Abstract
The Ca2+ activated Cl− channel formed by transmembrane member 16A (TMEM16A) is broadly expressed and regulates diverse processes. In addition to Ca2+, TMEM16A channels require the acidic phospholipid phosphatidylinositol 4,5-bisphosphate (PI(4,5)P2) to open. Like other channels regulated by PI(4,5)P2, TMEM16A-conducted currents recorded in excised patches slowly decay overtime. Here we assessed how intracellular Ca2+ alters the rate of this current rundown, using the channels endogenously expressed in oocytes from the African clawed frog, Xenopus laevis. We found that in excised, inside-out patches, the concentration of applied Ca2+ alters the rate of rundown, with high Ca2+ concentrations speeding rundown by activating membrane associated phospholipase C (PLC). Together, these results clarify our understanding of how Ca2+ regulates both TMEM16A directly, and targets PLC to regulate the membrane PI(4,5)P2 content.
1 Introduction
The Ca2+ -activated Cl− channel, TMEM16A, is broadly expressed and regulates diverse physiologic processes ranging from mucosal secretion (Cabrita et al., 2021; Huang et al., 2012), transduction of sensory signals (Chen et al., 2021; Hernandez-Clavijo et al., 2021), smooth muscle tone (Bulley et al., 2012; Danielsson et al., 2020; Wang et al., 2021), and fertilization (Wozniak, Phelps, Tembo, Lee & Carlson, 2018; Wozniak, Tembo, Phelps, Lee & Carlson, 2018). Because TMEM16A channels regulate these important yet varied processes, it could be targeted by novel therapeutics as treatments for chronic diseases such as hypertension.
TMEM16A channels are homodimers, with each subunit comprising ten transmembrane domains, large intracellular N- and C-terminal domains, a membrane-embedded Ca2+ binding site, and an independently operating Cl− conducting pore (Al-Hosni, Ilkan, Agostinelli & Tammaro, 2022; Hawn, Akin, Hartzell, Greenwood & Leblanc, 2021; Shi et al., 2020). Five conserved amino acids in transmembrane domains 6-8 form the Ca2+ binding site, with each site capable of accommodating two Ca2+ ions (Brunner, Lim, Schenck, Duerst & Dutzler, 2014; Dang et al., 2017; Paulino, Kalienkova, Lam, Neldner & Dutzler, 2017). The channels gates differentially depending on whether one or two Ca2+ ions are bound (Peters et al., 2018). Moreover, other divalent cations in addition to Ca2+ are capable of opening TMEM16A channels (Yuan et al., 2013).
In addition to divalent cations, TMEM16A channels also require the acidic phospholipid phosphatidylinositol 4,5-bisphosphate (PI(4,5)P2) to open (De Jesus-Perez et al., 2017; Le, Jia, Chen & Yang, 2019; Ta, Acheson, Rorsman, Jongkind & Tammaro, 2017; Tembo et al., 2022; Tembo, Wozniak, Bainbridge & Carlson, 2019; Yu, Jiang, Cui, Tajkhorshid & Hartzell, 2019). A hallmark of channels potentiated by PI(4,5)P2 is that their currents rundown when recorded in excised patches (Suh & Hille, 2008). Indeed, TMEM16A conducted currents decay in excised patches, even in the presence of continuously applied intracellular Ca2+ (Tembo et al., 2022; Tembo, Wozniak, Bainbridge & Carlson, 2019). How PI(4,5)P2 potentiates TMEM16A conductance is unknown. One hypothesis states that PI(4,5)P2 stabilizes the open state of permeation pore of TMEM16A channels by binding to a separate regulatory module (Le, Jia, Chen & Yang, 2019), while another suggests that PI(4,5)P2 opens the pore by direct interaction with the outside of a pore-lining helix (Yu, Jiang, Cui, Tajkhorshid & Hartzell, 2019).
