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1 Rammelkamp Center for Education and Research, MetroHealth Medical Center, Cleveland, OH 44109, USA
2 Department of Physiology and Biophysics, Case Western Reserve University School of Medicine, Cleveland, OH 44106, USA
| Abstract |
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4%) to whole-cell currents in the presence of extracellular Na+. Measurement of single-cell fura-2 fluorescence during perforated-patch recording of TRPC6 currents showed that OAG increased [Ca2+]i 50100 nM when the membrane potential was clamped at between 50 and 80 mV, but had little or no effect if the membrane potential was left uncontrolled. These results suggest that in cells exhibiting a high input resistance, the primary effect of activating TRPC6 will be membrane depolarization. However, in cells able to maintain a hyperpolarized potential (e.g. cells with a large inwardly rectifying or Ca2+-activated K+ current), activation of TRPC6 will lead to a sustained increase in [Ca2+]i. Thus, the contribution of TRPC6 current to both the kinetics and magnitude of the Ca2+ response will be cell specific and dependent upon the complement of other channel types.
(Received 6 December 2005;
accepted after revision 25 January 2006;
first published online 26 January 2006)
Corresponding author W. P. Schilling: Rammelkamp Center for Education and Research, Room R-322, MetroHealth Medical Center, 2500 MetroHealth Drive, Cleveland, OH 44109-1998, USA. Email: wschilling{at}metrohealth.org
| Introduction |
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Over-expression of TRPC6 channels in HEK 293 (Inoue et al. 2001; Dietrich et al. 2003), COS-7 (Boulay et al. 1997; Zhang & Saffen, 2001) and CHO-K1 cells (Hofmann et al. 1999) is associated with an enhanced Ca2+ influx as indicated by fluorescent Ca2+ dyes, suggesting that these channels may be Ca2+ permeable. However, the data from electrophysiological studies are unclear on this point. Heterologous TRPC6 currents have been characterized in different cell types and are clearly activated by receptor stimulation and exogenous application of DAG analogues (Hofmann et al. 1999; Inoue et al. 2001; Estacion et al. 2004). Inward TRPC6 current is greatly attenuated by replacement of monovalent cations in the bath by the large relatively impermeant cation, N-methyl-D-glucamine (NMDG) and the reversal potential shifts to negative values demonstrating that TRPC6 channel has permselectivity expected for a non-selective cation channel. However, replacement of monovalent cations in the bath solution by Ca2+ causes substantial reduction in outward current via TRPC6 channels (Inoue et al. 2001), suggesting that Ca2+ may act as a channel blocker. In a recent study, increases in Ca2+ from the normal value of 2 mM to 10 mM in the presence of Na+ produced a substantial reduction in TRPC6 inward current (Shi et al. 2004), again suggesting channel block. However, the actual percentage of whole-cell TRPC6 currents attributable to Ca2+ influx in the presence of normal extracellular Na+ remains unknown. Therefore, the purpose of the present study was to compare receptor-mediated changes in Ca2+ influx measured using fura-2 with changes in membrane currents in cells expressing human TRPC6 channels. Fura-2 measurements were performed on dispersed cells in a cuvette-based assay, and TRPC6 currents were measured using the patch-clamp technique in whole-cell recording mode. In addition, simultaneous recordings of TRPC6 current and fura-2 fluorescence were obtained at the single-cell level using the perforated-patch technique and fluorescence video microscopy. The results are consistent with a pore permeation model in which Ca2+ acts primarily as a blocking ion and contributes only a small percentage to whole-cell currents in the presence of Na+. Furthermore, Ca2+ entry via TRPC6 was greatly attenuated by depolarization. Thus, in cells with a high input resistance, activation of TRPC6 current will primarily cause depolarization, greatly attenuating Ca2+ entry via TRPC6 channels. However, in cells able to maintain a negative membrane potential, for example, cells with a robust Ca2+-activated or inwardly rectifying K+ current, the depolarizing effect of TRPC6 will be reduced and the driving force for Ca2+ entry will be enhanced. In this way, TRPC6 current will serve a dual signalling role (i.e. depolarization versus sustained Ca2+ entry) that will be cell specific and dependent upon the complement of other channel types. A preliminary report of this work has been published (Estacion et al. 2005).
