0022-3565/07/3213-1075–1084$20.00 THE JOURNAL OF PHARMACOLOGY AND EXPERIMENTAL THERAPEUTICS Copyright © 2007 by The American Society for Pharmacology and Experimental Therapeutics JPET 321:1075–1084, 2007 Vol. 321, No. 3 118786/3206608 Printed in U.S.A. Stimulation of Ca2⫹-Gated Cl⫺ Currents by the CalciumDependent K⫹ Channel Modulators NS1619 [1,3-Dihydro-1-[2hydroxy-5-(trifluoromethyl)phenyl]-5-(trifluoromethyl)-2Hbenzimidazol-2-one] and Isopimaric Acid Sohag N. Saleh, Jeff E. Angermann, William R. Sones, Normand Leblanc, and Iain A. Greenwood Received December 19, 2006; accepted March 5, 2007 ABSTRACT Because chloride (Cl⫺) channel blockers such as niflumic acid enhance large-conductance Ca2⫹-activated potassium channels (BKCa), the aim of this study was to determine whether there is a reciprocal modification of Ca2⫹-activated chloride Cl⫺ currents (IClCa) by two selective activators of BKCa. Single smooth muscle cells were isolated by enzymatic digestion from murine portal vein and rabbit pulmonary artery. The BKCa activators NS1619 [1,3-dihydro-1-[2-hydroxy-5-(trifluoromethyl)phenyl]-5-(trifluoromethyl)-2H-benzimidazol-2-one] and isopimaric acid (IpA) augmented macroscopic IClCa elicited by pipette solutions containing [Ca2⫹]i ⬎ 100 nM without any alteration in current kinetics. Enhanced currents recorded in the presence of NS1619 or IpA reversed at the theoretical Cl⫺ equilibrium potential, which was shifted by approximately ⫺40 mV upon replacement of the external anion with the more permeable thiocyanate anion. NS1619 increased the sensitivity of calcium-activated chloride channel (ClCa) to Ca2⫹ (⬃100 nM at ⫹60 mV) and induced a leftward shift in their voltage dependence (⬃80 mV with 1 M Ca2⫹). Single-channel experiments revealed that NS1619 increased the number of open channels times the open probability of small-conductance (1.8 –3.1 pS) ClCa without any alteration in their unitary amplitude or number of observable unitary levels of activity. These data, in addition to the established stimulatory effects of niflumic acid on BKCa, show that there is similarity in the pharmacology of calciumactivated chloride and potassium channels. Although nonspecific interactions are possible, one alternative hypothesis is that the channel underlying vascular IClCa shares some structural similarity to the BKCa or that the latter K⫹ channel physically interacts with ClCa. S.N.S. was funded by a Glaxo Smith Kline-Biotechnology and Biological Sciences Research Council award. This work was supported by the National Institutes of Health (Grant HL 1 R01 HL075477-01 to N.L.), by the British Heart Foundation (Grant PG/05/038 to I.A.G.), and by The Wellcome Trust (grant to I.A.G.). This publication was also made possible by Grant NCRR 5P20 RR15581 (to N.L.) from the National Center for Research Resources, a component of the National Institutes of Health supporting a Center of Biomedical Research Excellence at the University of Nevada School of Medicine (Reno, NV). Its contents are solely the responsibility of the authors and do not necessarily represent the official views of National Center for Research Resources or National Institutes of Health. Article, publication date, and citation information can be found at http://jpet.aspetjournals.org. doi:10.1124/jpet.106.118786. Ca2⫹-activated chloride Cl⫺ currents (IClCa) are present in a wide variety of cell types, including endothelial, secretory, and smooth muscle cells (Hartzell et al., 2005; Leblanc et al., 2005). In vascular smooth muscle cells, IClCa have a number of distinctive characteristics, including an activation threshold for [Ca2⫹] of about 200 nM, voltage-dependent kinetics, a lyotropic anion permeability profile, and small unitary conductance (Hartzell et al., 2005; Leblanc et al., 2005). In contrast to the extensive electrophysiological studies on IClCa, the molecular identity of the gene(s) encoding for the channel generating IClCa is still unknown, and attempts to ABBREVIATIONS: IClCa, calcium-activated chloride current; NFA, niflumic acid; CCB, chloride channel blocker; BKCa, calcium-activated potassium channel; NS1619, 1,3-dihydro-1-[2-hydroxy-5-(trifluoromethyl)phenyl]-5-(trifluoromethyl)-2H-benzimidazol-2-one; IpA, isopimaric acid; PV, portal vein; I-V, current-voltage; Iinitial, current measured at the beginning of a voltage-clamp test pulse immediately following the capacitative current; Ilate, current measured at the end of a voltage-clamp test pulse; GClCa, conductance of the calcium-activated chloride channel; Erev, reversal potential of the current; NP0, number of open channels times the open probability; Itail, current measured 20 ms after repolarization from a voltage-clamp step used to elicit time-dependent calcium-activated chloride current; IBKCa, calcium-activated potassium current; ClCa, calcium-activated chloride channel. 1075 Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 Ion Channels and Cell Signaling Research Centre, Division of Basic Medical Sciences, St. George’s, University of London, London, United Kingdom (S.N.S., W.R.S., I.G.); and Department of Pharmacology, Center of Biomedical Research Excellence, University of Nevada School of Medicine, Reno, Nevada (J.E.A., N.L.) 1076 Saleh et al. tural similarity with the BKCa or that the latter channel physically interacts with Ca2⫹-activated Cl⫺ channels. Materials and Methods Cell Dissociation and Solutions. IClCa were recorded using the whole-cell voltage-clamp technique from single smooth muscle cells isolated from murine PV or rabbit pulmonary artery. BALB/c mice (6 – 8 weeks) were sacrificed by cervical dislocation in accordance with schedule 1 of the United Kingdom Animals Act (1986). After an incision of the abdomen, the PV was removed and immediately placed in chilled physiological salt solution composed of 125 mM NaCl, 5.4 mM KCl, 15.4 mM NaHCO3, 0.33 mM Na2HPO4, 0.34 mM KH2PO4, 10 mM glucose, 11 mM HEPES, and 1 mM