The full length TMEM16A isoform requires the phosphate at the 4’ position of PI(4,5)P2 in order to activate these channels (Ko & Suh, 2021; Tembo et al., 2022). Whereas the full-length channel is widely expressed in mammals, a TMEM16A splice variant expressed in the brain and skeletal muscle lacks four residues (EAVK) that reside in a linker connecting transmembrane domains 2 and 3; for this variant, the phosphate position does not matter for the phospholipid to potentiate channel activity (Ko & Suh, 2021; Le, Jia, Chen & Yang, 2019).
Notably, the lysine of the EAVK motif potentially interacts with the 4’ phosphate of PI(4,5)P2. Here we explored the relationship between intracellular Ca2+ on both the regulation of TMEM16A and the rate of current rundown in excised inside-out patches. Using electrophysiology recordings made on oocytes from the African clawed frog, Xenopus laevis, a cell that abundantly expresses TMEM16A channels, we found that millimolar Ca2+ application both activated TMEM16A conducted currents, but that these currents quickly decayed in excised patches. By contrast, the current rundown was significantly slower when the lower concentration of Ca2+ was applied at 500 µM, or when the channel was activated by 2 mM of other divalent cations including Ni2+ or Ba2+. Together these data reveal that 2 mM Ca2+ activates TMEM16A as well as phospholipase C (PLC) enzymes associated with the patch to speed PI(4,5)P2 depletion.
2 Methods
2.1 Animals
Animal procedures used were approved by the Animal Care and Use Committee at the University of Pittsburgh and are consistent with the accepted standards of humane animal care. Xenopus laevis adult, oocyte-positive females were obtained commercially (NASCO, Fort Atkinson, WI or Xenopus 1, Dexter MI) and housed at 18-20 °C with a 12/12-hour light/dark cycle.
2.2 Oocyte Collection
X. laevis females were anesthetized by immersion in 1.0 g/L tricaine pH 7.4 for 30 min before oocytes were collected. The ovarian sacs were surgically obtained and manually pulled apart using blunt forceps. Oocytes were treated with a 90-min incubation in 1 mg/ml collagenase in the ND96 solution, then repeatedly rinsed in OR2 to remove collagenase. Healthy oocytes were stored at 12-14 °C in pyruvate- and gentamycin-supplemented ND96 solution.
2.3 Solutions
Inside-out patch-clamp recordings were conducted in a HEPES-buffered saline solution made as follows (in mM): 130 NaCl and 3 HEPES, pH 7.2, and filtered using a sterile, 0.2 µm polystyrene filter (Tembo, Wozniak, Bainbridge & Carlson, 2019). The HEPES-buffered saline solution was supplemented with 0.2 mM EGTA for Ca2+-free recordings. For recordings made with intracellular Ca2+, the HEPES-buffered saline solution was supplemented with 2 mM, or 500 µM CaCl2 with indicated reagents. Total Ca2+ concentrations are reported throughout the manuscript. Free Ca2+ concentrations were calculated using Maxchelator (Bers, Patton & Nuccitelli, 2010) and are 1.8 mM Ca2+ (with 2 mM total Ca2+) and 300 µM Ca2+ (with 500 µM total Ca2+). The diC8-PI(4,5)P2 analog was added to the 2 mM Ca2+-containing HEPES-buffered saline solution and applied as indicated.
The oocyte wash solution, called Oocyte Ringers 2, and storage solution, ND96, were made as follows. Oocyte Ringers 2 (OR2) (in mM): 82.5 NaCl, 2.5 KCl, 1 MgCl2, and 5 mM HEPES, pH 7.2. ND96 (in mM): OR2 supplemented with 5 mM sodium pyruvate 100 mg/L gentamycin, pH 7.6, and 0.2 µm polystyrene filtered.