| Methods |
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Normal Hepes-buffered saline (HBS) contained (mM): NaCl 140, KCl 5, MgCl2 1, CaCl2 1.8, D-glucose 10 and Hepes 15 with 0.1% bovine serum albumin; pH was adjusted to 7.4 at 37°C with NaOH. Ca2+-freehigh-K+ HBS contained (mM): KCl 145, MgCl2 1 EGTA 0.3, D-glucose 10 and Hepes 15 with 0.1% bovine serum albumin; pH was adjusted to 7.4 at 37°C with NaOH. RHC80267, U73122 and U73343 were obtained from Calbiochem. Fura-2 acetoxymethyl ester (fura-2 AM) was obtained from Molecular Probes. 1-oleoyl-acetyl-sn-glycerol (OAG), obtained from Sigma in single-use aliquots, was dissolved in ethanol at a final concentration of 30 mM and used immediately for experimentation. All other salts were of reagent grade.
Cell culture
HEK 293 cells were grown at 37°C in monolayer culture in a humidified air atmosphere with 5% CO2 using minimal essential medium or Dulbecco's modified Eagle's medium supplemented with 2 mML-glutamine, 10% heat-inactivated fetal bovine serum and 1% penicillin-streptomycin-neomycin antibiotic mixture (GIBCO).
Expression of TRPC6 in mammalian cells
The transfection and clonal selection of cell lines stably expressing human TRPC6 channels was previously described (Estacion et al. 2004). Unless otherwise indicated, all experiments reported here were performed using TRPC6-clone 14 cells, serially cultured under continuous selection pressure with G418.
Measurement of free cytosolic Ca2+ concentration
Cuvette experiments.
[Ca2+]i was measured using the fluorescent indicator, fura-2, as previously described (Schilling et al. 1989). Briefly, cells were harvested and re-suspended in HBS containing 20 µM fura-2 AM. Following 30-min incubation at 37°C, the cell suspension was diluted
10-fold with HBS, incubated for an additional 30 min, washed and resuspended in fresh HBS. Aliquots from this final suspension were washed twice immediately prior to fluorescence measurement and resuspended in Ca2+-freehigh-K+ HBS. Fluorescence was recorded in a mechanically stirred cuvette using an SLM 8100 spectrophotofluorometer. For measurements of [Ca2+], excitation wavelength alternated between 340 and 380 nm every second, and fluorescence intensity was monitored at an emission wavelength of 510 nm. Calibration of the fura-2 associated with the cells was accomplished with lysis by Triton X-100 in the presence of a saturating concentration of Ca2+ followed by addition of EGTA (pH 8.5). [Ca2+]i was calculated using the equations of Grynkiewicz et al. (1985) using a Kd value for Ca2+ binding to fura-2 of 224 nM. All measurements were performed at 37°C.
Imaging experiments.
Fura-2-loaded HEK 293 cells attached to glass coverslips were mounted in a perfusion chamber and placed on the stage of a Leica DMIRE2 inverted microscope. The cells were illuminated with light from a 175-W xenon lamp using a filter cube and dichroic mirror appropriate for fura-2. Excitation wavelength alternated between 340 and 380 nm using a Sutter filter wheel and appropriate filters. Epifluorescence was recorded using a SPOT-RT camera (Diagnostic Instruments, Sterling Heights, MI, USA) and images were acquired and analysed using SimplePCI imaging software (Compix Inc., Cranberry Township, PA, USA). Fura-2 calibration was performed using acquisition parameters identical to those used in each experiment, by recording the fluorescence from a solution containing fura-2 and either saturating or zero Ca2+ concentrations. All fura-2 imaging experiments were performed at room temperature (
22°C). For statistical purposes, [Ca2+]i responses from individual cells on each coverslip were averaged. In general, the number of cells imaged per coverslip was 1020. The average values from multiple coverslips were averaged and reported as mean ±S.E.M. with n equal to the number of coverslips.
