration-dependence for external Na+ inhibition over a range of voltages (Figure 2D) and found that inhibition was only weakly voltage-dependent, with an extrapolated apparent affinity (K1/2) at 0 mV of 2 mM (Figure 2E). These results suggest that external Na+ stabilizes a closed state of the TRPV1 channel by binding to a site on the extracellular side of the protein. This ion-binding site is not highly selective for Na+, as external K+ can stabilize the closed state almost as effectively as Na+, followed by Rb+, Tris+, Cs+ and Li+ (Figure 2—figure supplement 1).
An external Na+ binding site that stabilizes TRPV1 in a closed state is interesting because titratable acidic residues are commonly found in such sites (Lev et al., 2013) and acid is a physiological stimulus for this channel, with mildly acidic conditions sensitizing the channel to either capsaicin or heat, and strongly acidic conditions causing channel activation (Jordt et al., 2000;Ryu et al., 2003). To explore a possible mechanistic link between the external Na+ site and acid regulation, we changed external pH from 7.4 to 6 and observed a pronounced shift in the concentration-dependence for Na+ inhibition to higher Na+ concentrations (Figure 3A). Moreover, activation of the channel by pH 6 could be completely overcome by raising the Na+ concentration to 300 mM. These results are consistent with the expectation that protonation of acidic residues forming the Na+ binding site would lower the affinity of the metal ion, suggesting that the inhibitory Na+ binding site is intimately involved in the regulation of the TRPV1 channel by acid. However, acidic solutions further stimulated channel activation in the absence of external Na+ (Figure 3A), indicating that protons also activate TRPV1 channels through a Na+-independent mechanism. These findings support the idea that proton-mediated channel activation and proton-dependent potentiation of responses to other stimuli have distinct mechanisms (Jordt et al., 2000; Ryu et al., 2007).
We next set out to determine whether other stimuli acting on the extracellular pore activate TRPV1 through a mechanism associated with the binding of external Na+. The double-knot tarantula toxin (DkTx) is an interesting candidate as it activates the TRPV1 channel with high avidity by binding to the periphery of outer pore of the channel (Figure 3—figure supplement 1A) (Bohlen et al., 2010; Cao et al., 2013; Bae et al., 2016). We recently solved the solution structure of DkTx and performed a detailed analysis of its interactions with the TRPV1 channel, which suggested that the toxin activates TRPV1 by disrupting a cluster of hydrophobic residues at the extracellular half of the S5 and S6 segments (Bae et al., 2016). Interestingly, removal of external Na+ before application of the toxin activates TRPV1 to a similar extent when compared with a saturating concentration of DkTx (Figure 3B and C), and removal of external Na+ did not produce further activation of DkTx-bound channels. In contrast, application of a saturating concentration of capsaicin produced further activation (Figure 3C). The lack of additivity for the activation of TRPV1 by DkTx and the removal of external Na+ contrasts with our results with acidic extracellular pH in the absence of external Na+ (Figure 3A), and suggests that DkTx and external Na+ modulate the TRPV1 through convergent mechanisms.
The unambiguous identification of the Na+-binding site would require a high resolution structure of TRPV1. However, a glutamate at position 600 near the top of S5 (Figure 3—figure supplement 1A) has been previously associated with the inhibition of TRPV1 by external Na+ (Ohta et al., 2008), and has also been shown to be involved in the proton-dependent potentiation of TRPV1 responses to heat and capsaicin (Jordt et al., 2000). To confirm a key role of this residue in modulation of TRPV1 by external Na+, we investigated the effect of removing external Na+ on E600Q mutant channels, and found that the removal of external Na+ no longer produced constitutive activation even though the mutant remained responsive to capsaicin (Figure 3D). Consistent with DkTx and external Na+ having convergent mechanisms for modulating TRPV1, E600Q channels were not responsive to a concentration of DkTx that is saturating in WT channels (Figure 3D). These results demonstrate an important role for E600 in mediating channel inhibition by external Na+ and activation by DkTx, and suggest that this residue may be a part of the Na+ binding site.
Another interesting region within the outer pore of TRPV1 is the pore turret (Δ604–626, Figure 3—figure supplement 1B), a stretch of 22 residues that was removed in the construct of TRPV1 recently used for structure determination (Liao et al., 2013) and that is located near to E600 and to the binding site for DkTx (Figure 3—figure supplement 1A). We therefore explored whether the deletion of the pore turret retains modulation by external Na+. Initially, we found that the removal of external Na+ produced robust channel activation at depolarized potentials in channels lacking the pore turret (Figure 3E), and that the addition of 10 µM capsaicin in the presence of external Na+ further activated the channels, similar to WT TRPV1. Interestingly, the removal of the pore turret increased the apparent affinity of the channel for Na+ (Figure 3F), indicating that the pore turret does not form the Na+ binding site, but influences the cation-binding site through an allosteric mechanism. However, we also made the surprising discovery that the removal of external Na+ in the presence of 10 µM capsaicin resulted in enhanced channel activation at positive voltages relative to 10 µM capsaicin in the presence of 130 mM external Na+ (Figure 3E), in stark contrast with WT channels where I-V relations under these two conditions superimpose at depolarized potentials due to maximal channel activation (Figure 1C and Figure 3C). Increasing the concentration of capsaicin from 10 to 40 µM did not further activate Δ604–626 TRPV1 channels in the presence of external Na+ (Figure 3E), indicating that 10 µM is a saturating concentration and that capsaicin is a partial agonist for this construct. This reveals that the pore turret is mechanistically associated with the modulation of the channel not only by stimuli acting on the extracellular pore (e.g. external Na+), but also by capsaicin that binds near the intracellular part of the protein (Figure 1A).
Finally, we were interested in determining whether external Mg2+ ions activate the TRPV1 channel directly, as was suggested in two previous studies that analyzed the effect of substituting external Na+ with Mg2+ without considering the inhibitory effects of external Na+ (Cao et al., 2014; Yang et al., 2014). We tested the ability of 130 mM external MgCl2 to activate the TRPV1 channel in the presence of 130 mM external NaCl (and 260 mM intracellular NaCl), as we did previously in Figure 2B to determine whether NMDG+ was an activator of TRPV1. Contrary to what we observed for NMDG+, Mg2+ ions produced robust activation of the TRPV1 channel in the presence of 130 mM external Na+ (Figure 3—figure supplement 1C), indicating that Mg2+ can activate the TRPV1 channel directly.
Collectively, our results thus far highlight a central role of the outer pore in the allosteric control of TRPV1 channel gating. Furthermore, they suggest that the binding of DkTx, protons and external Na+ to the extracellular pore of TRPV1 modulate channel function through at least partially overlapping mechanisms. We next set out to determine whether the external Na+ site has an influence in the mechanism of temperature-sensitivity of the TRPV1 channel, as protons have been shown to potentiate responses of the channel to heat (Jordt et al., 2000), and the outer pore has been associated with temperature-sensitivity (Myers et al., 2008; Grandl et al., 2010; Cui et al., 2012; Cao et al., 2014; Yang et al., 2014).
TRPV1 is widely agreed to be activated by noxious heat above 35°C in the absence of other stimuli (Liu et al., 2003; Yao et al., 2010), but whether the channel responds to lower temperatures has not been carefully examined because the open probability (Po) in this temperature range is very low (Oseguera et al., 2007). If TRPV1 remains sensitive to changes in temperature below 35°C, it is possible that the spontaneous activation that we observed upon removing external Na+ at room temperature might be caused by an alteration in the temperature-dependence for channel activation. We therefore began by investigating TRPV1 channel activity over a broad temperature range in the presence of external Na+ using cells with widely varying expression levels of the channel. We measured macroscopic current-temperature (I-T) relations between ~8°C and 45°C using slow temperature ramps and observed steep temperature-dependent activation over the entire range of temperatures explored (Figure 4A and B). Although these I-T relations largely reflect temperature-dependent changes in Po, the rate of ion conduction through open channels is also weakly temperature-dependent and thus will contribute to the slope of I-T relations. To directly evaluate temperature-dependent changes in Po, we estimated the temperature-dependence of ion conduction (Figure 4—figure supplement 1B–E) and then calculated Po-T relations from the macroscopic I-T relations (Figure 4C and Figure 4—figure supplement 1F, see Materials and methods). To qualitatively compare the slopes of Po-T relations between cells and conditions, we fit a single exponential function (Equation 1, see Materials and methods) to the data over defined temperature ranges to obtain apparent enthalpy (ΔHapp) values (see Figure 4—figure supplement 2C–E). At temperatures > 35°C, we observed steep temperature-dependence to Po at positive membrane voltages (Figure 4C and D), which became even steeper at negative membrane voltages (Figure 4D, Figure 4—figure supplement 2B and E), consistent with previous studies (Voets et al., 2004; Yao et al., 2010). At temperatures between 8 and 25°C, a range in which the temperature-sensitivity of TRPV1 has not been previously investigated, we also observed steep temperature-dependence to Po (Figure 4C and D, Figure 4—figure supplement 2C–E). However, the entire Po-T relationship could not be described by a single temperature-dependent transition due to the presence of an apparent plateau near 22°C, raising the possibility that multiple temperature-dependent transitions are involved in the gating mechanism of TRPV1.