2.4 Patch-Clamp Recordings
Patch-clamp recordings were conducted on X. laevis oocytes following the manual removal of the vitelline membrane. TMEM16A current recordings were made in the inside-out configuration of the patch-clamp technique using an EPC-10 USB patch-clamp amplifier (HEKA Elektronic). The Patchmaster software (HEKA Elektronic) was used for data acquisition. Briefly, following the establishment of a gigaseal (greater than 1 GΩ), patches were excised in HEPES-buffered saline solution lacking both EGTA and added calcium. Following excision in this EGTA-free, HEPES-buffered saline, the patch resistances typically decreased to 20-200 MΩ, but returned to >1 GΩ with EGTA application. Data were collected at a rate of 10 kHz. Glass pipettes were pulled from borosilicate glass (OD 1.5 mm, ID 0.86 mm; Warner Instruments) and were fire polished using a Narshige microforge. Pipettes resistance ranged from 0.4-1.5 MΩ. All experiments were initiated within 10 s of patch excision. A VC-8 fast perfusion system (Warner Instruments) was used for solution application.
Patch-clamp data were analyzed with Excel (Microsoft) and IGOR Pro (Wavemetrics) with Patchers Power Tools. Currents were processed such that peak currents were normalized to 1. To calculate the rate of rundown, plots of normalized current at -60 mV versus time were fit with the single exponential equation:
where Y0, x, t, and Y(x) represent the initial current, time, rate of current rundown, and current at time x (Tembo, Wozniak, Bainbridge & Carlson, 2019). Remaining current at 100, 150, and 200 s was assessed by determining the proportion of maximum current at each of these time points (relative to the beginning of the experiment and included 10 s of EGTA-containing, no Ca2+ added solution application).
To calculate the current recovered following application of the synthetic PIP2 analog, diC8-PIP2, the fold change in current recovered was calculated by dividing the peak current after diC8-PIP2 addition by the baseline current. The peak current was defined as the highest current obtained after diC8-PIP2 addition. The baseline current was defined as the current observed at the point of diC8-PIP2 addition. The equation used was:
A fold recovery of 1 relates to unchanged current, and a recovery > 1 indicates that diC8-PIP2 application increased the current.
3 Results
3.1 TMEM16A currents decayed in excised patches and were recovered by PI(4,5)P2
Using X. laevis oocytes, we recorded Ca2+-activated TMEM16A-conducted currents using the excised-inside-out configuration of the patch clamp technique. Briefly, currents were recorded during 150 ms steps to -60 and +60 mV before and during application of 2 mM Ca2+. As we previously reported, application of 2 mM Ca2+ evoked robust TMEM16A-conducted currents immediately following patch excision (Tembo et al., 2022; Tembo, Wozniak, Bainbridge & Carlson, 2019). Figure 1A depicts currents recorded during steps to -60 and +60 mV at indicated time points (10-180 s) following 2 mM Ca2+ addition. Despite the continued application of intracellular Ca2+, these currents decayed over time (Figure 1). By fitting single exponential functions (Equation 1) to plots of normalized currents recorded during steps to -60 mV versus time (Figure 1B), we found that currents decayed with an average tau (τ) of 90.1 ± 8.3 s (N = 18).
Excised inside-out patches clamp recordings were obtained from macropatches made on X. laevis oocytes. (A) Example currents recording during 150-ms steps to -60 and +60 mV at the given times after patch excision. (B) Normalized plot of currents vs time after patch excision. 2 mM Ca2+ was applied at 10 s, as denoted by the blue bar, and currents were fitted with a single exponential (red line). (C) Box plot distribution of rate of current decay (τ) obtained from fits with single exponentials (N = 18). The box represents 25-75% of the data distribution, the whiskers indicate 0% to 100% of the data, and the center line represents the median. (D) Example plot of relative current recorded at -60 mV vs time of an inside-out patch before and during application of 100 µM diC8-PI(4,5)P2 (N = 6). The diC8-PI(4,5)P2 analog was applied following rundown, once currents reached a steady state. (E) Box plot distribution of the fold-recovery of current after 100 µM diC8-PIP2 application.