CaCl2 (pH was adjusted to 7.2 with NaOH). The PV was freed of fat and connective tissue and then cut into longitudinal strips and individual smooth muscle myocytes isolated using the same procedure described by Saleh and Greenwood (2005). Rabbit pulmonary artery myocytes were prepared as described fully by Greenwood et al. (2001, 2004). A small aliquot of smooth muscle cells stored in 0.1 to 0.01 mM CaCl2 physiological salt solution was placed in a glass chamber on the stage of a Zeiss Axiovert (Carl Zeiss MicroImaging GmbH, Jena, Germany) or Nikon Diaphot TMD inverted microscope (Nikon, Tokyo, Japan). After allowing 15 to 20 min for adhesion, the cells were superfused at a rate of 5 ml/min, with an external solution composed of 126 mM NaCl, 11 mM glucose, 10 mM HEPES, 10 mM TEA-Cl, 1.2 mM MgCl2, and 1.5 mM CaCl2 (pH was adjusted to 7.2 with NaOH). Individual SMCs were identified by their spindle-shaped appearance and ability to contract. Electrophysiology and Statistical Analysis. Macroscopic IClCa was recorded using the whole-cell configuration of the patch-clamp technique with either an EPC-8 HEKA (Lambrecht/Pfalz, Germany) or an Axopatch-1D (Molecular Devices, Sunnyvale, CA) patch-clamp amplifier. Voltage-clamp protocols were computer-driven using a D/A and A/D acquisition system (DigidataA 1322 board; Molecular Devices) and pClamp 8.2 or 9.0 software (Molecular Devices). Patch pipettes were manufactured from borosilicate glass and fire polished, giving pipettes with resistance of between 2 and 5 M⍀. IClCa was evoked using pipette solutions containing a known concentration of free [Ca2⫹]. With this technique, pipette solutions containing free [Ca2⫹] higher than the activation threshold (⬃180 nM) persistently stimulate the Cl⫺ channel resulting in a sustained Cl⫺ current without any reliance upon Ca2⫹ influx or release from internal stores as described in a number of previous publications (Greenwood et al., 2001, 2004; Britton et al., 2002; Piper et al., 2002; Angermann et al., 2006). The intracellular solution contained 106 mM CsCl, 20 mM TEA, 3 mM Na2ATP, 0.2 mM GTP䡠Na, 10 mM HEPES-CsOH, pH 7.2, 10 mM BAPTA, and 0.42 mM MgCl2 (0.42) and an appropriate concentration of CaCl2 (0.84 – 8.4 mM) to make up free Ca2⫹ concentrations of 0.02, 0.1, 0.25, 0.5, and 1 M as calculated by EqCal (Biosoft, Ferguson, MO). Under these conditions, any contribution from K⫹ channels should be negligible, and the membrane conductance is dominated by Cl⫺ channel activity. A number of different voltage protocols were employed in the present study. A single test step every 15 s from ⫺60 to ⫹90 mV for 750 ms followed by repolarization to ⫺80 mV for 500 ms was used to ascertain when IClCa had stabilized and to investigate the time course of different drug effects (see Fig. 2B). Once IClCa had stabilized, a control current-voltage (I-V) relationship was constructed by depolarizing the myocyte from ⫺60 mV to a range of voltages from ⫺100 to ⫹100 mV for 1.5 s. I-V relationships were constructed at two different time points, namely immediately after the onset of the test step (Iinitial) and immediately before termination of the test pulse (Ilate; for example, see Fig. 1B). In Figs. 4 and 5, the chord conductance of IClCa in nanosiemens (GClCa) was calculated using the following formulation (eq. 1): G ClCa共V兲 ⫽ Ilate/共V ⫺ Erev) (1) Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 identify the proteins underlying IClCa have been hampered by the lack of high-affinity pharmacological probes. A number of structurally disparate agents block IClCa in smooth muscle cells (Large and Wang, 1996), with the most potent being niflumic acid (NFA), which inhibits spontaneously occurring transient Cl⫺ currents with an IC50 of approximately 2 M (Large and Wang, 1996). However, the inhibitory efficacy of NFA and other putative Cl⫺ channel blockers (CCBs) such as anthracene-9-carboxylic acid is inversely proportional to the degree of Cl⫺ channel stimulation. Consequently, the IC50 for NFA block of longer lasting IClCa evoked as a consequence of promoting Ca2⫹ influx through voltage-dependent Ca2⫹ channels is about 15 M (Leblanc et al., 2005; Saleh and Greenwood, 2005). As a corollary to these findings, fully activated or sustained IClCa evoked by pipette solutions of known free [Ca2⫹] are not inhibited markedly by NFA at concentrations [Ledoux et al., 2005; IC50 ⫽ 159 M at ⫹60 mV with 500 nM intracellular Ca2⫹ concentration ([Ca2⫹]i)] far higher than required to abolish spontaneously occurring IClCa. Paradoxically, niflumic acid and similar agents actually stimulate sustained IClCa, which is more obvious upon washout of the agent where IClCa increases by about 200 to 300% in rabbit pulmonary or coronary artery myocytes (Piper et al., 2002; Piper and Greenwood, 2003; Ledoux et al., 2005). These observations led to the suggestion that the Cl⫺ channel protein contained at least two binding sites for NFA: a low-affinity inhibitory site and a high-affinity stimulatory site that becomes more prominent with greater stimulation of the channel (Ledoux et al., 2005). In addition to its effect on IClCa NFA also stimulates largeconductance, Ca2⫹-dependent K⫹ channels (BKCa) in lipid bilayers (e.g., Ottolia and Toro, 1994) and vascular smooth muscle cells (Greenwood and Large, 1995). A number of experiments in smooth muscle cells led to the postulate that NFA and structurally similar agents, such as flufenamic acid and mefenamic acid, acted as partial agonists at a calcium binding domain on the BKCa complex (Greenwood and Large, 1995). Subsequent to this work, Toma et al. (1996) showed that three other chemically distinct CCBs, anthracene-9-carboxylic acid, ethacrynic acid, and indanyloxyacetic acid, also activated BKCa in vascular smooth muscle cells at concentrations higher than required to block IClCa. Consequently, there seems to be similarity in the pharmacology of BKCa and the channel underlying