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Address correspondence to Masahiro Oike, Department of Pharmacology, Graduate School of Medical Sciences, Kyushu University, Fukuoka 812-8582, Japan. Fax: (81) 92-642-6079; E-mail: moike{at}pharmaco.med.kyushu-u.ac.jp
| ABSTRACT |
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Key Words: ATP release nitric oxide hypotonic stress volume-regulated anion channel calcium
| INTRODUCTION |
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The cystic fibrosis transmembrane conductance regulator (Reisin et al., 1994
; Schwiebert et al., 1995
; Cantiello et al., 1998
) and the mdr-1 gene product P glycoprotein (Abraham et al., 1993
; Roman et al., 1997
) have been proposed as putative candidates for the mechanically or HTS-induced ATP release pathway, but more recently evidence has been presented that these proteins are modulators of ATP release through an ATP channel (Grygorczyk and Hanrahan, 1997
; Braunstein et al., 2001
; Roman et al., 2001
). Recently, it has been reported that the large conductance anion channel (Sabirov et al., 2001
) may be the pathway for HTS-induced ATP release in cultured mammary tumor cells, and that the mechanosensitive ATP release in Xenopus oocyte might be mediated by a membrane trafficking mechanism that is suppressed by brefeldin A and cytochalasin D (Maroto and Hamill, 2001
).
The ubiquitously expressed volume-regulated anion channel (VRAC) (Nilius et al., 1996
), which has been shown to be permeable for large anions (Strange et al., 1996
; Nilius et al., 1997a
; Okada, 1997
), is an alternative putative pathway for the release of negatively charged nucleotides, including ATP and UTP, all the more so because VRAC currents and the ATP release pathway share a number of common properties: (a) The HTS-induced ATP release in bovine aortic endothelial cells (BAEC) (Koyama et al., 2001
) and the activation of VRAC (Voets et al., 1998
; Nilius et al., 1999
) are both mediated by Rho/Rho-kinase and tyrosine kinase. (b) The HTS-induced ATP release and activation of VRAC are concurrent, i.e., both responses are activated within 1 min after starting hypotonic challenge and reach their maximum after a few minutes (Nilius et al., 1994a
; Koyama et al., 2001
). (c) Extracellular ATP is a voltage-dependent blocker of VRAC (Ackerman et al., 1994
; Jackson and Strange, 1995
; Tsumura et al., 1996
), which is reminiscent for open pore block, and a number of open pore blockers with dimensions even larger than those of ATP have been shown to permeate through VRAC (Droogmans et al., 1998
, 1999
).
In this study, we first examined the effects of VRAC inhibitors on the HTS-induced ATP release and the concomitant cellular responses in BAEC. Since the currently available VRAC inhibitors are not selective, we have used four different chemicals with distinct physicochemical properties and structure that have been reported to inhibit VRAC, i.e., tamoxifen (Nilius et al., 1994b
), fluoxetine (Maertens et al., 1999
), verapamil (Nilius et al., 1994a
), and glibenclamide (Yamazaki and Hume, 1997
), and found that as well as their blocking action on VRAC currents, they all inhibited HTS-induced ATP-release but not the responses to exogenously applied ATP. In a second series of experiments, we performed a detailed quantitative analysis of the voltage-dependent inhibition of the VRAC current by various nucleotides (ATP, ADP, UTP, CTP, GTP) using a permeating blocker model. This model does not only predict the binding of these nucleotides at an electrical distance of 0.4 inside the channel, but also their permeation across the membrane. Furthermore, we observed that high concentrations of extracellular ADP enhanced the outward component of the VRAC current and shifted its reversal potential to more negative values under conditions where the contribution of Cl- ions to the VRAC current was minimized by reducing intra- and extracellular Cl- concentrations. It is concluded that VRAC is permeable for these nucleotides, and provides a pathway for HTS-induced ATP release in BAEC.
| MATERIALS AND METHODS |
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Measurement of Intracellular Ca2+ Concentration
[Ca2+]i was measured at room temperature (2025°C) with fura-2 fluorescence using an Attofluor digital fluorescence microscopy system (Atto Instruments) as described previously (Koyama et al., 2001
).