Current rundown is a characteristic of channels regulated by the phospholipid PI(4,5)P2 when recorded using the inside-out configuration of the patch-clamp technique (Suh & Hille, 2008). PI(4,5)P2 is depleted in excised patches; indeed, we found that application of 100 µM of the soluble dioctanoyl-phosphatidyl 4,5-bisphosphate (diC8-PI(4,5)P2) recovered TMEM16A currents. Figure 1D shows an example plot of TMEM16A-conducted currents recorded at -60 mV versus time, before and during application of 100 µM diC8-PI(4,5)P2. By calculating the change in current with diC8-PI(4,5)P2 application (Equation 2), we observed that diC8-PI(4,5)P2 recovered an average of 3.5 ± 0.7-fold current (N=6, Figure 1D&E).
3.2 TMEM16A current decay was slower with other divalent cations
To explore TMEM16A regulation by other divalent cations, we applied Ni2+ or Ba2+ to inside-out patches excised from X. laevis oocytes (Yuan et al., 2013) (Figure 2A). We found that when applied at 2 mM, both Ni2+ and Ba2+ activated TMEM16A channels (Figures 2B&C), however, the current decay differed substantially from that in 2 mM Ca2+. For example, plots of the relative current in the presence of 2 mM Ni2+ were not well fit with single exponentials (Figure 2B), thus, we assessed the proportion of maximum current at 100, 150, and 200 s (Table 1). When activated with 2 mM Ni2+, the TMEM16A-conducted current at 100 s only decayed to 0.80 ± 0.05 proportion of maximum current (N=10). By contrast, the currents decayed significantly more in 2 mM Ca2+, with only 0.45 ± 0.05 remaining at 100 s (N=18) (P<0.01, T-test, Figure 2B). Similarly, the TMEM16A current decayed more slowly in 2 mM Ba2+. Plots of relative current versus time were well fit with single exponentials and these Ba2+ activated TMEM16A conducted currents decayed with an averaged τ of 361.2 ± 121.0 s (N=5, Figure 2E), substantially slower than in 2 mM Ca2+ (90.1 ± 8.3 s, P<0.01, T-test). At 100 s following excision, 0.74 ± 0.08 current remained in Ba2+, which was not significantly different from the current remaining at 100 s in Ni2+ (Figure 2B). Together these data establish that Ba2+ and Ni2+ activate TMEM16A, but even at millimolar concentrations, the rate of rundown in the presence of these divalent cations is substantially slower than in 2 mM Ca2+. Evidently, all three divalent cations activate TMEM16A, but Ca2+ additionally speeds rundown.
The mean ± S.E.M. for of the normalized currents at the indicated time, taken from excised inside-out patches.
(A) Schematic of TMEM16A binding site for divalent cations Ca2+, Ni2+, or Ba2+. (B-C) Representative plot of normalized currents versus time before and during application of 2 mM Ni2+ (B) or 2 mM Ba2+ (C). Divalent cations were applied at 10 s. Plots of normalized current in Ba2+ vs time was fit with a single exponential (red line). (D) Box plot distribution of relative remaining current at three time points following patch excision: 100, 150, and 200 s (N=5-18). (E) Box plot distribution of rate of current decay (τ) obtained from fits with single exponentials (N = 5).
3.3 Applied Ca2+ concentration altered the rate of TMEM16A current rundown
We next quantified the rate of TMEM16A current rundown at the lower Ca2+ concentration of 500 µM. In eleven independent trials, 500 µM Ca2+ activated TMEM16A conducted currents and that these currents decayed over time (Figure 3A&B). By fitting single exponentials to plots of normalized current vs time, we observed slower rundown in 500 µM vs 2 mM Ca2+, with an averaged τ of 193.4 ± 28.4 s compared to 91.0 ± 8.3 s (P=<0.01, T-test) (Figure 3). These data indicate that the applied concentration of Ca2+ alters the rate of rundown and suggest that millimolar Ca2+ targets TMEM16A channels while also regulating the rate of PIP2 depletion.