IClCa, especially in vascular myocytes. The aim of the present study was to explore this possibility further by studying how the well characterized BKCa modulators NS1619 and isopimaric acid (IpA) affect native IClCa in vascular smooth muscle cells (for chemical structures, see Olesen et al., 1994; Imaizumi et al., 2002). Because the structure of the BKCa is well characterized, the development of these pharmacological investigations may give some clues about structural features of the Cl⫺ channel to be deciphered. Specifically, we investigated whether NS1619 and IpA, which stimulate BKCa by a direct interaction with the poreforming subunit encoded by Slo1 (Joiner et al., 1998; Imaizumi et al., 2002), affect IClCa elicited by fixed elevated levels of [Ca2⫹]i in murine portal vein (PV) and rabbit pulmonary artery smooth muscle cells. Our data revealed that the BKCa activators augmented IClCa, and this effect was reversed by subsequent application NFA. These results suggest that the channel underlying IClCa may bear some struc- Modulation of Calcium-Activated Chloride Channels 1077 where Ilate is the current measured at the end of the pulse (see Fig. 1B), V is the potential in mV that evoked Ilate, and Erev is the reversal potential of Ilate determined by analysis of the I-V relationship. Finally, a two-step protocol was employed to determine the reversal potential of the currents evoked in the absence and presence of different agents. Cells were initially depolarized from ⫺60 to ⫹90 mV to fully activate the channels and then stepped to different test potentials between ⫺100 and ⫹40 mV at 20-s intervals (see Fig. 2B). For single-channel recordings of IClCa in the inside-out configuration, the bath solution contained 108 mM CsOH, 108 mM aspartic acid, 18 mM CsCl, 10 mM glucose, 11 mM HEPES, 1.2 mM MgCl2, 1 mM Na2ATP, 0.2 mM Na2GTP, and CaCl2 (0.1 mM for 14 nM free Ca2⫹ and 1.5 mM for 500 nM free Ca2⫹, calculated using EqCal software; pH was adjusted to 7.2 using Trizma base). The pipette solution facing the external surface of the membrane contained 126 mM N-methyl-D-glucamine Cl⫺ (prepared by equimolar addition of N-methyl-D-glucamine and HCl), 1 mM glucose, 10 mM HEPES, 0.005 mM nicardipine, 10 mM TEA-Cl, 10 mM 4-aminopyridine, 0.0001 mM iberiotoxin, 1.2 mM MgCl2, and 5 mM CaCl2 (pH adjusted to 7.2 with N-methyl-D-glucamine or HCl as appropriate). Unitary currents produced by the opening of single Ca2⫹-activated Cl⫺ channels were recorded with a EPC-8 HEKA patch-clamp amplifier at room temperature using the inside-out patch configuration of the patch-clamp technique. For these experiments, the micropipettes were fire-polished more heavily than those used for whole-cell recording experiments, yielding a pipette resistance lying between 10 and 15 M⍀. To reduce line noise, the recording chamber was superfused with solutions delivered through two 20-ml syringes, one filled with external solution and the other used to drain the chamber, in a “push and pull” technique. The external solution could thus be exchanged twice within 30 s. When recording single-channel currents, the holding potential was set at ⫹80 mV, and to evaluate I-V characteristics of unitary channel currents, the membrane potential was manually changed between ⫺80 and ⫹80 mV by turning the holding potential knob on the patch-clamp amplifier. Single-channel currents were initially recorded onto digital audio tape using a Fig. 2. NS1619 enhances a current whose properties are consistent with those of IClCa in murine portal vein myocytes. A, three families of current traces recorded in control, after a 3-min exposure to 30 M NS1619, and 5 min following washout of the drug. Currents were elicited by 750-ms voltageclamp steps ranging from ⫺100 to ⫹120 mV (20-mV increments) from a holding potential of ⫺50 mV. Bi, IClCa evoked by the double-pulse voltageclamp protocol shown below the two families of IClCa traces recorded in the absence (filled square) and presence (open circle) of 30 M NS1619. Bii, graph, mean data from five similar experiments to Bi. The plots were generated by measuring the amplitude of Itail 20 ms after stepping to the test potential and plotted against the corresponding voltage step. The current enhanced by NS1619 (open circles) reversed at the same voltage (⬃0 mV) as IClCa recorded in the absence of drug (filled squares). Scalars, 200 pA and 500 ms. A and B, cells were dialyzed with 250 nM free [Ca2⫹]. Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 Fig. 1. Characteristics of sustained IClCa evoked in murine portal vein myocytes. A, families of currents recorded at potentials between ⫺100 and ⫹120 mV following activation of IClCa by pipette solutions of different [Ca2⫹] (as shown). B, example of the effect of a test step to ⫹90 mV on the sustained IClCa evoked by 500 nM free [Ca2⫹]. B highlights the different parameters measured during the study. Protocol shown as an insert. Immediately after membrane depolarization, there was an instantaneous outward current (Iinitial) that was followed by a slowly developing outward relaxation resulting in more outward current at the end of the test step (Ilate). Upon repolarization to ⫺80 mV, an exponentially declining inward current (Itail) was recorded. Dashed line, zero current level. C, mean late current amplitude at five different test potentials plotted against activator [Ca2⫹] and fitted by a standard logistic equation. Data are the mean of ⬎four cells. 