Electrophysiological techniques
The giga-seal technique for current recording was utilized in the whole-cell mode. All experiments were performed on HEK 293 cells attached to circular glass coverslips which were transferred to a perfusable recording chamber on the stage of a Nikon inverted microscope immediately before use. Na+-containing Ringer solution was used as the extracellular solution and contained (mM): NaCl 160, KCl 4, CaCl2 2, MgCl2 1 and Hepes 10; pH 7.4. The pipette solution contained (mM): caesium aspartate 145, MgCl2 2, CaCl2 0.3, EGTA 10 and Hepes 10; pH 7.2 and pCa 8. In some experiments, Na+, or Na+ and K+ in the Ringer solution was isosmotically replaced by NMDG. Where indicated, [Ca2+] in the extracellular solution was varied from 0.02 to 20 mM by replacement of either Na+ or NMDG. Data were obtained using an Axopatch 200A amplifier (Pacer Scientific, Los Angeles, CA, USA) and sampled on-line using pCLAMP 8.0 software. The ground electrode was an AgAgCl wire connected to the bath via an agar bridge containing 150 mM NaCl. All recordings were made at room temperature. Electrode resistances ranged from 2 to 6 M
and whole-cell series resistances ranged from 4 to 20 M
. To generate currentvoltage (IV) relationships, voltage ramps from 120 to +120 mV over 200 ms were repetitively applied at 15-s intervals. Unless otherwise indicated, the holding potential between ramps was 50 mV and the currents were not leak-subtracted. All Figures show representative traces corrected for liquid junction potential. Where indicated, whole-cell membrane currents were also recorded using the perforated-patch technique as previously described (Korn & Horn, 1989). Pipettes were back-filled with pipette solution containing amphotericin-B. Following seal formation in cell-attached mode, the input resistance was continuously monitored. Experimental protocols were initiated when the access resistance reached a value of 40 M
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Current simulations and modelling
The effect of changes in extracellular Ca2+ on TRPC6 currents was simulated based on a single-site, two-barrier pore model (Hille, 2001). Specifically, an Excel spreadsheet was used to calculate IV relationships from the analytical solution to the model (eqn (15.10) of Hille, 2001; with equilibrium constants and maximal currents defined using eqns (15.8) and (15.9) and rate constants at 0 mV calculated as in eqn (15.11) with a pre-exponential factor of 6.11 x 1012). Parameters of the model (free energy levels for the barriers and binding site for Ca2+ and for monovalent cations, and the fractional electrical distance from the outside to the binding site (
)) were adjusted manually to fit the experimental data (i.e. to best approximate the shape of the IV plot and shifts in reversal potential). Parameter values are given in the legend to Fig. 5 (see also inset to Fig. 5B). The barriers were placed at the inner and outer edges of the membrane, so ion entry rates were voltage-independent. The rate constants for ion exit to the extracellular (ke) and intracellular (ki) sides were:
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| Results |
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TRPC6 channel activity was recorded using the patch-clamp technique in whole-cell recording mode. The pipette solution contained a high concentration of EGTA (10 mM) to buffer Ca2+ (pCa
8) and no ATP or GTP. The major cation in the pipette solution was Cs+ and the monovalent cations in the extracellular bath were Na+ and K+. Additionally, the bath solution contained 2 mM Ca2+. Under these conditions, exposure of HEK 293 cells stably expressing human TRPC6 to carbachol (CCh)
2 min after initiating whole-cell dialysis via the patch pipette, caused a time-dependent activation of membrane current (Fig. 1A) with distinctive inward and outward rectification properties as seen in the IV relationship (Fig. 1B). Current increased to a peak value within
1 min and subsequently declined slowly with time. As previously reported (Hofmann et al. 1999; Inoue et al. 2001; Estacion et al. 2004), application of OAG also increased TRPC6 current (Fig. 1C and D), but the response developed more slowly and the current density were less than that observed with CCh. Neither CCh- nor OAG-induced currents were observed in lacZ-transfected control HEK 293 cells. It is important to note that under these ionic conditions, outward current is primarily carried by Cs+, inward current is carried by Na+, K+ and Ca2+, and the current reversal potential is slightly negative (10 mV). Although the proportion of inward current carried by each ion has not been determined, previous experiments have estimated the permeability ratio of Na+: Cs+: K+: Ca2+ for the TRPC6 channel to be approximately 1: 0.8: 1: 5 (Hofmann et al. 1999; Inoue et al. 2001).