(A) Representative plot of normalized current recorded at -60 mV vs time of TMEM16A conducted currents in the presence of 500 µM Ca2+ denoted by the red bar. Plot was fit with a single exponential (red line) (B) Box plot distribution of the rundown rate (τ) during application of either 2 mM or 500 µM Ca2+ (N = 11-18).
3.4 ATP application partially rescued rundown in 2 mM Ca2+
We reasoned that in addition to activating TMEM16A, 2 mM Ca2+ could target other membrane associated proteins to speed PI(4,5)P2 depletion in excised patches. Because the rundown of TMEM16A currents in excised patches is due to PI(4,5)P2 depletion (Tembo et al., 2022; Tembo, Wozniak, Bainbridge & Carlson, 2019), we explored a possible role for Ca2+ in the regulation of PI(4,5)P2 homeostasis in excised patches. In living cells, phosphatases and kinases work together to maintain membrane PI(4,5)P2 content; in excised patches, membrane-anchored kinases lack access to the ATP required to fuel phosphorylation and regeneration of PI(4,5)P2 (Figure 4A) (Hilgemann & Ball, 1996; Suh & Hille, 2008). Continued and unopposed activity of phosphatases in excised patches therefore leads to the net dephosphorylation of PIP2 (Figure 4A). We have previously reported that application of 2 mM Ca2+ with ATP slowed rundown of TMEM16A conducted current recorded from excised inside out patches (Tembo, Wozniak, Bainbridge & Carlson, 2019). Here we compared how ATP application altered rundown in patches treated with 2 mM or 500 µM Ca2+.
(A) Schematic illustrating the roles of phosphatases and kinases in maintaining phosphoinositide homeostasis in whole cells (left) vs excised patches (right). (B) Plot of normalized currents vs time during application of 2 mM Ca2+ with 1.5 mM Mg-ATP recorded from inside-out patches and fit with a single exponential (red line). (C) Box plot distribution of rate of current decay (τ) as reported by single exponentials, from patches treated with 2 mM Ca2+ with ATP or without ATP. (D) Example plot of TMEM16A conducted current before and during application of 1.5 mM Mg-ATP with 500 µM Ca2+ represented by the orange bar. (E) Box plot distribution of the proportion current at 100s in patches treated with indicated concentrations of Ca2+ (in mM) and with or without 1.5 mM Mg-ATP, as indicated (N=7-18 patches).
By fitting plots of the normalized current vs time with single exponentials, we observed that ATP application substantially slowed the τ of rundown from an average of 91.0 ± 8.3 s (N=18) in 2 mM Ca2+ alone, to 239.8 ± 13.6 s with ATP (N=7) (P<0.01, Figure 4C&D). A slowing of current decay was also observed in the proportion of maximum current at 100 s, from 0.45 ± 0.05 in 2 mM Ca2+ to 0.70 ± 0.05 with ATP (N=7-18). ATP also slowed current decay in 500 µM Ca2+; however, plots of current decay with 500 µM Ca2+ vs time were not well fit by single exponentials (Figure 4D). Again, we assayed for changes in current decay by quantifying the proportion of maximum current at 100 s, we observed a change from 0.67 ± 0.06 to 0.83 ± 0.03 (P=0.03, T-test, N=8-11). ATP slowed rundown with both 500 µM and 2 mM Ca2+, but rundown was still quicker in 2 mM Ca2+ with ATP. Together, these data suggest that millimolar Ca2+ speeds PI(4,5)P2 depletion by potentiating a process not recovered by ATP.