Having found that TRPV1 remains temperature-sensitive at room temperature and below in the presence of external Na+, we measured macroscopic current-temperature (I-T) relations in the absence of external Na+ (Figure 5A and B) and constructed Po-T relations (Figure 5C). Remarkably, both I-T and Po-T relations displayed greatly diminished slopes and readily detectable channel activity at the lowest experimentally accessible temperatures (Figure 5A–C). In addition, removal of external Na+ produced marked temperature-dependent inactivation of TRPV1 channels between 25 and 38°C (Figure 5B, see yellow arrow), a process that typically occurs after repetitive cycles of heating and cooling in the presence of extracellular Na+ (Joseph et al., 2013) and at temperatures above ~50°C in single heat-activation experiments (Figure 5B, see purple arrow). Notably, temperature-inactivated channels could not be subsequently activated by heating, but were partially responsive to saturating capsaicin (Figure 5—figure supplement 1A) (Cao et al., 2014). This facilitation of temperature-dependent inactivation in the absence of external Na+ can explain why removing Na+ also leads to progressive rundown of the TRPV1 channel at room temperature (Figure 1—figure supplement 1). We also observed that capsaicin diminishes rundown at room temperature when external Na+ was removed (Figure 5—figure supplement 1B), consistent with a mechanistic link between temperature-dependent inactivation and channel rundown in the absence of external Na+ at room temperature.
We next explored why the TRPV1 channel lacks steep temperature-dependent activation in the absence of external Na+. One possibility is that the mechanism of heat activation remains intact, but that increases in Po upon heating cannot be seen because channels run down after opening during temperature ramps (see Figure 7—figure supplement 5 and Materials and methods for an illustration using an allosteric model for channel gating). If this is the case, increasing the rate at which temperature is changed in the absence of external Na+ should diminish the effects of rundown and reveal the presence of heat activation. To examine this possibility, we measured I-T relations in either the presence (Figure 5D, large grey circles) or absence (Figure 5D, large orange circles) of external Na+ by rapidly jumping between solutions at different temperatures (Figure 5—figure supplement 3), and observed that I-T relations in the absence of external Na+ obtained from temperature-ramps and from jumps agreed up to ~25°C, after which they deviated markedly (Figure 5D, note deviation between orange circles and small yellow circles as highlighted by the blue lines). Additionally, the rate of temperature-dependent inactivation in the absence of external Na+ at T > 45°C became so fast that the speed of our temperature-jumps was not sufficient to visualize the increase in Po before significant inactivation occurred (note the last orange circle in Figure 5D). These results suggest that temperature-dependent activation has been greatly perturbed in the absence of external Na+ at temperatures below 25°C, but that activation at higher temperatures appears largely intact (Figure 5D, compare orange and grey large circles). Taken together, these findings suggest that the Na+ regulatory site is strongly coupled to a temperature-dependent transition that governs TRPV1 activation at low temperature, and confirm the presence of multiple temperature-dependent transitions.
The results obtained from measurements of Po-T relations are depicted schematically in Figure 5E, where dotted horizontal lines represent plateau regions where steep temperature-dependence cannot be readily observed (ΔHApp~0), and arrows represent regions where Po increases steeply with temperature (ΔHApp>> 0). The vertical dotted grey line indicates the lowest temperature that we can achieve experimentally, with the yellow arrow crossing that temperature representing a hypothetical temperature-sensitive transition in the absence of external Na+. We include this transition because the Po-T relation in the absence of Na+ shows some temperature-dependence to Po at T < 10°C (Figure 5C and 6A). To verify the existence of this transition in the absence of external Na+, we tested two manipulations that should shift the temperature range over which that transition operates. Capsazepine has been proposed to shift heat activation of TRPV1 to higher temperatures (Matta and Ahern, 2007), and we therefore tested whether this allosteric inhibitor might produce a rightward shift in the Po-T relation, making the temperature- sensitive transition more readily detectable in the absence of external Na+. Indeed, the addition of capsazepine resulted in clear temperature-dependence of Po at low temperatures in the absence of external Na+ (Figure 6A and C). Next, we tested intermediate external Na+ concentrations to see if temperature-dependent changes in Po could be detected at lower temperatures. We obtained Po-T relations at 10, 30 and 65 mM external Na+, and observed clear temperature-dependence at low temperatures (Figure 6B), with enthalpies close to those measured in the presence of 130 mM external Na+ in the same temperature range (Figure 6C). Taken together, these findings suggest that the TRPV1 channel undergoes the same conformational transitions in response to heat regardless of whether external Na+ is present, and thus that the enthalpy (ΔHo) associated with Na+ binding is not itself responsible for temperature-dependent gating (for a more detailed discussion see Materials and methods). Rather, it seems that external Na+ modifies the midpoint (or entropy, △S) of the temperature-sensitive transition that operates at low temperatures. Additionally, external Na+ appears to stabilize a closed state of the channel independently of its effect on temperature-sensitivity, as the Po values corresponding to the inferred plateau regions (denoted by dotted lines in Figure 6B - insert) decrease as the concentration of external Na+ is increased.
These features of our results can be depicted in a simple allosteric model wherein two temperature-sensitive transitions are allosterically coupled to a temperature-insensitive opening transition, with Na+ regulating both the midpoint (△S) of the temperature-sensitive transition operating at low temperatures and the open/closed equilibrium (Figure 7A, see Materials and methods for an in-depth discussion on the choice of model and the inherent assumptions). In the presence of Na+, the two temperature-sensitive transitions have similar midpoints, such that the plateau between the two is barely noticeable in the Po-T relation (Figure 6B insert, grey arrows). Upon Na+ removal, the midpoint of the first temperature-sensitive transition shifts to lower temperatures, effectively extending the middle plateau where Po is temperature-independent (Figure 6B insert, yellow lines and arrows) and the channel mostly occupies the open/closed equilibrium highlighted with orange squares in Figure 7A. Additionally, external Na+ also negatively impacts the opening transition through allosteric coupling, which results in the intermediate plateau between the two temperature-dependent transitions in Po-T relations having a lower Po in the presence of external Na+. This simple model can qualitatively reproduce our results at intermediate Na+ concentrations (Figure 7B and Figure 6—figure supplement 1). One important feature of the model is that the opening transition is relatively temperature-insensitive, and that the channel can open even when the temperature sensor is in the deactivated state (Figure 7A, C – O transitions with blue squares). Although we would not rule out measurable changes in ΔHo during opening, as shown by an alternate model that also satisfactorily reproduced our experimental results (Figure 7—figure supplement 1A), such a mechanism would require divergent temperature-sensitive transitions depending on whether external Na+ is bound to the channel, which we consider to be more conceptually complex than the allosteric model proposed here (see Materials and methods for a more detailed discussion). Additionally, in the alternate model ii, external Na+ influences the temperature-dependent transition that occurs at lower temperatures in the same way as in Model i (Figure 7—figure supplement 1A). We also cannot rule out the possibility that the temperature sensors have to activate for the channel to open (i.e., occupancy of the open states with blue squares in Figure 7A is negligible), as the gating of TRPV1 channels remains temperature-sensitive even at the lowest temperatures examined. However, in the absence of constraining experimental data, we have opted for the more general mechanism depicted in Figure 7A.
Voltage is also known to influence temperature-sensitivity of TRPV1 (Figure 4B and D) (Voets et al., 2004; Matta and Ahern, 2007; Yao et al., 2010). However, the low permeability of NMDG+ precluded examination of the influence of external Na+ on temperature-sensitivity of TRPV1 at negative voltages. Nonetheless, our data show that at the highly depolarized potentials where we performed our experimental studies and modeling, voltage does not have a predominant influence on temperature-sensitivity of this channel (see Figure 7—figure supplement 3 and Materials and methods for a more detailed discussion), and therefore we did not include voltage in our modeling.