1078 Saleh et al. Bio-Logic DRA-200 digital tape recorder (Bio-Logic SAS, Claix, France) at a bandwidth of 5 kHz (⫺3 db, low-pass four-pole Bessel filter, HEKA EPC-8 patch-clamp amplifier) and a sampling rate of 48 kHz. For off-line analysis, single-channel records were filtered at 100 Hz (⫺3 db, low-pass eight-pole Bessel filter, Frequency Devices, model LP02; Scensys Ltd,. Aylesbury, UK) and acquired using a Digidata 1322A and pCLAMP 9.0 software (Molecular Devices) at a sampling rate of 1 kHz. Data were captured with a Pentium III personal computer (Research Machines, Abingdon, Oxfordshire, UK). Single-channel current amplitudes were calculated from idealized traces of at least 60 s in duration using the 50% threshold method with events lasting for ⬍6.664 ms [2 times rise time for a 100 Hz (⫺3 db) low pass filter] being excluded from analysis. In Fig. 7, outward channel currents are shown as upward deflections. NP0 was calculated using eq. 2: NP0 ⫽ 冘 (Onn) T (2) Results Characterization of Ca2ⴙ-Activated Clⴚ Currents in Mouse Portal Vein Myocytes. Although sustained IClCa evoked by pipette solutions of known free [Ca2⫹] have been characterized extensively in rabbit pulmonary artery, coronary artery, and portal vein (Greenwood et al., 2001, 2004; Ledoux et al., 2003, 2005; Angermann et al., 2006), our previous study in mouse portal vein (Britton et al., 2002) only looked at a limited range of [Ca2⫹]. Figure 1A shows typical families of IClCa recorded from different mouse PV smooth muscle cells dialyzed with a pipette solution containing 20, 100, 250, 500, or 1000 nM Ca2⫹. These experiments clearly show that as the intracellular Ca2⫹ was raised, the current at a holding potential of ⫺60 mV increased consistent with the tonic activation of Cl⫺ channels. Depolarization generated distinctive voltage-dependent kinetics that are of IClCa elicited by this technique (Arreola et al., 1996; Nilius et al., 1997; Kuruma and Hartzell, 2000; Greenwood et al., 2001, 2004; Ledoux et al., 2003, 2005; Angermann et al., 2006). Ilate measured at the end of a depolarizing step (Fig. 1B), composed by the sum of an instantaneous (Iinitial) and a timedependent current component, exhibited strong outward rectification, a property previously ascribed to voltage-dependent gating. The slow inward tail current (Itail) detected upon repolarization to ⫺60 mV was consistent with voltage-dependent deactivation. These currents were maintained for at least 10 min after membrane rupture without any significant change in amplitude (data not shown). The evoked current reversed at ⫺3.1 ⫾ 2 mV (n ⫽ 14) near the theoretical equilibrium potential for Cl⫺ (⫺5 mV), and the reversal potential was shifted to more negative potentials (⫺44.5 ⫾ 4 mV; n ⫽ 9) upon replacement of external NaCl with NaSCN. This gave a PSCN/PCl of 5.5 ⫾ 0.45 (n ⫽ 9) that was identical to that recorded in other smooth muscle cell types (e.g., Greenwood and Large, 1999; Piper et al., 2002). These data Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 where On is time spent at the open level; n is the number of observed channels in the patch, and T is total recording time. Data were analyzed using associated Clampfit software (Molecular Devices), whereas figures were produced using Microcal Origin 6.1 or 7.5 (Northampton, MA). All data are means ⫾ S.E.M. taken from at least three animals, whereas statistical tests were performed using paired Student’s t test. NS1619 and NFA were purchased from SigmaAldrich (St. Louis, MO). Isopimaric acid was obtained from Alomone Labs Ltd. (Jerusalem, Israel). allied to the findings of Britton et al. (2002) confirmed that the channel underlying IClCa in mouse portal vein myocytes exhibits very similar biophysical properties as Ca2⫹-dependent Cl⫺ channels in other vascular myocytes (Greenwood et al., 2001, 2004; Ledoux et al., 2003, 2005; Angermann et al., 2006). The Effect of NS1619 on IClCa. NS1619 is a benzimidazole compound that stimulates Ca2⫹-activated potassium (K⫹) currents (IBKCa) in smooth muscle preparations at concentrations between 3 and 100 M (Olesen et al., 1994; Holland et al., 1996; Huang et al., 1997). Application of 30 M NS1619, a concentration shown to produce a marked stimulation of IBKCa in smooth muscle (Olesen et al., 1994; Holland et al., 1996; Huang et al., 1997), enhanced the amplitude of IClCa considerably within 3 min of cell dialysis (Fig. 2A) that was manifest as a greater increase in the amplitude of IClCa at the end of the test step. For IClCa activated by 250 nM [Ca2⫹]i, 30 M NS1619 increased the amplitude of Iinitial by 23% from 39.5 ⫾ 5 to 48.6 ⫾ 5 pA (n ⫽ 14, p ⫽ 0.04, paired Student’s t test), whereas the amplitude of Ilate was increased 93% by this compound from 104 ⫾ 18 to 200 ⫾ 36 pA (p ⬍ 0.0001). Application of the appropriate vehicle had no significant effect on IClCa (n ⫽ 3, data not shown). The effects of NS1619 were reversed significantly upon washout of the agent (Fig. 2A) and were concentration-dependent, with 300 nM and 3 M NS1619 producing an increase in the amplitude of the late current at ⫹70 mV of 8 ⫾ 6% (n ⫽ 4) and 29 ⫾ 9% (n ⫽ 5), respectively. Moreover, 30 M NS1619 had no effect on the negligible current evoked with pipette solutions containing 20 nM [Ca2⫹] (n ⫽ 3). NS1619 had no effect on the time-dependent kinetics exhibited by IClCa (compare panels Aii and Bii in Fig. 3). Moreover, the increase in current amplitude seen in the presence of NS1619 was not due to the de novo activation of a conductance distinct from IClCa because the current recorded in the presence of 30 M NS1619 displayed a reversal potential that was close to the equilibrium potential for chloride ions and not significantly different from that determined in the absence of drug (⬃⫺1 mV; Fig. 2B). Furthermore, the reversal potential of the current recorded in the presence of NS1619 was shifted in a similar manner to control IClCa (see description above; also Britton et al., 2002) by replacement of the external Cl⫺ with SCN⫺ (Erev, ⫺43 ⫾ 13 mV, n ⫽ 4; data not shown). IpA is a pimarine compound structurally unrelated to NS1619 that also augments IBKCa via an interaction with the pore forming subunit (Imaizumi et al., 2002). IpA had similar effects on IClCa as NS1619, and at ⫹80 mV, 3 M IpA increased Ilate evoked by 250 nM Ca2⫹ from 3.4 ⫾ 1 to 7.7 ⫾ 5 pA/pF (p ⬍ 0.001; paired Student’s t test). Similar to NS1619, IpA did not affect