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Effect of RHC80267
Previous studies have shown that the DAG lipase inhibitor, RHC80267 (RHC), which is thought to increase both basal and receptor-stimulated DAG levels, increases [Ca2+]i and whole-cell currents in cells over-expressing TRPC6 channel (Hofmann et al. 1999; Inoue et al. 2001). We therefore examined the effect of RHC on membrane currents and [Ca2+]i in TRPC6-expressing cells. Addition of RHC to the bath solution produced a time- and concentration-dependent increase in TRPC6 current. The current activation rate and magnitude were similar to that observed with OAG (Fig. 2A and B). In contrast, addition of RHC to the extracellular solution (Ca2+-freehigh-K+ HBS) had no effect on basal [Ca2+]i and re-admission of Ca2+ produced a response that was not significantly different from basal influx (Fig. 2C and D). Thus it would appear that inhibition of DAG lipase does not stimulate Ca2+ influx in TRPC6-expressing cells. We next determined whether RHC could enhance CCh-induced responses. As seen in Fig. 2C and D, RHC decreased CCh-induced release of Ca2+ from internal stores and slightly reduced CCH-induced Ca2+ influx, when examined at either maximal (Fig. 2C) or submaximal (Fig. 2D) concentrations of CCh. Thus, as seen with OAG, RHC activated TRPC6 whole-cell currents, but did not increase Ca2+ influx as monitored by fura-2 fluorescence.
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U73122, an inhibitor of PLC, has previously been shown to block agonist-induced changes in [Ca2+]i in most cell types (Bleasdale et al. 1990; Smith et al. 1990; Thompson et al. 1991). Furthermore, previous studies have shown that activation of TRPC6 by receptor stimulation is also blocked by U73122 (Hofmann et al. 1999; Inoue et al. 2001). U73343, a less active analogue with little or no effect on PLC (Smith et al. 1990; Bleasdale et al. 1990), is commonly used as a negative control. As expected, U73122 blocked both the CCh-induced release of Ca2+ from internal stores in the TRPC6-expressing cells, and the subsequent Ca2+ influx observed upon re-admission of Ca2+ to the extracellular buffer (Fig. 3E). U73343 had no significant effect on either the release of Ca2+ from internal stores or on Ca2+ influx following re-admission of Ca2+. Much to our surprise, both U73122 and U73343 blocked the CCh-induced increase in TRPC6 currents (Fig. 3AD). These compounds were effective when added either before (Fig. 3C and D) or after CCh (Fig. 3A and B). Furthermore, the inhibition seen when either U73122 or U73343 was added after activation of TRPC6, was rapid and occurred without delay suggesting a direct, membrane-delimited effect on the TRPC6 channels. As both U73122 and U73343 block the channel, the effect must, at least in part, be independent of PLC. From these experiments it was again clear that the effects observed by whole-cell recording of TRPC6 current were different from those obtained using the fura-2 assay as an indicator of channel activity.
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As noted above, all of the fura-2 experiments presented thus far were performed in Ca2+-freehigh-K+ buffer to keep the membrane potential near zero. As previous studies have shown that store-operated and receptor-initiated Ca2+ entry is greatly attenuated by depolarization (Schilling, 1989; Schilling et al. 1989, 1992), it seemed possible that the failure to observe an increase in [Ca2+]i in response to OAG may reflect limited Ca2+ permeability of TRPC6 channels under depolarized conditions. To test this hypothesis, the fura-2 experiments were repeated in normal HBS. As seen in Fig. 4A, addition of OAG had no effect on basal [Ca2+]i under this condition and the subsequent Ca2+ influx component was essentially identical to basal Ca2+ influx recorded in the absence of OAG. However, when OAG was added to the cells in the continuous presence of extracellular Ca2+, a small, transient increase in [Ca2+]i of
30 nM was observed. A similar increase in [Ca2+]i was not seen in either wild-type HEK 293 cells or in lacZ-transfected control cells (data not shown). Thus the small increase in [Ca2+]i is related to TRPC6 expression. When the TRPC6-expressing cells were challenged with OAG in high-K+ buffer containing 2 mM Ca2+, the change in [Ca2+]i (
15 nM) was barely detectable (Fig. 4B). However, the OAG response was increased in high-K+ buffer by elevating the extracellular Ca2+ to 10 mM (increase [Ca2+]i of
50 nM). Overall, these results suggest that activation of TRPC6 current by OAG produces a small increase in [Ca2+]i in HEK 293 cells under normal ionic conditions, but the response is greatly reduced by holding the membrane potential near zero with high-K+ buffer; that is, depolarization inhibits Ca2+ influx via TRPC6 current.