3.5 Inhibiting PLC slowed rundown of TMEM16A-conducted currents
We speculated that Ca2+ may activate PLC to thereby increase PIP2 cleavage for the generation of IP3. Importantly, the PI(4,5)P2 lost due to PLC cleavage cannot be recovered with ATP application. We verified that PLCs are present in the X. laevis eggs using a proteome dataset from fertilization-competent eggs (Wuhr et al., 2014) and queried for all proteins encoded by known PLC genes. Notably, this dataset was acquired on fertilization-competent eggs, but we are using immature stave VI oocytes for our experiments. Therefore, we also examined an RNA-sequencing dataset acquired from different stages of development of X. laevis oocytes and eggs (Session et al., 2016). We reasoned that if a protein is present in the stage VI oocyte, RNA should be present in the developing oocyte. Indeed, two PLC isoforms fit these criteria: PLCγ1 (encoded by the PLCG1 gene) and PLCβ3 (encoded the PLCB3 gene) (Supplemental figure 1).
We next determined whether inhibition of PLCs slowed rundown of TMEM16A currents. To do so, we used two PLC inhibitors: U73122 (Jin, Lo, Loh & Thayer, 1994) and PMSF (Walenga, Vanderhoek & Feinstein, 1980). We found that TMEM16A conducted currents ran down more slowly in the presence of 1 µM U73122 compared to application of 2 mM Ca2+ alone. In 1 µM U73122, the proportion of remaining current at 100 s was 0.71 ± 0.08 (N=5), compared to 0.45 ± 0.05 (N=18) in Ca2+ alone (P= 0.02, T-test). 2 mM PMSF similarly slowed rundown, with 0.78 ± 0.05 (N=6) proportion of remaining current at 100 s. Together, these data demonstrate that in addition to activating the channel, 2 mM Ca2+ also activates PLC to speed the rundown of TMEM16A conducted current.
Discussion & Conclusions
Here we demonstrate that in addition to activating TMEM16A channels, intracellular Ca2+ speeds current rundown by turning on membrane tethered PLCs in excised inside out patches. TMEM16A channels require both intracellular Ca2+ and PIP2 to open and conduct Cl− currents (De Jesus-Perez et al., 2017; Le, Jia, Chen & Yang, 2019; Ta, Acheson, Rorsman, Jongkind & Tammaro, 2017; Tembo et al., 2022; Tembo, Wozniak, Bainbridge & Carlson, 2019; Yu, Jiang, Cui, Tajkhorshid & Hartzell, 2019). Like other channels regulated by PIP2, TMEM16A-conducted currents decay when recorded in the inside-out configuration of the patch clamp technique (Figure 1), even in the continued presence of Ca2+ (De Jesus-Perez et al., 2017; Tembo, Wozniak, Bainbridge & Carlson, 2019). We previously demonstrated that this current decay from excised patches can be sped by scavenging membrane PIP2, slowed by inhibiting the membrane associated phosphatases or refueling the kinases (Tembo, Wozniak, Bainbridge & Carlson, 2019).
Our finding that TMEM16A-conducted currents decayed more slowly when the channels were activated by the other divalent cations Ni2+ or Ba2+ (Figure 2) provided our first hint that Ca2+ may target the channel and independently regulate PIP2 present in excised patches. This hypothesis was further supported by the demonstration that TMEM16A conducted current rundown was slower with application of a lower concentration of Ca2+, 500 µM (Figure 3).
Furthermore, ATP application slowed rundown in both 2 mM and 500 µM Ca2+, however, rundown was slower and more current remained when ATP was applied with 500 µM Ca2+ compared to 2 mM, indicating that another process contributed to rundown in higher Ca2+ (Figure 4).
PLCs can be activated directly by Ca2+ (Hwang, Oh, Shin, Kim, Ryu & Suh, 2005; Ryu, Suh, Cho, Lee & Rhee, 1987), we therefore speculated that Ca2+ may activate a membrane-associated PLC to speed rundown. Here we used bioinformatics to verify that indeed PLCs are present in the developing gamete: PLCγ1 and PLCβ3 (Supplemental Figure 1). To more directly test whether PLC depletion of PIP2 speeds TMEM16A current decay in excised patches, we quantified the rate of rundown with application of two different PLC inhibitors: U73122 and PMSF. Both inhibitors significantly slowed rundown in 2 mM Ca2+, thereby suggesting that PLC activity indeed contributed to loss of TMEM16A conducted current.