the reversal potential of the evoked current (⫺3 ⫾ 0.3 and ⫺3.3 ⫾ 0.4 mV, n ⫽ 4, in the absence and presence of IpA) and had no effect on any of the kinetics of IClCa (e.g., at ⫹80 mV, the mean time constant for current development was 542 ⫾ 46 and 505 ⫾ 52 ms in the absence and presence of IpA, n ⫽ 9, p ⫽ 0.3). Overall, these data show that two structurally unrelated activators of BKCa enhanced IClCa in murine portal vein myocytes. Effect of Niflumic Acid on IClCa Enhanced by NS1619. Similar to studies on rabbit pulmonary artery and coronary artery myocytes that revealed a paradoxical stimulatory effect of the chloride channel blocker NFA on IClCa (for structure, see Greenwood and Large, 1995; Piper et al., 2002; Modulation of Calcium-Activated Chloride Channels 1079 Fig. 3. Effect of niflumic acid on IClCa in the absence or presence of NS1619 in murine portal vein myocytes. Ai, representative experiment showing the effect of 100 M NFA on IClCa evoked by dialysis with 500 nM free [Ca2⫹]. Aii, effect of NFA on the mean time constants for activation at ⫹90 mV (rise, ⽧) and deactivation at ⫺80 mV (decay, ⽧). Bi, effect of 100 M NFA on IClCa augmented by 30 M NS1619. Dotted line, control currents. Bii, effect of NFA on the mean rate of activation at ⫹90 mV (rise t) and mean time constant for deactivation at ⫺80 mV (decay t) elicited in control and after exposure to NS1619. All data are the mean ⫾ S.E.M. of six to nine cells. Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 Fig. 4. Effect of NS1619 on the Ca2⫹ sensitivity of IClCa in murine portal vein myocytes. A, six graphs summarizing the effects of NS1619 on the [Ca2⫹]I dependence of IClCa conductance measured at membrane potentials ranging from ⫺100 to ⫹80 mV. All data are the means ⫾ S.E.M. of four to seven cells. The lines passing through the control and NS1619 data points at ⫺100, ⫺80, ⫺60, and ⫹80 mV are B-spline fits calculated by Origin software. For the remaining two graphs at ⫹40 and ⫹60 mV, the lines are least-squares fits to a logistic function (with error bars taken into account for weighting) of the following form: y ⫽ (A1 ⫺ A2)/(1 ⫹ (x/x0)p) ⫹ A2, where y represents IClCa conductance (nanosiemens), A1 and A2 are, respectively, the maximal and minimal conductance levels (nanosiemens), x is [Ca2⫹]i (nanomolar), x0 is the [Ca2⫹]i yielding half-maximal IClCa conductance (nanomolar; apparent Kd for Ca2⫹), and p is the power factor (index of steepness of the relationship). B, bar graph reporting the effect of NS1619 on the apparent Kd ⫾ fitting error scaled to the square root of 2 for Ca2⫹ at ⫹40 and ⫹60 mV estimated from the analyses of the data sets displayed in A. The calculated errors for the NS1619 bars are within the thickness of bar lines. Ledoux et al., 2005), a supramaximal concentration of NFA (100 M) inhibited Ilate at ⫹80 mV in murine PV myocytes by 32 ⫾ 11% (Fig. 3Ai; n ⫽ 6) that was associated with a slowing of the rate of current development ( ⫽ 296 ⫾ 37 ms in control and 717 ⫾ 74 ms with NFA; p ⬍ 0.01; see Fig. 3Aii), which was reversible upon washout. In addition, NFA increased the current at the holding potential of ⫺60 mV by 58 ⫾ 5 pA and slowed significantly the decay of Itail (Fig. 3Aii). In the presence of 30 M NS1619, application of 100 M NFA inhibited Ilate by 52 ⫾ 9% (Fig. 3Bi), and similar to control IClCa, NFA prolonged the development of current at ⫹80 mV from 256 ⫾ 23 to 415 ⫾ 138 ms (n ⫽ 4; p ⫽ 0.03) and increased the decay 1080 Saleh et al. Ca2⫹; e.g., at ⫹40 mV, the Kd for Ca2⫹ was 529 nM in control and 413 nM in the presence of 30 M NS1619. NS1619 also had a marked effect on the voltage dependence of IClCa activation (Fig. 5). NS1619 produced little effect on IClCa conductance when the cells were dialyzed with 100 nM Ca2⫹ (Fig. 5A, top left). A significant elevation of IClCa conductance by NS1619 with 250 nM Ca2⫹ was detectable at potentials more positive than ⫹20 mV (Fig. 5A, top right). A more pronounced effect of NS1619 became evident at higher [Ca2⫹]i characterized by a leftward shift of the voltage dependence of IClCa conductance, leading to enhancement of steady-state IClCa at negative potentials (Fig. 5A, bottom), especially with 1 M Ca2⫹ (e.g., 3.4-fold increase at ⫺60 mV). All the data sets in Fig. 5A were fitted to a Boltzmann relationship to determine the values for half-maximal activation of IClCa by voltage (V0.5). For all fits, fitting was constrained to a maximal conductance of 11.94 nS, which was determined by fitting the NS1619 data sets with 1 M Ca2⫹ (Fig. 5A, bottom right). The V0.5 values estimated in control and in the presence of NS1619 were plotted as a function of [Ca2⫹]i in Fig. 5B. As previously shown for IClCa recorded from rabbit pulmonary artery myocytes (Angermann et al., 2006), V0.5 declined exponentially as a function of [Ca2⫹]i in control. V0.5 decreased significantly with NS1619 for [Ca2⫹]i between 250 and 1000 nM. The absolute magnitude of the NS1619-induced shift of V0.5 increased from 34 mV with 250 nM [Ca2⫹]i to 84 mV with 1000 nM [Ca2⫹]i (Fig. 5C), indi- Fig. 5. Effect of NS1619 on the voltage dependence of IClCa in murine portal vein myocytes. A, six graphs summarizing the effects of NS1619 on the voltage dependence of IClCa conductance measured at the four intracellular Ca2⫹ concentrations as indicated. All data are the means ⫾ S.E.M. of four to seven cells. All lines passing through the data points are least-squares fits to a Boltzmann function (with error bars taken into account for weighting) of the following form: y ⫽ ((A1 ⫺ A2)/(1 ⫹ exp ((x ⫺ x0)/dx))) ⫹ A2, where y represents IClCa conductance (nanosiemens), A1 and A2 are, respectively, the maximal and minimal conductance levels (nanosiemens), x is the step voltage (millivolts), x0 is the voltage for half-maximal activation or V0.5 (millivolts; see B), and dx is the slope factor (millivolts). As explained in the text, all data sets were fitted to the latter equation by limiting the maximal conductance level (A1) to 12.94 nS, a value determined based on the fitting of the NS1619 group of data (open circles) measured with 1000 nM Ca2⫹ (bottom side graph). From the curve fitting analysis of the data presented in A, the V0.5 values (mean ⫾ fitting error scaled with square root of 2) determined for the control (filled squares) and NS1619 (open circles) data sets were plotted as a function of [Ca2⫹]i in B. The lines are monoexponential fits to the data points with error bars taken into account for weighting. C, graph of the shift in V0.5 induced by NS1619 as a function of [Ca2⫹]i; the data points were calculated by a simple subtraction of the V0.5 values (control ⫺ NS1619) shown in B for each [Ca2⫹]i. Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 of Itail at ⫺60 mV (p ⫽ 0.004; n ⫽ 4; Fig. 3Bii). These data show that the augmentation of IClCa by NS1619 does not affect the interaction of NFA with the channel. It is important to stress that in the absence of NFA, NS1619 did not significantly alter the time constants of activation and deactivation of IClCa relative to control (compare the open bars in Aii and Bii). Does the NS1619-Induced Increase in IClCa Involve a Change in Ca2ⴙ or Voltage Dependence? As shown earlier, activation of IClCa is reliant upon the level of free [Ca2⫹] in the pipette solution, a process that is influenced by membrane potential (Angermann et al., 2006). We thus examined whether NS1619 might exert its stimulatory effect by altering the Ca2⫹ and/or voltage dependence of IClCa. Figure 4A presents the results of our analysis of the Ca2⫹ dependence of the steady-state chord conductance of IClCa at membrane potentials spanning the negative and positive membrane potential ranges. As three of the six panels clearly show, it was not possible to determine an apparent Kd for Ca2⫹ at negative potentials because the conductance displayed no sign of saturation at elevated [Ca2⫹]i in the absence or presence of NS1619. However, both the control and NS1619 data sets at potentials ⱖ ⫹40 mV were successfully fitted to a logistic function yielding apparent Kd values for Ca2⫹ that declined linearly with membrane potential in both groups between ⫹40 and ⫹100 mV (Fig. 4B). The graph in Fig. 4B shows that NS1619 increased the sensitivity of IClCa to intracellular Modulation of Calcium-Activated Chloride Channels relationship that reversed close to ⫺50 mV (a cesium-aspartate-based bathing solution was used that set the equilibrium potential for chloride ions at approximately ⫺50 mV) with slope conductance values calculated to be 1.8 ⫾ 0.3 and 3.1 ⫾ 0.2 pS (n ⫽ 6, Fig. 7A). These values are similar to single IClCa characterized by Piper and Large (2003), who suggested that the larger conductance is the fully open channel, whereas the smaller is a subconductance state. In control condition, the open time distribution was fitted to a double exponential function with mean open times of 4.8 ⫾ 2 and 15 ⫾ 6 ms (n ⫽ 4). Application of 30 M NS1619 resulted in an immediate and reversible effect on channel activity causing a significant increase in the frequency of channel opening over an identical period of time (Fig. 7, B and C). due to the presence of multiple channels in the patch and the very high channel activity elicited by NS1619, kinetic analysis could not be performed in the presence of this agent. With 500 nM [Ca2⫹]i, NP0 was significantly enhanced from 0.271 ⫾ 0.14 in control to 1.52 ⫾ 0.38 with 30 M NS1619 (Fig. 7D). Discussion This study shows for the first time that two structurally distinct activators of BKCa, NS1619 and isopimaric acid, augmented sustained IClCa in vascular smooth muscle cells. As for IClCa recorded in the absence of drug, the current enhanced by NS1619 reversed near the equilibrium potential for Cl⫺, its reversal potential, was shifted by over ⫺40 mV by replacement of extracellular Cl⫺ with SCN⫺, was blocked by the putative IClCa blocker niflumic acid, and exhibited a unitary conductance consistent with that reported for single Ca2⫹-activated Cl⫺ channels (ClCa) recorded in many types of vascular smooth muscles (1–3 pS; Van Renterghem and Lazdunski, 1993; Hirakawa et al., 1999; Piper and Large, 2003). A careful analysis of the biophysical characteristics of IClCa revealed that NS1619 enhanced IClCa by increasing the sensitivity of the channels to Ca2⫹ and shifting their voltage Fig. 6. Effect of NS1619 on IClCa recorded in rabbit pulmonary artery myocytes. A, representative trace of IClCa evoked by 500 nM [Ca2⫹] and recorded at different potentials in the absence and presence of 30 M NS1619. Cells were held at ⫺60 mV and depolarized to ⫹80 mV for 750 ms followed by repolarization to ⫺80 mV for 1 s. B, 100 M NFA had qualitatively similar effects on IClCa as it has on control IClCa. C, mean kinetics of IClCa at ⫹80 and ⫺80 mV in the absence (open bars) and presence (filled bars) of 30 M NS1619. Mean of six cells ⫾ S.E.M. Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 cating that the effects of the BKCa opener on the voltage dependence of IClCa are Ca2⫹-dependent. Effects of NS1619 in Rabbit Pulmonary Artery Myocytes. IClCa generated in murine PV myocytes were qualitatively similar to IClCa evoked by this technique in rabbit pulmonary artery, coronary artery, and PV myocytes (Greenwood et al., 2001). However, it is possible that the stimulatory effect of NS1619 was a “quirk” of the murine PV myocytes. Consequently, experiments were undertaken to determine whether NS1619 also augmented IClCa in rabbit pulmonary artery myocytes, a cell type where IClCa has been studied extensively (Greenwood et al., 2001, 2004; Angermann et al., 2006). NS1619 (30 M) had similar effects on IClCa evoked in pulmonary artery myocytes (Fig. 6A). The amplitude of Ilate was increased 63 ⫾ 8% in eight cells with no significant effect on the kinetics of IClCa either at ⫹90 or ⫺80 mV (Fig. 6C). The