Capsaicin is arguably the best characterized TRPV1 agonist, activating the TRPV1 channel to a maximal Po close to 1 (Premkumar et al., 2002; Hui et al., 2003), and has also been shown to influence temperature-sensitivity of this receptor (Voets et al., 2004; Matta and Ahern, 2007; Yao et al., 2010). We were therefore interested in determining whether it exerts a similar influence on the temperature-sensitivity of TRPV1 as external Na+. To explore this possibility, we measured Po-T relations using slow temperature ramps in the presence of 130 mM external Na+ and different concentrations of capsaicin (Figure 8A and Figure 8A—figure supplement 1A for Po-T relations from individual cells). Although we observed detectable temperature-dependent changes in Po at low temperatures for subsaturating concentrations of capsaicin, the Po values varied by more than 100-fold over the range of capsaicin concentrations, suggesting that capsaicin has a larger effect on the closed/open transition compared to the temperature-dependent transition (Figure 8A - insert). This contrasts with the effects of removing external Na+, which produces much larger shifts in the Po-T relation and smaller changes in Po (Figure 6B). Notably, incorporating these features in our model (Figure 8B) can qualitatively describe our experimental findings with capsaicin (Figure 8A and Figure 8—figure supplement 1A). The Po-T relation in saturating capsaicin exhibited marginal temperature-dependent changes, consistent with a large influence of capsaicin on the open/closed equilibrium of the channel leading to full receptor activation at a saturating concentration of this agonist (Figure 8A).
If capsaicin has a relatively modest influence on the activation of the temperature-sensor (as compared to its larger effects on the open/closed equilibrium), then it should be possible to observe temperature-dependent changes in saturating capsaicin in a construct where capsaicin-bound channels are not fully activated, such as the turret deletion (Figure 3E). To test this possibility, we first determined whether TRPV1 channels lacking the pore turret are temperature-sensitive, as this is a controversial issue (Yang et al., 2010; Yao et al., 2010; Cui et al., 2012; Liao et al., 2013). Interestingly, we found that the turret deletion can still be robustly activated by heat, albeit at somewhat higher temperatures compared to the WT channel (Figure 9A), confirming that the turret is not the temperature sensor.
To look for temperature-dependent changes in Po for the turret-deletion construct at saturating capsaicin, we initially examined the effects of lowering temperature from 22 to 8°C on capsaicin activation in the presence of external Na+ compared to maximal activation in the presence of saturating capsaicin with no external Na+ (Figure 9B). At 8°C, the fractional activation by saturating capsaicin in the presence of external Na+ was substantially lower than what we observed at 22°C, revealing that lowering temperature further decreased the efficacy of capsaicin (Figure 9B; 8°C colored circles; 22°C colored ramps; see black arrows). We then obtained the full Po-T relationship in the presence of external Na+ and capsaicin, as before for the WT channel, but for the turret deletion we observed large temperature-dependent changes in Po, with two components in the relation separated by a clear plateau at intermediate temperatures (Figure 9C and Figure 9—figure supplement 1B for Po-T relations from individual cells). These findings with the turret deletion further support the allosteric framework for conceptualizing the mechanism by which Na+ and capsaicin influence temperature-dependent gating. Notably, we could accurately describe the Po-T relations in saturating capsaicin and the dose-response for external Na+ for the turret deletion using model i (Figure 9—figure supplement 1A and B), simply by assuming that the deletion of the pore turret increased the affinity of the channel for external Na+ and reduced the strength of the coupling between the binding of capsaicin and the opening of the pore (Figure 7—source data 2E). Together, these results qualitatively show that capsaicin influences both the activity of the temperature-sensor and the open/closed equilibrium, but appears to have a larger influence on the latter. Even though the values of the coupling parameters in our modeling are not well-determined, we believe that the larger influence of capsaicin on the open/closed equilibrium is robust enough to support this conclusion.
The results thus far demonstrate that the external pore of TRPV1 contains Na+ ion binding sites that exert strong control over temperature-dependent activation and inactivation, as well as the closed/open equilibrium. Our previous results with DkTx suggest external Na+ and DkTx modulate the TRPV1 through a common mechanism (Figure 3B–D). In addition, our recent analysis of the interaction between DkTx and TRPV1 suggests that the toxin activates the channel by inducing a displacement of the S5-S6 segments relative to the S1-S4 domain (Figure 10—figure supplement 1A), which results in the disruption of a cluster of buried hydrophobic residues at the extracellular ends of the S5 and S6 segments (Bae et al., 2016). This is interesting in light of a recent demonstration in the Shaker Kv channel that movement of hydrophobic residues between buried and solvent-exposed environments imparts temperature-dependence (Chowdhury et al., 2014). We therefore measured Po-T relations in the presence of external Na+ and DkTx to test whether the binding of the toxin has an effect on temperature-sensitivity, and observed that activation of the channel by heat was effectively ablated between 5 and 35°C (Figure 10, and Figure 10—figure supplement 1B for Po-T relations from individual cells). This finding is particularly striking when considering that the Po is situated well below the theoretical upper limit of 1.0. These results demonstrate that DkTx also exerts strong control over temperature-sensor activation, which in our model can be achieved simply by trapping the channel in the intermediate plateau and preventing temperature-sensor deactivation or full activation (Figure 10, insert).
The present results examining the regulation of temperature-dependent gating by external Na+ and capsaicin have four important implications for understanding the gating mechanisms of the TRPV1 channel. First, our results demonstrate that the TRPV1 channel has evolved external Na+ binding sites that must be occupied for the channel to remain closed at physiological body temperatures in mammals. The steeply temperature-sensitive transition that normally opens TRPV1 in response to noxious heat still operates in the absence of Na+, yet without external Na+ the channel would be spontaneously open at physiological temperatures, many channels would be inactivated, and responses to noxious heat would therefore be diminished. Our results also show that the Na+ sites will play physiologically important roles in activation of the channel by acid, as protonation of acidic residues involved in binding Na+ leads to diminished Na+ occupancy and activation of the channel. This connection between Na+ and pH regulation provides a mechanistic explanation for previous observations where mildly acidic solutions potentiate activation of TRPV1 by heat (Jordt et al., 2000). Thus, this Na+ regulatory mechanism plays a fundamental role in tuning the properties of TRPV1 to serve as a detector of noxious heat and acid, and possibly other stimuli that have yet to be examined.
Second, our results reveal the existence of multiple temperature-sensitive transitions that are coupled to the opening transition (see model in Figure 7A ). Although we see only hints of the presence of distinct temperature-dependent transitions in the presence of external Na+ (Figure 4C), they become unambiguous when Na+ is removed (Figure 5D)and when studied in the presence of capsaicin with the turret deletion construct (Figure 9C). Our results suggest that the role of the first temperature-sensitive transition is to maintain the channel in a closed state at physiological temperatures, whereas the second transition functions to activate the channel in response to noxious heat. It is interesting that both Na+ and capsaicin do not seem to have a substantial impact on the second transition, at least to the extent that we could study this component in the presence of inactivation. In contrast, external Na+ exerts strong control over the first transition. Capsaicin also modifies the shape of macroscopic Po-T relations (Figure 8A), but we were able to detect temperature-dependent transitions at low temperatures even in the presence of near-saturating capsaicin concentrations (e.g. 100 nM) that increase the Po at room temperature to values higher than those measured in the absence of external Na+ or in the presence of DkTx (Figure 3C). In contrast, we observed marginal to no temperature-dependence in the Po-T relations at low temperatures in the absence of external Na+ or in the presence of DkTx (Figure 5D and Figure 10). These observations suggest that the vanilloid has a larger influence on the open/closed equilibrium than on the temperature-sensing machinery. The existence of multiple temperature-sensitive transitions also provides a possible explanation for why Po-T relations at negative voltages are at least two-fold steeper than at positive voltages (Figure 4B) (Voets et al., 2004; Yao et al., 2010). If hyperpolarization shifts the temperature-sensitive transition operating at lower temperatures so as to coincide with the second temperature-sensitive transition, the △Ho of the two transitions would add to make the Po-T steeper. Overall, the present results on the influence of Na+ and capsaicin on temperature-dependent gating in TRPV1 provide a set of essential constraints for understanding the gating mechanism of the channel using an allosteric framework.