Measurement of the Intracellular Production of NO
NO was measured with diaminofluorescein-2 (DAF-2), an NO-sensitive fluorescent dye (Kojima et al., 1998
), as reported previously (Kimura et al., 2001
). Since DAF-2 fluorescence increases almost linearly with NO concentration (Kojima et al., 1998
), the fluorescence intensities in each experiment were normalized to a reference image recorded before hypotonic challenge (Kimura et al., 2001
).
Measurement of Extracellular ATP Concentration by Luciferase Bioluminescence
The extracellular ATP concentration ([ATP]o) was measured using luciferinluciferase bioluminescence as described previously (Koyama et al., 2001
). ATP concentration in the presence of VRAC inhibitors was calculated from calibration curves in the presence of these inhibitors.
Measurement of Membrane Current
Whole cell membrane current was recorded in the conventional ruptured whole cell configuration (Hamill et al., 1981
) with an EPC-9 amplifier (Heka Elekronik GmbH). The pipette solution for examining the effects of VRAC inhibitors and brefeldin A contained (in mM): KCl 40, K-aspartate 100, MgCl2 1, Na2ATP 5, HEPES 10, and EGTA 5 (pH adjusted to 7.3 with KOH). For the effects of 1 mM extracellular nucleotides (Figs. 4 and 5)
, the pipette solution contained (in mM): CsCl 45, Cs-aspartate 100, MgCl2 1, Na2ATP 5, HEPES 10, BAPTA 5, and CaCl2 1.436 (to give free [Ca2+]i of 30 nM, pH adjusted to 7.3 with CsOH). To examine the contribution of extracellular ADP to the VRAC current (see Fig. 6)
, we have used a pipette solution with reduced Cl- concentration containing (in mM): Cs-aspartate 145, MgCl2 1, Na2ATP 1, HEPES 10, BAPTA 5, and CaCl2 1.503 (to give free [Ca2+]i of 30 nM, pH adjusted to 7.3 with CsOH). The osmolarity of each solution was adjusted to 300 mOsm with a freezing point depression osmometer (OM-801; Vogel) by adding mannitol. In the experiments with extracellular nucleotides, we pretreated the cells with 1 µM thapsigargin for 30 min to deplete intracellular Ca2+ stores in order to avoid a possible contamination with Ca2+-activated chloride currents (Nilius et al., 1997b
) that might be activated by nucleotide-induced Ca2+ release.
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Data Analysis
The voltage dependence of current inhibition in the presence of extracellular nucleotides was fitted to Eqs. 1 and 2 using Origin software (OriginLab Corp.).
Data are given as mean ± standard error of the mean. Statistical significance between two groups was determined by using Student's unpaired t test. Probabilities less than 5% (P < 0.05) were regarded as significant.
| RESULTS |
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The time course of activation and the pharmacological properties of this current indicate that it is probably due to activation of the ubiquitously expressed VRAC channels (Nilius et al., 1996
). Because it was recorded using a pipette solution containing 5mM EGTA, it is unlikely that it was due to activation of Ca2+-activated Cl- channels by the concomitant HTS-induced Ca2+ release. Moreover, its outward rectification is less prominent than that of Ca2+-activated Cl- channels (Nilius et al., 1997b
). Because it is inhibited by tamoxifen, this current is also different from the tamoxifen-activated large conductance Cl- channel current in endothelium (Li et al., 2000
). Also, exogenous ATP did not activate a similar current in isotonic solutions, indicating that it was not activated by an autocrine action of ATP released from the cell during the hypotonic challenge.
The current in isotonic solution was insensitive to VRAC inhibitors, and was not suppressed in hypertonic solution (unpublished data), indicating that it is not due to a partial activation of VRAC in isotonic solution.