augmented IClCa recorded in the presence of NS1619 was modulated by 100 M NFA in a manner identical to control IClCa recorded in the absence of NS1619 (Fig. 6B). These data show that the enhancement of IClCa by NS1619 is a characteristic of vascular IClCa and is not unique to the mouse PV. Properties of Single Ca2ⴙ-Activated Clⴚ Channels in Inside-out Patches. IClCa was investigated in the inside-out configuration of the patch-clamp technique so that the [Ca2⫹]i could be manipulated, and the reagents could be applied directly onto the intracellular surface of the membrane. Piper and Large (2003) have previously conducted a thorough analysis on the single-channel IClCa in this particular preparation; therefore, extensive characterization was not deemed necessary. At ⫹80 mV in low-Ca2⫹ solution (14 nM), no channel activity was present (Fig. 7B), but the rapid addition of 500 nM Ca2⫹ evoked an outwardly directed single-channel current. This Ca2⫹-activated channel opened to two levels of approximately 0.2 and 0.4 pA (see Fig. 7, Bii and Ci), which may represent either two channels in the patch or two conductance levels. Both channels displayed a linear I-V 1081 1082 Saleh et al. dependence toward negative potentials that resulted in an increase in open probability and/or number of available channels. These findings, allied to the observation that Cl⫺ channel blockers stimulate BKCa, show that there is a similarity in the pharmacology of calcium-activated chloride channel and large-conductance calcium-dependent potassium channel encoded by Slo1. Activators of BKCa Stimulate IClCa. Extensive studies on the effect of global dephosphorylation on IClCa in rabbit pulmonary artery myocytes revealed that augmentation of IClCa produced by prohibiting phosphorylation by intracellular dialysis with the nonhydrolyzable ATP analog adenylyl5⬘-imidodiphosphate was mediated by a marked negative shift in the voltage dependence of activation (Angermann et al., 2006). It is possible that NS1619 or IpA enhanced IClCa by blocking CaMKII (Greenwood et al., 2001) and/or by stimulating calcineurin (Ledoux et al., 2003; Greenwood et al., 2004), which have been shown to induce such shifts. However, this seems unlikely because alterations in the phosphorylation status of the channel or regulatory subunit were accompanied by marked changes in activation and deactivation kinetics of IClCa, whereas those produced by NS1619 or IpA were not. Future studies will be undertaken to ascertain how phosphorylation affects the stimulatory action of NS1619 and IpA. NS1619 (0.3–30 M) and IpA (3 M) enhanced IClCa at concentrations that increase BKCa markedly (Olesen et al., 1994; Imaizumi et al., 2002). Because IClCa in the present study was evoked without reliance upon other mechanisms such as the opening of Ca2⫹ channels or Ca2⫹ release processes the stimulatory effect of NS1619 and IpA reflected an augmentation of the Cl⫺ channel activity as opposed to a perturbation of Ca2⫹ homeostatic mechanisms. Analysis of the effect of NS1619 on the intrinsic Ca2⫹ or voltage sensitivity of IClCa (described extensively by Angermann et al., 2006) showed that NS1619 reduced the apparent Kd for Ca2⫹ at positive potentials and caused a negative shift in the voltage dependence of activation, resulting in basal activation of the channels at negative potentials in the presence of 1 M Ca2⫹. Furthermore, other experiments confirmed that application of NS1619 to excised patches reversibly increased NP0 of a low conductance (⬃3 pS) anion channel whose activation had an absolute requirement for an elevated Ca2⫹ concentration facing the cytoplasmic side of the membrane patch. Consistent with our whole-cell data, the channel stimulated by NS1619 had similar characteristics to those of ClCa described in this preparation (Piper and Large, 2003) and thus was not due to the activation of an unidentified silent channel. Because a detailed kinetic analysis could not be performed due to the presence of numerous channels in all patches tested, it was not possible to conclude unequivocally whether NS1619 exerted its effects on single ClCa by increasing their open probability, by recruiting silent channels, or both. Similar to Piper and Large (2003), we identified two conductance levels in our single-channel experiments, and although not analyzed in detail, our data suggest that NS1619 did not produce a shift in the proportion of the two conductance levels. Clearly, more experiments are necessary to address this question, in particular by examining the Ca2⫹ and voltage dependence of single ClCa. The ability of all the BKCa modulators to affect IClCa could simply be a pluripotent effect of “dirty drugs.” However, the likelihood of two specific activators of BKCa having nonspecific effects seems remote. This leaves four plausible interpretations of our data. Firstly, the enhancement of the evoked current by NS1619 and IpA could have been due to the de novo activation of IBKCa. However, the fact that the current in the presence and absence of either activator reversed close to the theoretical Cl⫺ equilibrium potential, which was shifted by the same extent upon replacement of the external Cl⫺ by the more permeable anion thiocyanate, suggests that this scenario is unlikely. Any contribution to Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 Fig. 7. The effect of NS1619 on unitary IClCa in smooth muscle cells from the rabbit pulmonary artery. A, I-V relationship showing the two conductance levels that were predominantly seen in the inside-out configuration with 500 nM [Ca2⫹]i. The mean data were fitted with linear relationships yielding the slope conductance values shown. Bi, long-term trace from a patch being held at ⫹80 mV exposed initially to 14 nM [Ca2⫹]i and subsequently to 500 nM [Ca2⫹]i in the presence and absence of 30 M NS1619, all applied to the internal surface of the membrane. No channel activity was seen with 14 