Here we report plots of current decay versus time using varying conditions, some of which were fit by single exponentials and others which were not. For example, plots of rundown in 2 mM Ni2+ were not well fit by single exponentials whereas plots in 2 mM Ba2+ were. The mechanism underlying this variability is not yet clear. Theoretically, fitting plots of relative current versus time with a single exponential would indicate that a single process gives rise to rundown. However, our data suggest that at least in 2 mM Ca2+, activity of both phosphatase and PLC deplete patch PI(4,5)P2. Further work is needed to understand this variability.
Fertilization activates TMEM16A channels in X. laevis eggs to allow Cl− to leave the cytoplasm and depolarize the membrane (Wozniak, Phelps, Tembo, Lee & Carlson, 2018). This fertilization-signaled depolarization rise rapidly stops multiple sperm from entering an already fertilized egg, a process known as the fast block to polyspermy (Wozniak & Carlson, 2020).
Indeed, sperm can bind but will not enter depolarized eggs (Jaffe, 1976). Fertilization activates TMEM16A in X. laevis by a pathway requiring PLC activation and IP3 signaled Ca2+ release from the ER (Wozniak, Tembo, Phelps, Lee & Carlson, 2018) and occurs within seconds of fertilization. Fertilization also initiates a slower block to polyspermy that also require PLC and Ca2+ release from the ER to signal exocytosis of cortical granules from the egg minutes after sperm entry. The Ca2+ wave that initiates cortical granule exocytosis starts at the site of sperm entry and takes minutes to traverse the egg (Busa & Nuccitelli, 1985; Fontanilla & Nuccitelli, 1998). Whether the same process activates the PLC needed for the fast and slow polyspermy blocks in X. laevis eggs has not yet been determined.
A prominent role for Ca2+ in the regulation of PIP2 and TMEM16A is intriguing because both Ca2+ and PIP2 are required for the channel to open, yet elevated Ca2+ could signal deactivation of the channel even when Ca2+ is bound to the channel. Although here we report that millimolar Ca2+ concentrations were required to activate PLC and speed rundown, X. laevis eggs experience prolonged periods of high intracellular Ca2+ shortly after fertilization (Wagner et al., 2004). It is possible that this Ca2+ mediated PLC activation could give rise to the regenerative Ca2+ wave that initiates X. laevis cortical granule exocytosis (Fall, Wagner, Loew & Nuccitelli, 2004; Wagner et al., 2004). For example, fertilization could produce an acute and localized bolus of Ca2+ in X. laevis eggs. This Ca2+ could then activate nearby PLCs, which would then cleave PIP2 to generate IP3 and signal the release of more Ca2+. This mechanism would give rise to a self-sustaining and regenerating Ca2+ wave (Lechleiter, Girard, Peralta & Clapham, 1991; Lechleiter & Clapham, 1992; Marchant, Callamaras & Parker, 1999).
Conflict of Interest
The authors declare no conflicts of interest in the contents of this manuscript.
Representative plots of normalized current recorded at -60 mV vs time of TMEM16A conducted currents in the presence of 2 mM Ca2+ with 1 µM U73122 (A) or 2 mM PMSF (C). (B) Box plot distribution of rate of current decay (τ) as reported by single exponentials, from patches treated with 2 mM Ca2+ alone (control) or with U73122 or PMSF, as indicated (N=5-18).
In excised patches, PI(4,5)P2 levels are regulated by membrane anchored enzymes including phosphatases, kinases, and PLCs.
Acknowledgments
We thank G.V. Hammond for helpful discussions and advice and D. Summerville for excellent technical assistance. This work was supported by an American Heart Association Predoctoral Fellowship 18PRE33960391 to M.T. and National Institute for Health grant 1R01GM125638 to A.E.C.