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The rather modest increase in [Ca2+]i (<50 nM) induced by OAG under normal ionic conditions may reflect: (1) low permeability of TRPC6 for Ca2+ relative to Na+; (2) a TRPC6 current-induced depolarization; or (3) a combination of both effects. To evaluate the permeability of TRPC6 for Ca2+, we measured TRPC6 currents using extracellular solutions in which the Na+ and K+ were replaced by the large, impermeable cation, NMDG. Extracellular Ca2+ was then varied from 0.02 to 20 mM. IV relationships from a representative TRPC6-expressing HEK 293 cell under each ionic condition are shown in Fig. 5A and on an expanded scale in Fig. 5C. Currents were initially activated by OAG in normal Na+-containing Ringer solution (Fig. 5A and C). Under this condition, the currents reversed at 7 mV and exhibited the double rectification indicative of TRPC6. In NMDG-containing solution with 0.02 mM Ca2+, the inward current was substantially attenuated and the reversal potential was shifted to 82 mV. Although the currents shown in Fig. 5 were not leak-subtracted, the small inward current seen under this condition reflects, at least in part, a slight permeability of TRPC6 current for NMDG (see below), a characteristic that has been noted for another monovalent cation channel (Artigas & Gadsby, 2004). In NMDG-containing solution with 2 mM Ca2+, the reversal potential was 56 mV, and outward current was reduced relative to that observed in 0.02 mM Ca2+, but there was little change in inward current amplitude. In NMDG-containing solution with 20 mM Ca2+, the reversal potential was shifted to 24 mV and outward current was further reduced, again without change in inward current. Similar profiles were obtained when TRPC6 currents were measured in HEK 293 cells transiently expressing TRPC6 using the pIRES2-EGFP vector construct as previously described (Estacion et al. 2004). Thus, the results are not specific to this clonal cell line.
The insensitivity of inward current to elevations in extracellular [Ca2+], and the concomitant reduction in outward current suggests that Ca2+ is acting primarily as a channel blocker rather than a charge carrier. Consistent with this hypothesis, a single-site pore model reproduced the major characteristics of the data set (Fig. 5B and D). In this model, the binding site within the channel is placed at an electrical distance 85% across the membrane field. If the total electrical potential drop across the membrane thickness is linear, this would place the binding site close to the cytoplasmic surface. The model assumes that Na+, K+ and Cs+ have equal affinity for the binding site of the pore, but that the affinity of the site for Ca2+ is approximately two orders of magnitude greater than that for monovalent cations (inset, Fig. 5B; see Methods for additional details). Using these basic parameters, the model simulates all of the changes noted upon elevation of extracellular Ca2+ from 0.2 to 20 mM including: (1) the rightward shift in reversal potential; (2) the blockade of outward current; and (3) the insensitivity of the inward current. Additionally, the model simulates the dramatic increase in inward current observed in Na+-containing buffer. However, the model does not reproduce some features seen in the Na+ data set (compare trace d in Fig. 5A and C with trace d in Fig. 5B and D). Specifically, IV relationships generated by the model do not exhibit the slight hump in the current seen around 0 mV or the flattening of inward current seen at potentials more negative than 60 mV. Also, the model predicts that current in Na+-containing buffer reverses at approximately +5 mV, whereas the actual data traces in the presence of Na+ reverse at 10 mV. Overall, however, the IV relationships generated by the model are remarkably similar to those derived experimentally. We obtained another set of IV relationships using extracellular buffer in which only the Na+ was replaced by NMDG; that is, 4 mM K+ was present in the extracellular buffer (Fig. 1 of Supplemental material, available on-line). Using model parameters identical to those shown in Fig. 5, the model was again able to reproduce reversal potential shifts and account for the presence of K+. The mean(±S.E.M.) reversal potentials for several experiments are plotted in Fig. 6 for each Ca2+ concentration tested in either the presence or absence of K+. The lines shown in Fig. 6 represent the reversal potentials predicted by the model as a function of extracellular Ca2+ concentration and the symbols are the actual reversal potentials measured under each condition. Again there is excellent agreement between the experimental and the predicted values. It is important to note that calculation of the relative permeability of TRPC6 for Ca2+versus monovalent cations based on the experimentally determined reversal potentials in 2 or 20 mM Ca2+ yields values of 1.23 and 1.06, respectively. Thus, although the relative permeability of TRPC6 for Ca2+versus, in this case, Cs+ remains essentially constant at 1 as extracellular Ca2+ concentration is increased, the conductance is greatly reduced due to channel blockade.