nM [Ca2⫹]i, and this is highlighted in Bii, trace 1, which shows the channel activity of the corresponding long-term trace on a shorter time scale. Bii, traces 2 and 3, correspond to channel activity with 500 nM [Ca2⫹]i and 30 M NS1619, respectively. C, two amplitude histograms displaying the frequency of channel openings within a 2-min period before (Ci) and after (Cii) the application of 30 M NS1619. D, bar graph, effect of NS1619 on channel NP0. Modulation of Calcium-Activated Chloride Channels revealed no homology of mouse Slo1 with either CLCA or Bestrophin genes when aligned specifically. Recently, Suzuki and Mizuno (2004) identified genes called Tweety (ttyh1–3), whose products have comparable structure with BKCa and encode for a large-conductance Cl⫺ channel activated by an increase in [Ca2⫹] with an EC50 of 2 M. Although the biophysical properties of the currents generated by expression of ttyh3 were not similar to native IClCa in smooth muscle cells, this paper highlights that putative Cl⫺ channel correlates can have considerable homology with K⫹ channels. It is likely that the protein forming the ClCa is a multimeric complex that may incorporate a number of the proteins described above. Interestingly, coexpression of the  subunit that associates with mSlo1 expression products to form native BKCa has been shown to increase the Ca2⫹ sensitivity of mCLCA1 (Greenwood et al., 2002). Overall, the data of the present study suggest that determination of the elusive nature of the Ca2⫹-activated Cl⫺ channel may lie with previously unconsidered protein interactions. 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Can J Physiol Pharmacol 83:541–556. Ledoux J, Greenwood IA, and Leblanc N (2005) Dynamics of Ca2⫹-dependent Cl⫺ channel modulation by niflumic acid in rabbit coronary arterial myocytes. Mol Pharmacol 67:163–173. Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017 the gross current due to BKCa activation would be negligible due to the presence of TEA in the internal and external solutions, lack of external K⫹, and the presence of Cs⫹ instead of K⫹ in the internal solution. Consequently, the stimulatory effect produced by NS1619 or IpA was the result of a modulation of the activated Cl⫺ conductance and not by unmasking a quiescent BKCa or another conductance. Secondly, IClCa recorded in K⫹-free conditions in the present study and similar previous investigations represent an abstract scenario with Cl⫺ ions permeating an extant BKCa. There are many splice variants of the Slo genes (Butler et al., 1993; Tseng-Crank et al., 1994), but none of them correlates with an anion permeable pore. Moreover, the anion permeability of the sustained IClCa in various vascular smooth muscle cells (Greenwood et al., 2001; Piper et al., 2002; present study) is identical to transient IClCa occurring either spontaneously or following the influx of Ca2⫹ through voltage-dependent channels (e.g., Greenwood and Large, 1999). Furthermore, spontaneously occurring IClCa have been recorded in K⫹-containing conditions contemporaneously with spontaneous K⫹ currents carried by BKCa (e.g., Wang et al., 1992; Large and Wang, 1996; ZhuGe et al., 1998; present study; data not shown). A final possibility is that Slo1 somehow interacts physically with neighboring ClCa. However, the most prosaic and simplest hypotheses that can be derived from the data of the present study, allied to the findings that CCBs activate BKCa, is that there are some similarities in the proteins underlying native IClCa and those that are encoded by Slo1, which underpins the similarity in the pharmacology of IClCa and BKCa. Molecular Identity of the Ca2ⴙ-Activated Clⴚ Channel. To date two families of genes (CLCA and bestrophin) have been postulated to underlie the Ca2⫹-dependent Cl⫺ conductance, but the role of CLCA gene products as ion channels has been repudiated on the strength of the poor membrane topology and immunocytochemical evidence, whereas some of these proteins are speculated to exist as secretory products (Gibson et al., 2005; Loewen and Forsyth, 2005). Bestrophin genes are expressed in vascular smooth muscle cells (Leblanc et al., 2005), and the expression of Bestrophin genes in HEK-293 cells produces Ca2⫹-sensitive Cl⫺ conductances (Sun et al., 2002) at physiological [Ca2⫹] (Qu et al., 2004). Moreover, mutations of specific amino acids within the putative pore region have been shown to alter ion conductance proving that these proteins do form anion channels (Qu et al., 2004). However, there are considerable differences between native IClCa and currents produced by Bestrophin expression in mammalian cell lines, and we do not know if BKCa activators enhance Cl⫺ currents produced by the heterologous expression of Bestrophin genes. The crossover in channel pharmacology suggest that gene products of Slo1 or other members of the Slo family of genes (Slick, Slo2.1; Slack, Slo2.2) could also be considered as molecular candidates for the channel underlying IClCa. 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Van Renterghem C and Lazdunski M (1993) Endothelin and vasopressin activate low conductance chloride channels in aortic smooth muscle cells. Pflugers Arch 425: 156 –163. Wang Q, Hogg RC, and Large WA (1992) Properties of spontaneous inward currents recorded in smooth muscle cells isolated from the rabbit portal vein. J Physiol 451:525–537. ZhuGe RH, Sims SM, Tuft RA, Fogarty KE, and Walsh JV Jr (1998) Ca2⫹ sparks activate K⫹ and Cl⫺ channels, resulting in spontaneous transient currents in guinea-pig tracheal myocytes. J Physiol 513:711–718. Address correspondence to: Dr. Iain A. Greenwood, Ion Channels and Cell Signaling Research Centre, Division of Basic Medical Sciences, St. George’s, University of London, SW17 0RE London, UK. E-mail: [email protected] Downloaded from jpet.aspetjournals.org at ASPET Journals on June 15, 2017
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