Third, our results provide clues about where these important Na+ binding sites are located. Because Na+ inhibition has only very weak voltage-dependence, these Na+ binding sites are likely to be located outside the ion permeation pathway within each subunit. Indeed, the large outward Na+ currents we observe on removing external Na+ at positive voltages indicate that the permeation pathway must have a high Na+ occupancy even in the absence of external Na+. Mutating acidic residues forming the external Na+ site would weaken Na+ binding affinity, possibly leading to lower Na+ occupancy in the presence of 130 mM external Na+. However, such an effect would not necessarily cause spontaneous TRPV1 activity because the lower Na+ occupancy would be expected to promote the form of inactivation that we observed on removing external Na+. Additionally, removing external Na+ would be expected to cause less activation of the channel compared to the WT protein because ion occupancy would be diminished by the mutant. E600 in the extracellular loop just after the S5 helix (Figure 3—figure supplement 1A) has been proposed to be responsible for proton-mediated potentiation of heat- and capsaicin-dependent activation of the channel (Jordt et al., 2000), making it an excellent candidate for forming the Na+ binding site. The E600Q mutant displayed modest spontaneous activity when recording at room temperature (Ohta et al., 2008), and only weak activation when removing external Na+ or applying DkTx when compared with the WT channel, consistent with a role in forming the Na+ binding site. Interestingly, E600 is located near the pore turret (Liao et al., 2013) (Figure 3—figure supplement 1A), which when deleted from TRPV1 causes a dramatic increase in the apparent affinity of Na+ (Figure 3F), and this residue is also located very close to where DkTx binds (Cao et al., 2013) (Figure 3—figure supplement 1A and Figure 10—figure supplement 1A).
Finally, our results have important implications for interpreting the recent cryo-EM structures of TRPV1 and in localizing the region of the protein involved in temperature sensing. In the cryo-EM studies on the turret deletion construct of TRPV1, capsaicin appears to produce a partial opening of the internal pore, and the combined influence of RTx and DkTx to produce further expansion of the internal pore together with a conformational change within the selectivity filter (Cao et al., 2013) (Figure 10—figure supplement 1A). These differences between the two structures might indicate that there are two gates that can be differentially regulated by activating stimuli (Cao et al., 2013) (Figure 1A). However, we discovered that capsaicin is a partial agonist of the turret deletion construct, suggesting that the partially open features of the capsaicin-bound channel may not represent a unique conformation of the protein, but an average of closed and open states. The cryo-EM structure of the apo state of TRPV1 (Liao et al., 2013), however, reveals that the internal pore must expand for the pore to support ion permeation, consistent with accessibility studies (Salazar et al., 2009). The observation of temperature-independent plateaus in Po-T relations under diverse conditions that produce submaximal open probabilities suggests that the opening of the pore does not require the two temperature-dependent transitions to occur, and that the open/closed equilibrium itself is not the source of the temperature-sensitivity of TRPV1. If opening of the internal pore is indeed temperature-insensitive, what is the significance of the structural changes in the external pore observed in the structure of the RTx/DkTx-bound channel? The present findings with external Na+ and DkTx suggest that these structural changes in the external pore are tightly associated with the temperature-sensing machinery, either by participating in allosteric coupling or in the actual mechanism of temperature-sensing.
The WT rat TRPV1 channel in pcDNA3.1 vector was kindly provided by Dr. David Julius (UCSF), and subcloned into the low-expression pcDNA1 vector. The E600Q point mutation and Δ604–626 deletion were introduced into rTRPV1 using a two-step PCR mutagenesis technique and the resulting constructs were verified by sequencing.
HEK293 cells were cultured following standard protocols (Li et al., 2015) and transiently transfected with plasmids for the expression of TRPV1 and GFP (pGreen-Lantern, Invitrogen, Carlsbad, CA) using FuGENE6 (Promega, Madison, WI).
Standard whole-cell patch clamp recordings from transiently transfected HEK293 cells at room temperature (22–24°C) were performed unless stated otherwise. The data were acquired with an Axopatch 200B amplifier (Molecular Devices, Sunnyvale, CA), filtered with an 8-pole low-pass Bessel filter (model 900, Frequency Devices, Ottawa, IL) and digitized with a Digidata1322A interface and pClamp10 software (Molecular Devices). All data were analyzed using Igor Pro 6.34A (Wavemetrics, Portland, OR). Pipettes were pulled from borosilicate glass and heat-polished to final resistances between 1 and 5 MΩ. 80–95% series resistance (Rs) compensation was used in all whole-cell recordings except those involving changes in temperature.
The intracellular recording solution consisted of (in mM): 130 NaCl, 10 HEPES, 10 EGTA, pH 7.4 (NaOH/HCl). For experiments involving changes in temperature, 10 mM MgCl2 was added to the intracellular solution to block endogenous inward-rectifying and low-threshold temperature-sensitive currents that were observed in some recordings. The addition of the divalent did not cause any appreciable effect on TRPV1 channel currents, consistent with a previous report (Yang et al., 2014). Moreover, we did not observe significant contaminating currents at room temperature when magnesium was omitted from the pipette solution, except in a small subset of cells that exhibited noticeable inward currents that were easily recognizable due to the outward-rectifying character of TRPV1, and thereby could be readily discarded. The control extracellular solution (130 Nao) consisted of (mM): 130 NaCl, 10 HEPES, 10 EGTA, pH 7.4 (NaOH/HCl). The zero-sodium extracellular solution (0 Nao) consisted of (mM): 130 NMDGCl, 10 HEPES, 10 EGTA, pH 7.4 (NMDG/HCl). For solutions with different extracellular Na+/NMDG+ concentrations, NaCl was replaced with NMDGCl. Capsaicin and capsazepine (100 mM) stock solutions were prepared in ethanol or 1:1 ethanol/DMSO, respectively. All chemicals and reagents were from Sigma-Aldrich (San Luis, MO). DkTx was produced recombinantly, folded and purified as described previously (Bae et al., 2012).
A holding potential of -90 mV was used in all experiments. The data were acquired at 5–10 kHz and low-pass filtered at 2 kHz. For voltage-ramps, voltage was initially stepped down to -120 mV for 50 ms, then ramped up to +140 mV over 1 s before returning to -90 mV. Ramps were applied every 5 s. For I-V relations obtained with steps, voltage was stepped from -90 mV to the test potential for 100 (room temperature recordings) or 400 ms (low temperature recordings, due to slow kinetics), and returned to -90 mV after each pulse. Test pulses went from -120 to +140 mV in 10-mV increments. Current time courses at a fixed voltage were obtained by applying trains of pulses from -90 to +90 mV of either 100 (experiments at room temperature) or 300 ms duration (experiments starting at lower temperatures). The pulse interval was varied, using 3–5 s for I-T relations and 100 ms for time courses at room temperature.
In all experiments at room temperature, a gravity-fed rapid solution exchange system (RSC-200, BioLogic, France) was used. The cells were lifted from the coverslip and placed in front of glass capillaries perfused with different solutions. For I-V relations at a low temperature and fast temperature-jumps, a custom-made temperature-controlled perfusion system was used, as described below and in Figure 5—figure supplement 3A. I-T relations in response to slow temperature ramps were obtained in a temperature-controlled microincubator stage (see below and Figure 4—figure supplement 1A).
Po-T relations were constructed by factoring out the temperature-dependence of conduction through an open channel from I-T relations (see below), and then scaled based on the relative current magnitudes at each condition measured at +90 mV and at room temperature from voltage-ramps (see below for details). The scaling of Po-T relations was also verified using noise analysis (see below).
To obtain a qualitative assessment of the temperature-dependence of channel function, the steepest portions of I-T relations were fit to Equation 1:
where I(T) is the current as a function of temperature, ΔHapp and ΔSapp are the apparent enthalpy and entropy, respectively, T is the temperature (in Kelvins) and R is the gas constant. Approximate Q10 values were calculated from .