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The results of the experiments presented thus far suggest that TRPC6 has a low inherent Ca2+ conductance and that depolarization further attenuates Ca2+ entry via TRPC6. However, it might be possible to observe Ca2+ entry via TRPC6 if the membrane potential is held sufficiently negative. To test this hypothesis, cells were loaded with fura-2 and then subjected to whole-cell voltage clamp using the perforated-patch technique as described in the Methods. Fluorescence images were acquired from the patched cell and from all unpatched cells in the field of view. A representative experiment is shown in Fig. 9. Addition of OAG (100 µM) in Na+-containing Ringer solution with 0.02 mM extracellular Ca2+ had no effect on [Ca2+]i but clearly caused an increase in whole-cell current with an IV relationship characteristic of TRPC6 current (Fig. 9, inset). At a holding potential of 50 mV, addition of 2 mM Ca2+ in the continuous presence of OAG caused an increase in [Ca2+]i that was substantially greater than that observed in the unpatched cells. Changing holding potential to +50 mV caused a decrease in [Ca2+]i, whereas changing the holding potential to 80 mV caused a further increase in [Ca2+]i. Thus, Ca2+ influx via TRPC6 appears to follow the electrochemical driving force imposed by the holding potential. This basic experiment was repeated four times in Na+-containing Ringer solution and the results from the patched cells held at 50 mV are shown in Fig. 10A and from the unpatched cells in Fig. 10C. Although the exact membrane potential of the unpatched cells is unknown, the reversal potential for whole-cell TRPC6 currents under this condition is approximately 7 mV (see Fig. 5). Thus, if TRPC6 current dominates the whole-cell conductance, the membrane potential of the unpatched cells should approach 7 mV. Upon increasing the extracellular Ca2+ concentration in the presence of OAG, [Ca2+]i increased in the patched cells to 131 ± 34 nM, whereas [Ca2+]i increased in the unpatched cells to only 41 ± 2 nM. In order to increase the driving force for Ca2+ entry in the unpatched cells, this experiment was repeated in NMDG-containing Ringer solution. Under this ionic condition, the reversal potential for the whole-cell TRPC6 current is approximately 56 mV (see Fig. 5). As seen in Fig. 10D, [Ca2+]i increased to 58 ± 5 nM in the unpatched cells, whereas in the patched cells held at 50 mV the value was 135 ± 28 nM. Thus, following activation of TRPC6 current by OAG, the membrane potential of the unpatched cells in the presence of NMDG is more negative than in the presence of Na+, but less negative than 50 mV. In order to obtain a better estimate of basal Ca2+ influx in these experiments, the cells were first perfused with Ca2+ in the absence of OAG and then re-perfused with Ca2+ in the presence of OAG (Fig. 11). In Na+-containing Ringer solution, the change in [Ca2+]i upon addition of Ca2+ to the bath was the same in the presence or absence of OAG. However, in NMDG-containing Ringer solution, an OAG-induced increase in [Ca2+]i was clearly seen. Taken together, the results suggest that although Ca2+ conductance of TRPC6 is low relative to monovalent cation conductance, an increase in [Ca2+]i can be observed if membrane potentials are held sufficiently negative.