All dose-response curves were obtained with voltage-ramps and fit to the Hill equation: , where Imin and Imax are the currents at saturating concentrations of Na+ and 0 Na+, respectively, K1/2 is the concentration of half-maximal inhibition, s is the Hill coefficient and [X] is the molar concentration of Na+. Dose-response relations for extracellular Na+ at pH 7.4 and 5.5 were obtained using 130 mM internal Na+ and, for all test solutions, a total concentration of external monovalent cations (Na+ + NMDG+) of 130 mM. For the dose-response relation at pH 6.0, 300 mM intracellular Na+ was used with a total concentration of external cations of 300 mM. For experiments at pH 6 and 5.5, methanethiosulfonic (MTS) acid was used as a counterion instead of chloride to ablate endogenous proton-activated chloride currents (Lambert and Oberwinkler, 2005). Solutions at pH 6.0 or 5.5 were buffered with 10 mM Bis/Tris or 10 mM MES, respectively.
For obtaining I-T relations a custom-modified temperature-controlled microincubator stage was used (Figure 4—figure supplement 1A). Both T and I were simultaneously recorded and the bath was kept static during the course of the recordings. Only a single experimental solution was tested per cell. Currents were elicited while increasing or decreasing temperature by applying trains of voltage pulses from -90 to +90 mV (from a holding of -90 mV), with pulse durations that ranged from 100 to 400 ms. Longer pulses were used for I-T relations at the lowest temperatures, since activation kinetics were much slower. Pulse length did not have an appreciable effect on I-T relations when evaluated at the same time-points for experiments with different pulse durations (data not shown). For obtaining I-T relations extending to cold temperatures, experiments were started at room temperature, and the temperature was decreased to the lowest value in which TRPV1 currents could still be reliably measured, as indicated by time-dependent relaxations in response to the depolarizing pulses that were at least twice the magnitude of the currents at -90 mV. Immediately after reaching the minimal temperature, experiments were initiated by increasing the temperature. For I-T relations starting at room temperature, the experiments were started without an initial cooling phase.
To generate I-T relations, steady-state currents at +90 mV for each pulse within a train were quantified and plotted as a function of temperature. Since not all individual I-T relations obtained for a given experimental solution contained data at exactly the same temperatures, currents at similar temperatures from different cells were manually matched before averaging both the currents and the temperatures. Individual I-T relations were normalized to their current value at room temperature, and then averaged to obtain mean I-T curves. Standard errors for the temperature are also included in all I-T and Po-T relations shown, but are too small to be seen. No series resistance (Rs) compensation was used in the I-T experiments, since Rs changes with temperature, leading to oscillations and patch rupture during the course of the experiments. To minimize voltage errors, only currents less than 2.5 nA were used for analysis.
Solutions were passed through glass capillary spirals immersed in water baths at different temperatures, and recordings were performed in a small-volume (200–500 µL) chamber during constant perfusion (Figure 5—figure supplement 3A). Temperature was measured with a thermistor located very close to the pipette tip. One perfusion line was used for a given test solution and temperature. An intracellular solution containing 130 mM Na+ + 10 mM Mg2+ was used. All experiments started in 130 Nao at 8°C (Figure 5—figure supplement 3B), followed by 8°C in the absence of external Na+ (i.e. 130 NMDGo) to provide a reference point for normalization before changing to a test solution with or without external Na+ and at T ≥ 11°C. A single test solution was evaluated per cell, and test solutions with and without external Na+ were analyzed separately to generate the I-T relations shown in Figure 5D (grey and orange large circles). In the representative experiments shown in Figure 5—figure supplement 3B, the test solutions were 0 Nao at 32°C (left panel) and at 22°C (right panel). In some cases, saturating capsaicin at room temperature was applied at the end of the experiment. For each cell, the current measured in the test solution was normalized to the current in control solution (i.e. 0 Nao, 8°C), and the resulting ratio averaged among experiments obtained using the same test condition (both temperature and presence or absence of external Na+). An I-T relation (either with or without external Na+) was finally constructed by plotting together the mean current ratios as a function of the temperature of the test solution. The final I-T relations in Figure 5D were scaled so that the current ratio at room temperature (22°C) was equal to 1.
Temperature-dependent changes in macroscopic currents have two predominant sources: the temperature-dependence of channel gating (Po(T), opening and closing of the pore) and the rate of ion conduction through an open channel i(T). The contribution of the leak currents was considered negligible since the magnitude of the measured currents was always considerably larger than the magnitude of the leak, and accounting for the leak did not significantly change the shape of the I-T or Po-T relations under any condition (data not shown). To estimate the temperature-dependence of ion conduction through an open channel we measured I-T relations in the presence of a saturating concentration of capsaicin, a condition in which all channels remain open over the experimental temperature range. I-T relations in saturating capsaicin (Figure 4—figure supplement 1B, closed circles) could be satisfactorily fit by a single exponential function of temperature () over the studied temperature range, indicating that Po does not change appreciably from 7–40°C. This is also consistent with G-V relations obtained from families of voltage pulses at room temperature (Figure 1—figure supplement 3A) and at 8°C (Figure 7—figure supplement 3A) in saturating capsaicin with 130 mM extracellular Na+, which superimpose very well and show clear saturation at positive potentials (Figure 7—figure supplement 3B). Individual I-T experiments were normalized by their own fits to Equation 1, and the resulting data were normalized to their respective values at 24°C before averaging, to finally generate a curve that only reflects changes in Po as a function of temperature (Figure 4—figure supplement 1B, open circles). As expected, the resulting normalized Po-T relation for saturating capsaicin does not exhibit large temperature-dependent changes. The mean enthalpy for ion conduction estimated this way (9.0 ± 0.5 kcal/mol, Figure 4—figure supplement 1B, insert) was used to factor i(T) out of all other macroscopic I-T relations (see Figure 4—figure supplement 1F for an example of an I-T to Po-T transformation for data obtained with 130 mM external Na+). Single-channel current amplitude measurements at +90 mV with and without external Na+ measured at several temperatures (Figure 4—figure supplement 1C and D) could be satisfactorily fit by Equation 1 with an enthalpy of 9 kcal/mol (Figure 4—figure supplement 1E, see below for experimental details) and our estimate of 9 kcal/mol for the temperature-dependence of i(T) is close to previous estimates for TRPV1 (Liu et al., 2003; Grandl et al., 2010) and other ion channels (Hille, 2001).
Data for single-channel recordings were acquired at 10 kHz and filtered at 2 kHz using pipettes with resistances of 5–14 MΩ. Pipettes were covered in Q-dope or dental wax. Currents were elicited by 500-ms pulses from -90 to +90 mV every 100 ms during heating-temperature ramps in outside-out patches containing a few channels (Figure 4—figure supplement 1C and D). Temperature was controlled with the micro-incubator stage (Figure 4—figure supplement 1A). Traces without channel openings were used for leak subtraction. All-points histograms for data obtained within a 2°C interval were assembled from segments of recordings where single-channel openings were clearly discernible, and data were fitted to a sum of Gaussian functions to obtain the mean current value for a single open channel (Figure 4—figure supplement 1E).
Once the temperature-dependence of ion conduction for an open channel has been factored out of I-T relations, the resulting data reflect only the changes in Po as a function of temperature. To graph the resulting relations on an absolute Po scale, we used the relative magnitudes of macroscopic currents at room temperature measured with the different solutions tested in this study. I-V relations in saturating capsaicin with and without external Na+ superimpose at positive potentials (Figure 1C), we did not observe large changes in single channel conductance at +90 mV and at room temperature between patches with or without external Na+ (Figure 2A), and capsaicin does not affect the single-channel conductance of TRPV1 (Premkumar et al., 2002; Hui et al., 2003), suggesting that the single channel current at positive voltages is not substantially altered under our experimental conditions. Based on measurements provided in the literature using single-channel recordings (Premkumar et al., 2002; Hui et al., 2003) or noise-analysis of macroscopic currents (Oseguera et al., 2007), we assumed that the Po in saturating capsaicin (10 µM) + 130 mM external Na+ at +90 mV and at room temperature is ~0.9. The Po at room temperature and +90 mV for 0 Nao (i.e., 130 mM extracellular NMDG) was then estimated from the macroscopic I-V relations (Figure 5—figure supplement 2A and C) to be ~0.2. For other experimental conditions where Po is similar to that measured in 0 Nao, we estimated the Po-values at room temperature and +90 mV simply by recording I-V relations at the test conditions and 0 Nao and scaling based on 0 Nao. The following conditions were scaled in this way (Figure 5—figure supplement 2A and C): 0 Nao + 1 µM Cpz., 0 Nao + 10 µM Cpz., 10 Nao, 30 Nao, 130 Nao + 100 nM caps., 130 Nao + 25 nM caps., 130 Nao + 1 µM DkTx. For experimental conditions where Po was much lower than for 0 Nao, we used 30 Nao as a reference in cells expressing TRPV1 to higher levels (Figure 5—figure supplement 2B and C). The following conditions were scaled in this way: 130 Nao, 65 Nao, 130 Nao + 10 nM caps. Notably, the Po value estimated here for 130 Nao is consistent with measurements of unliganded Po for TRPV1 at depolarized potentials (Oseguera et al., 2007). We also validated our scaling procedure using noise analysis (see below for methodological description). Using this approach, we obtained a mean Po at ~24°C of 0.91 ± 0.02 (mean ± SEM, n = 4) for data in 130 Nao + 10 µM caps. and a Po of 0.21 ± 0.04 in the absence of external Na+ and capsaicin (see Figure 5—figure supplement 2G for Po values from individual cells at different temperatures), which is very close to our initial estimated values.
It is important to note that our estimated absolute Po values from macroscopic recordings in HEK293 cells in the presence of external Na+ at elevated temperatures are almost an order of magnitude lower than those measured previously using single-channel recordings from oocytes (Liu et al., 2003), which showed that the Po at T > 50°C is close to 1. Macroscopic recordings from the same group performed at T > 50°C with and without capsaicin also show that the addition of the vanilloid produces an increase in Po of at least twofold (Yao et al., 2010), suggesting that Po at high temperatures can be substantially less than 1. Macroscopic data from other laboratories also show less-than-maximal channel activation by temperature as compared with saturating capsaicin (Cao et al., 2014). One important consideration in comparing single-channel and macroscopic data is the fact that temperature-inactivated channels can still respond to saturating capsaicin (Cao et al., 2014), and that temperature-dependent channel inactivation (or rundown) also occurs in the presence of external Na+, so that it is possible that a subset of channels in HEK293 cells cultured at 37°C are inactivated and therefore unresponsive to heat. This would lead to an underestimation of the Po in the absence of external Na+ or in heat-activation experiments in the presence of Na+ when measured from macroscopic current recordings, as in the present study. However, we think that this underestimation is not large given our noise-analysis results in the absence of external Na+ (Figure 5—figure supplement 2D–G) and the observation of frequent closures in our outside-out recordings where the activity of single channels can be discerned, indicating that the Po in the absence of external Na+ is not maximal even at 30°C (Figure 2A and Figure 4—figure supplement 1D). Given that all Po-T relations were scaled under similar conditions, a systematic underestimation of the Po would not change any of the conclusions of the present work.
A hybrid non-stationary/stationary noise analysis method was used. The data were acquired at 100 kHz and filtered at 15 kHz, and pipettes were covered in Q-dope or dental wax to reduce noise and stray capacitances. Series resistance compensation (90% ) was used in all recordings. Whole-cell and pipette capacitances were also compensated. For experiments at T > 6°C, temperature was controlled using perfusion (Figure 5—figure supplement 3A). The temperature-controlled recording chamber (Figure 4—figure supplement 1A) was used for experiments at T < 6°C. The data were acquired at a single temperature per cell. For the WT channel, currents in response to 40–50 voltage pulses (3 s inter-pulse interval) of 400 ms duration from -90 to +90 mV were obtained at 0 Nao, followed by another 50 pulses at 10 µM capsaicin + 130 Nao. For TRPV1-Δ604–626, 10 traces were obtained in 0 Nao (not used for analysis), followed by 50 traces in 10 µM capsaicin + 130 Nao, and finally 50 traces in 0 Nao + 10 µM capsaicin. For each experiment, the current variance (σ2I) was calculated from the ~50 current traces obtained with the same extracellular recording solution (i.e. 0 Nao or 130 Nao + caps, for the WT channel) as the ensemble average of the squared differences of successive currents records (Heinemann and Conti, 1992; Alvarez et al., 2002), an optimal method for channels with rundown. Briefly, we first calculated difference records yj between current traces xj elicited by successive voltage steps as: , where j goes from 1 to the total number N of current traces recorded at a given experimental condition (i.e. ~50 for most experiments). The variance σ2I was then calculated from: , where is the mean of the difference records. The mean current (Imean) traces for each experiment were calculated by averaging together all ~50 current records obtained in the same experimental condition (see example in Figure 5—figure supplement 2E). To correct for leak and baseline variance, σ2I and Imean calculated from the steady-state data points at -90 mV and 0 Nao (0 Nao + caps for TRPV1-Δ604–626) were subtracted from σ2I and Imean, respectively, measured at +90 mV at the other experimental condition(s). The initial and final points of the σ2I and Imean traces at +90 mV were deleted due to contaminating capacitive currents that could not be fully compensated. Data for the two conditions (i.e. 0 Nao and 130 Nao + caps, for the WT channel) were then plotted together in σ2I vs Imean plots (see example in Figure 5—figure supplement 2D), and fitted to Equation 2:
where i is the single-channel current amplitude and N is the number of channels in the cell. The open probability (Po) at both conditions was then calculated from the two mean steady-state current (Imean,ss) traces (such as those in Figure 5—figure supplement 2E) and the values for i and N obtained from fits of Equation 2, using Equation 3:
(see Figure 5—figure supplement 2G for all calculated Po-values for the WT channel at both 0 Nao and 130 Nao + caps.). The noise-analysis approach used here assumes that i and N are not changed by Na+-removal or addition of capsaicin, since data obtained at two different conditions were plotted together in our variance vs mean plots, and fitted with the same parameters. We believe this assumption to be supported by several lines of evidence, as discussed above.
It is important to note that the single-channel current values at +90 mV estimated from noise analysis systematically underestimate i by a factor of ~2 when compared to single-channel recordings (Figure 5—figure supplement 2F). This underestimation was the same for experiments performed at all temperatures and also for both WT and Δ604–626 channels. When σ2I vs Imean plots were fit by Equation 2 while constraining the value of i based on single-channel recordings (see red fit in Figure 5—figure supplement 2D), the resulting values for N were considerably smaller than those obtained from unconstrained fits. However, the Po calculated using parameters from unconstrained fits are similar to that calculated using constrained fits (Figure 5—figure supplement 2G), indicating that the noise analysis provides approximate estimates of the Po that coincide with equivalent values obtained using single-channel recordings (Premkumar et al., 2002; Hui et al., 2003). Notably, the temperature-dependence of i-T relations obtained from the estimates of i using noise analysis is consistent with estimates we obtained from macroscopic I-T relations in saturating capsaicin and single-channel recordings (Figure 5—figure supplement 2F).
The allosteric model i is conceptually simple and contains the necessary features to qualitatively reproduce the most relevant aspects of our data pertaining to the effects of temperature, external Na+ and capsaicin on the gating of TRPV1. A slightly simpler version of the model (with only a single temperature-dependent transition) has been used to accurately reproduce the effects of capsaicin, voltage and a narrow range of temperatures in TRPV1 (Matta and Ahern, 2007; Yao et al., 2010; Gregorio-Teruel et al., 2014; Gregorio-Teruel et al., 2015). However, four mechanistically relevant assumptions inherent to this model are not so evidently justified by the data, and require further discussion.