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| Discussion |
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Although it is clear that activation of TRPC6 current by OAG can increase [Ca2+]i, the magnitude of the response was rather modest when compared to that observed following muscarinic receptor stimulation. This rather surprising result prompted us to examine the Ca2+ permeability of TRPC6 channels in greater detail using electrophysiological approaches. In the first protocol, TRPC6 channels were activated by OAG in buffer containing normal concentrations of Na+ and K+. The extracellular solution was then changed to one containing NMDG and various concentrations of Ca2+. If the channels were permeable to Ca2+, we anticipated rightward shifts in reversal potential and increases in inward current as Ca2+ was increased. Although the reversal potentials shifted as expected (i.e. to the right), inward current did not appreciably change and outward current was dramatically reduced as the Ca2+ concentration was increased in the extracellular buffer. In the second protocol, the extracellular solution was changed to the NMDG-containing solution with a fixed concentration of Ca2+ before activation of the channels with OAG. This allowed for a good estimate of leak current before activation of TRPC6 channels. Again, the results showed that inward currents were little affected by activation of TRPC6 under conditions that were expected to yield large Ca2+ currents. Together the results suggest that Ca2+ acts more as a TRPC6 channel blocker than a charge carrier. To estimate the contribution of Ca2+ to total inward current in the presence of normal Na+ and K+ levels, we simulated the experimental conditions using a single-site pore model in which the binding site of the pore was placed close to the cytoplasmic membrane surface and the affinity of the binding site for Ca2+ was approximately two orders of magnitude greater than that for monovalent cations. Although permeation in this channel is likely to be more complex, the simple single-site pore model reproduced the major features of the TRPC6 currents recorded under various ionic conditions and clearly supports the conclusion that TRPC6 channels have a limited Ca2+ permeability. Under physiological ionic conditions, the model predicts that TRPC6 channels are primarily monovalent cation channels. If activation is sustained, this could lead to a gain of Na+ and loss of K+ by the cell. This could explain our recent observation that TRPC6 channels physically associates with the Na+K+- ATPase/pump in kidney and brain, and in the plasmalemma of the TRPC6-expressing HEK 293 cell line used in the present study (Goel et al. 2005). As suggested for TRPC3 (Rosker et al. 2004), alteration in the Na+ gradient could also lead to Ca2+ entry via the Na+Ca2+ exchanger or may enhance Ca2+ signalling events in restricted subplasmalemmal compartments (Arnon et al. 2000). It is interesting that TRPC6 current-induced membrane depolarization and the subsequent activation of voltage-gated Ca2+ channels has been implicated in myogenic contraction of arterial smooth muscle cells (Welsh et al. 2002). In contrast, TRPC3 channels mediate depolarization and contraction of arterial smooth muscle in response to receptor stimulation (Reading et al. 2005). In a recent study using A7r5 smooth muscle cells, activation of endogenous TRPC6 channels by OAG causes an increase in [Ca2+]i that is blocked by nimodipine, suggesting that the rise in [Ca2+]i reflects a TRPC6-induced depolarization which in turn activates voltage-gated Ca2+ channels (Soboloff et al. 2005).
Taken together, the results of the present study suggest that TRPC6 channels play a dual role in signal transduction. In cells with high input resistance, the primary effect of TRPC6 activation will be depolarization, which limits Ca2+ entry via TRPC6 channels, but may facilitate a rapid burst of Ca2+ entry via voltage-gated Ca2+ channels if present. In cells with, for example, a large inward-rectifier or Ca2+-activated K+ channel current to hold the membrane potential negative, receptor-mediated activation of TRPC6 will directly serve as a sustained Ca2+ influx pathway. Thus, TRPC6 channels can perform a dual signalling role to either depolarize the cell and rapidly deliver Ca2+ or provide a more sustained change in [Ca2+]i depending on the particular needs of the cell and the complement of other channel types.
| Supplemental material |
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Supplementary Figure 1. Effect of extracellular Ca2+ on whole-cell currents in TRPC6-expressing HEK 293 cells: NMDG buffer with 4 mM K+
Supplementary Figure 2. Activation of TRPC6 in low- or high-Ba2+ buffer
Supplementary Figure 3. Model predictions for Ca2+ and monovalent current via TRPC6 channels
This material can also be found as part of the full-text HTML version available from http://www.blackwell-synergy.com
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