The most important assumption regarding the model is that the opening transition is temperature-independent. This feature of the model was incorporated in order to reproduce the plateaus observed in some Po-T relations, in which the Po does not increase with temperature despite being well below its maximal theoretical value of 1.0 (Figure 5E). Are there other gating mechanisms that produce temperature-independent gating at Po < 1.0 and have a temperature-dependent open/closed equilibrium? This is relevant given a recent study on Kv channels, which suggested that the opening transition of channels structurally related to the TRPV1 can be steeply temperature-dependent (Yang et al., 2014). Additionally, if the opening transition were responsible for the heat-activation of the TRPV1, a lot of information on the elusive mechanism of temperature-dependent gating could be readily gained from the structures of the channel in the closed and open states (Cao et al., 2013). A temperature-dependent open/closed equilibrium implies that the enthalpies (Ho) associated with the open and the closed states are different (i.e. ΔHo is large). A modulator such as Na+ could affect the temperature-dependence of channel opening by altering the enthalpy of the open or the closed state such that ΔHo changes. In this scenario, a temperature-independent opening transition (with ΔHo ≈ 0) could become temperature-dependent through the binding of sodium, if sodium increases the enthalpy of the open state or decreases the enthalpy of the closed state. The resulting Po-T relations would be flat (no temperature-dependence) in the absence of Na+, and steeply temperature-dependent in the presence of Na+. However, our experimental results suggest that the channel retains temperature-dependence in the absence of external Na+, as evidenced by the steep I-T relations at T > 30°C obtained from temperature jumps (Figure 5D) and the I-T relations at low temperatures in the presence of capsazepine without external Na+ (Figure 6A). This indicates that external Na+ is not directly responsible for conferring temperature-sensitivity to the TRPV1 channel. Thus, a model in which external Na+ confers temperature-sensitivity to the opening transition would require distinct Na+-independent heat-driven transitions to occur in the absence of external Na+ in order to replicate our experimental results. Model ii (Figure 7—figure supplement 1A) incorporates these requirements and reproduces our experimental findings with comparable accuracy as model i (Figure 7—figure supplement 1B). However, model ii is mechanistically more complex than model i, since it requires distinct temperature-dependent transitions depending on whether the channel is bound to external Na+ or not, implying that the TRPV1 possess different mechanisms of temperature-sensing. On the contrary, model i requires a single pair of temperature-dependent transitions and a common mechanism for temperature-sensing. Although a distinction between the two possibilities cannot be made, we favor model i due to its simplicity. Additionally, it can be concluded that the opening transition is not obligatorily temperature-dependent, but could become temperature-dependent under more complex models for TRPV1 channel gating.
The second important assumption is the inclusion of an additional temperature-dependent transition in model i. The inherent complexity of Po-T relations in 130 Nao (Figure 4C) strongly suggest that there are at least two temperature-dependent transitions involved in the gating mechanism of the TRPV1 channel. Furthermore, the Po-T relations obtained with the turret-deletion construct in saturating capsaicin and external Na+ unambiguously show the presence of at least two different temperature-dependent transitions associated with gating of TRPV1 (Figure 9C and Figure 9—figure supplement 1B). One transition appears to dominate temperature-dependent gating at T > 38°C, and represents the steep temperature-dependence that has been measured for TRPV1 in previous studies (Liu et al., 2003; Voets et al., 2004; Yao et al., 2010; Cao et al., 2013). Another transition dominates channel activity at lower temperatures, and appears to have a somewhat lower temperature-dependence, although this may only be the result of this temperature-dependent transition being close to saturation in the experimentally accessible range of temperatures. If the data is simulated using a model with a single temperature-dependent transition (Model iii, Figure 7—figure supplement 1C) with a large associated enthalpy, the resulting Po-T curves at T < 35°C would be steeper than the experimental data. If the enthalpy for the temperature-sensor is chosen such that the model agrees well with the experimental data at T < 35°C, then the predicted Po-T relations lack the highly temperature-dependent increase in Po at T > 38°C that is characteristic of the TRPV1 channel (see the predictions in Figure 7—figure supplement 1D), indicating that activation of the TRPV1 by heat involves at least two temperature-dependent transitions. Finally, we arranged the two temperature-dependent transitions in Model i sequentially, as opposed to considering them as separate coupled equilibria in a parallel arrangement. We chose a sequential arrangement of the transitions because it reduces the number of states in the model and eliminates a free parameter (the allosteric coupling constant between the two temperature-dependent transitions). However, fits to the experimental Po-T relations of identical quality could be obtained with a parallel arrangement of temperature-sensors (data not shown), so that this aspect of the model is unconstrained.
A third assumption in Model i is that external Na+ can bind to the TRPV1 in all of its possible conformations (i.e., there are no states to which sodium cannot bind). This has important implications for the mechanism of Na+-regulation because one alternate mechanism by which sodium could inhibit the TRPV1 channel is by binding exclusively to the closed state. In that case, sufficiently high concentrations of external Na+ should completely prevent opening of the channel by other stimuli. We can exclude this possibility because the channel can be robustly opened with capsaicin (Figure 1C) and heat (Figure 4A) in the presence of a saturating concentration of Na+ (130 mM), or even when the concentration of extracellular Na+ ions is increased to 600 mM (Figure 7—figure supplement 2A) or 2 M (data not shown). In addition, temperature-dependent activation of TRPV1 in the presence of 600 mM external Na+ does not qualitatively differ from that measured with 130 mM external Na+ (Figure 7—figure supplement 2B), suggesting that external Na+ does not modulate the temperature-sensor by binding exclusively to its resting state.
The fourth assumption in the modeling was to neglect the effect of voltage-dependent gating on the calculated Po-T relations, given that all experimental data were obtained at a fixed voltage. The low permeability of NMDG+ relative to Na+ greatly limited the range of voltages over which we could obtain useful data at most of the relevant experimental conditions in this study (see Figure 1—figure supplement 4). We therefore decided to estimate how much could changes in voltage above 0 mV alter the shape of Po-T curves in both saturating capsaicin and in the absence of Na+. To do this, we first calculated G-V relations in saturating capsaicin at two temperatures (22°C and 8°C) from families of currents elicited by voltage-steps from -120 to +140 mV (Figure 1—figure supplement 3A and Figure 7—figure supplement 3A). The G-V relations at both temperatures reach saturation at 0 mV (Figure 7—figure supplement 3B), indicating that voltage does not appreciably influence channel gating and its temperature-dependence in saturating capsaicin at positive membrane potentials, consistent with previous measurements (Matta and Ahern, 2007; Yao et al., 2010). Furthermore, this indicates that voltage-dependent changes in the I-V relations in saturating capsaicin at positive voltages reflect only the changes in single-channel current as a function of voltage but not changes in Po. We therefore divided the I-V relations in the absence of external Na+ (22°C, Figure 1—figure supplement 3A; 8°C, Figure 7—figure supplement 3A) by the I-V relations in saturating capsaicin to obtain the fraction of open channels (Po) as a function of voltage for data at both temperatures (Figure 7—figure supplement 3C). The resulting Po-V relations at the two temperatures superimpose, confirming that removal of external Na+ leads to negligible temperature-dependence in channel gating over a range from 5 to 25°C. Moreover, the Po-V relations show only weak voltage-dependence, suggesting that the effects of voltage-dependent gating on our Po-T relations measured at a fixed voltage should have a minimal influence on the interpretation of our results. We therefore decided not to include voltage-dependent transitions in our final model.
One final modification to the model was included to better account for the Na+ and capsaicin concentration-dependence of Po, since both modulators seem to exhibit weak cooperativity. Indeed, cooperative interactions between capsaicin and protons have been proposed to occur (Ryu et al., 2003), as well as positive cooperativity in the binding of other vanilloids (Acs and Blumberg, 1994). To explicitly introduce cooperativity would have required us to extend the model to take into account the tetrameric assembly of TRPV1, incrementing the number of states, free parameters and assumptions necessary to model the data. We therefore introduced an arbitrary cooperativity term for the binding of both Na+ and capsaicin as is done in the Hill model of cooperativity, such that the modified capsaicin- or Na+-dependent equilibrium constants had the form: K1 = (K1’ x [Na])1.5 and K2 = (K1’ x [caps.])1.5.
Po values from the models were calculated using programs written in Igor. Data was fit by visual inspection while manually varying the parameters.
The molecular mechanism underlying high-temperature sensitivity in thermo-TRP channels remains unknown. In this regard, it was recently noted that changes in side-chain hydration associated with a protein conformational transition that involves only a few residues could result in moderate changes in ΔCp, which in turn would render that conformational change highly temperature-sensitive (Clapham and Miller, 2011). The applicability of this molecular mechanism for ion channels was recently demonstrated using voltage-gated potassium channels with engineered voltage-sensing domains (Chowdhury et al., 2014). Given the possibility that ΔCp is responsible for the temperature-sensitivity in TRPV1 channels, we tested whether considering a change in heat capacity for both temperature-dependent transitions in model i would have an influence on the behavior of the model and the interpretation of our results. Under this framework, equilibrium constants J(T) with the following form were selected (Clapham and Miller, 2011): , where ΔSo(T0) is the standard entropy change at reference temperature T0, R is the gas constant and T the temperature (in Kelvins). Notably, the fits to the experimental data generated by model i with ΔCp ≠ 0 are indistinguishable from those generated without considering a change in heat capacity (ΔCp = 0) (Figure 7—figure supplement 4B), as long as the respective equilibrium constants J1(T) and J2(T) take similar values in the experimentally explored range of temperatures (Figure 7—figure supplement 4A). No changes in parameters other than those associated with J1(T) and J2(T) were required (Figure 7—source data 2E). Thus, our results are equally compatible with temperature-sensing mechanisms that do or do not invoke changes in heat capacity.
Comparison of I-T relations obtained using slow temperature ramps and fast temperature jumps in the absence of external Na+ (Figure 5D) indicates that temperature-dependent inactivation can dominate the behavior of Po-T relations, obscuring the high temperature-sensitivity of gating of the TRPV1 channel. This phenomenon is apparent for several of the experimental Po-T curves measured in this study. However, since temperature-dependent inactivation is irreversible, it cannot be included in the mathematical models in this study, which are for equilibrium conditions. Nonetheless, we were interested in determining whether a simple decaying exponential function of time (to simulate inactivation) could effectively reduce the steepness of Po-T curves and ultimately lead to a steep temperature-dependent decrease in Po. The exponential function of time f(t) had the form: , where t is time and k(T) is a temperature-dependent rate constant given by: , where k0 is a pre-factor (see below), ΔH≠ is the activation enthalpy for the inactivation process, ΔS≠ is the activation entropy, R is the gas constant and T the temperature. The Po-T relation with inactivation would then be given by: The mechanism by which temperature-dependent inactivation depends on Na+, open probability and temperature is unknown and beyond the scope of this study. However, we decided to incorporate Na+-dependence in an arbitrary way that would yet allow us to qualitatively assess the effects of an exponentially decaying function of time and temperature on the Po-T curves at several Na+ concentrations. We therefore arbitrarily assigned k(T) a Na+- and temperature-dependent pre-factor k0 as follows: , where A is a constant and FNa is the fraction of Na+-bound states at equilibrium relative to the total number of states in model i. Finally, to include time in the final calculation of inactivating Po-T curves we took advantage of the sigmoidal shape of our experimental temperature vs time plots (see the inserts on Figure 4A and 5A), allowing us to have an empiric function to transform the temperature in the x-axis of Po-T plots into time. The function was: , where Tmax is the maximal temperature (which was set to 333 K) and T is the temperature (in Kelvins). Figure 7—figure supplement 5A shows a calculated temperature vs time plot, which was then used to obtain Po-T curves with inactivation (Figure 7—figure supplement 5B). This approach allowed us to replicate the overall shape of Po-T curves with inactivation and their Na+ dependence, confirming that temperature-dependent inactivation can indeed reduce the apparent steepness of Po-T relations and ultimately leading to a steep decay in open probability. The parameters used in the modeling were: A = 200, ΔH≠ = 45 kcal/mol, ΔS≠ = 0.133 kcal/mol.
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David E ClaphamReviewing Editor; Howard Hughes Medical Institute, Boston Children's Hospital, United States
In the interests of transparency, eLife includes the editorial decision letter and accompanying author responses. A lightly edited version of the letter sent to the authors after peer review is shown, indicating the most substantive concerns; minor comments are not usually included.
Thank you for submitting your work entitled "An external sodium ion binding site controls temperature-dependent gating in TRPV1 channels" for consideration by eLife. Your article has been favorably evaluated by Richard Aldrich (Senior editor) and three reviewers, one of whom, David Clapham, is a member of our Board of Reviewing Editors, and another is Baron Chanda.
The reviewers have discussed the reviews with one another and the Reviewing Editor has drafted this decision to help you prepare a revised submission.
Jara-Oseguera, Bae, and Swartz carry out the most thorough biophysical investigation of the TRPV1 channel to date and establish the allosteric nature of capsaicin and temperature gating of this important ion channel. The general question is how TRPV1 responds to small temperature changes. The results demonstrate that the TRPV1 channel has an external Na binding site that must be occupied for the channel to remain closed at physiological temperature, and is also likely responsible for acid sensing. The Na+ regulatory mechanism thus tunes TRPV1 for noxious stimuli. The authors find evidence for multiple temperature-sensitive transitions that couple to a relatively temperature-insensitive opening transition; the first temperature-sensitive transition maintains the channel in a closed state at physiological temperatures, whereas the second transition functions to activate the channel in response to noxious heat. Na+ inhibition has only very weak voltage-dependence, and there is substantial evidence in this paper that the site is near the turret, likely involving E600 in the extracellular loop just after the S5 helix and close to the DkTx binding site. This is a solid contribution to the field and for the first time provides evidence for multiple temperature-dependent transitions in the TRPV1 channel. Nevertheless, we have some concerns mainly with regards to the interpretation of their data and its implications.
Points to consider in the revision:
1) The data and their models are consistent with an allosteric site for sodium binding which when occupied favors channel closure. This allosteric site like all the other allosteric sites has an independent equilibrium constant and is coupled to pore opening with a coupling constant. It also coupled to temperature-sensors and capsaicin binding site with coupling constants of different strengths. However, the manuscript is presented as if the sodium binding site is uniquely involved in temperature-dependent gating. The title states that "sodium ion binding site controls temperature-dependent gating" whereas, in our opinion, it would be more appropriate to state that "sodium ion binding site is allosteric modulator of pore gating". The sodium ion binding site is as much of an influence on temperature-dependent gating as capsaicin, protons or voltage-sensor which incidentally was not included in this model. While the authors might argue that the coupling constants that link sodium ion binding site to the temperature-sensor activation is much higher than those linking capsaicin binding site, we think that simply reflects the problem of parameter identifiability. It is unclear whether these equilibrium parameters are unique especially in absence of kinetic constraints. For instance, if these model parameters are correct, then the coupling constants that link temperature dependent transition to pore opening is much smaller than those that link capsaicin binding or sodium activation to channel opening (models i and iii). Therefore, by this logic the TRPV1 channels are only weakly activated by temperature. In light of these uncertainties, it is incumbent on the authors to interpret their models with a degree of parsimony. These caveats should be also reflected in their Abstract.
2) The calculated Po in presence of full sodium is much smaller than 0.1 even at their highest temperatures (Figure 4C). Previous work from Feng Qin's lab using single channel measurements (Biophysical Journal 2003) showed that the Po values for TRPV1 channels at 50 degrees reach very close to 1. At 45 degrees, their Po values were 0.5 whereas in this manuscript the Po values are approximately 0.06 at those temperatures. Why is there so much discrepancy in the Po values even though both groups are studying the same channel expressed in Hek cells? Qin and coworkers obtained their Po measurements directly from single channel recordings whereas in this manuscript Po is deduced from macroscopic currents after correcting for temperature-dependent changes in conductance.
3) The authors do not have strong evidence to suggest that the temperature-sensor is allosterically coupled to the pore. A hallmark of allosteric system is that one should be able to observe temperature-independent transitions at both high and low temperatures. According to their models, the saturation at low temperatures will occur at ranges that would be experimentally intractable and at high temperatures this would be complicated by inactivation (or desensitization?). This is an unfortunate situation that ultimately makes it difficult to discriminate between an allosteric versus an obligatorily coupled temperature-sensor. To be fair, the authors acknowledge this problem and state that they favor the allosteric model because it is simpler. I would argue that an obligatorily coupled model has fewer free parameters than an allosteric model. Again these caveats should be clearly stated in their conclusion.
4) TRPM7 is ubiquitous and contributes to outward currents in all cells we have examined. This current runs up over time if Mg is omitted from the pipette (free Mg < 1 mM). The authors have used 10 mM Mg inside the cell in temperature experiments, but they might want to check in other cases where capsaicin, DkTx, and other experimental manipulations are carried out without temperature changes that the currents are not contaminated by M7.https://doi.org/10.7554/eLife.13356.035
- Kenton J Swartz
The funders had no role in study design, data collection and interpretation, or the decision to submit the work for publication.
We thank Mark Mayer, Joe Mindell, Shai Silberberg, Gilman Toombes and members of the Swartz lab for helpful discussions. We thank David Ide for help in manufacturing elements of the temperature-control system. This work was supported by the Intramural Research Program of the NINDS, NIH (to KJS) and by an NINDS Competitive Postdoctoral Fellowship (to AJO).
- David E Clapham, Reviewing Editor, Howard Hughes Medical Institute, Boston Children's Hospital, United States
- Received: November 26, 2015
- Accepted: January 28, 2016
- Version of Record published: February 12, 2016 (version 1)
This is an open-access article, free of all copyright, and may be freely reproduced, distributed, transmitted, modified, built upon, or otherwise used by anyone for any lawful purpose. The work is made available under the Creative Commons CC0 public domain dedication.