These VRAC inhibitors also suppressed the HTS-induced release of ATP, assessed from the increase in extracellular ATP concentration ([ATP]o, 9.7 ± 0.5 nM) (Fig. 1 B). Glibenclamide and fluoxetine inhibited this ATP release in a concentration-dependent manner that was similar to their effects on VRAC inhibition (Fig. 1 C). Furthermore, glibenclamide (Fig. 2 A, b), fluoxetine, and verapamil abolished HTS-induced Ca2+ oscillations (Fig. 2 A, a), and the HTS-induced NO production (Fig. 2 B, a) in BAEC, which are both mediated by the released ATP (Oike et al., 2000
). Because of its autofluorescence, we could not use tamoxifen in these fluorescent dye assays. These VRAC inhibitors did, however, not affect the responses downstream of ATP release, since they had no effect on Ca2+ transients (Fig. 2 A, c) and NO production (Fig. 2 B, b) induced by exogenously applied ATP (1 µM).
Effects of Brefeldin A on HTS-induced ATP Release and VRAC Current
It has been proposed recently (Maroto and Hamill, 2001
) that the HTS-induced ATP release in Xenopus oocytes represents a vesicular transport process sensitive to brefeldin A, an inhibitor of vesicular transport (Klausner et al., 1992
). Brefeldin A did not, however, affect HTS-induced ATP release (Fig. 3 A) or VRAC currents (Fig. 3 B), indicating that membrane trafficking does not contribute to HTS-induced ATP release in BAEC.
Voltage-dependent Inhibition of VRAC with Extracellular ATP in BAEC
The close correlation between the effects of VRAC inhibitors on current activation and ATP release in BAEC is compatible with the release of ATP through VRAC channels. The most compelling evidence for permeation of ATP through VRAC would be the demonstration of VRAC currents under conditions where ATP is the only permeant anion. Single-channel and whole-cell ATP currents have been measured through P-glycoprotein (Abraham et al., 1993
), the cystic fibrosis transmembrane conductance regulator (Reisin et al., 1994
), and through large conductance chloride channels (Sabirov et al., 2001
). Unfortunately, all our attempts to record single channel ATP currents from BAEC cells failed so far, whereas application of extracellular ATP at concentrations of 10 mM or higher induced membrane leakiness. We have therefore used an alternative approach to provide more direct evidence for ATP permeation that is based on a quantitative analysis of the voltage-dependent block of VRAC by extracellular ATP (Ackerman et al., 1994
; Jackson and Strange, 1995
; Tsumura et al., 1996
). As shown in Fig. 4, A and B, extracellular ATP (total concentration of 1 mM; free concentration of 0.15 mM) inhibited the outward current through VRAC, but not the inward current. Current inhibition at positive potentials, expressed as the fraction of hypotonic current blocked by extracellular ATP, showed a marked voltage dependency, which is reminiscent of open pore block due to binding of ATP inside the VRAC pore. This inhibition reached a maximum of
3040 mV and declined at more positive potentials (Fig. 4 C).
A similar bell-shaped voltage-dependence of inhibition of endothelial VRAC currents has already been observed with calix[4]arene and suramin (Droogmans et al., 1998
), and could be described by a model in which the relief of inhibition at strongly positive potentials was explained by the permeation of this large anion through VRAC. We have used the same "permeating blocker" model, which assumes binding of extracellular ATP to a site at an electrical distance
inside the channel pore from which it can be released either to the inside or outside, to analyze the voltage-dependence of VRAC inhibition by extracellular ATP, i.e.,
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ATPo and ATPi represent extracellular and intracellular ATP, and k01(V), k10(V), k12(V), and k21(V) represent the voltage-dependent transition rate constants between the various states. The fraction of channels occupied by ATP at extra- and intracellular concentrations [ATP]o and [ATP]i and potential V is given by
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![]() | (1) |
The calculated free [ATP]i in the pipette solution is 3.1 mM. This equation was fitted to the experimental data, and shown as the solid line in Fig. 4 C.
From the pooled data from nine cells, we obtained the following values for the parameters: Kd(0) = 1.0 ± 0.5 mM,
= 0.41 ± 0.03, and r = 0.38 ± 0.08.
We have also fitted the data to a simplified equation (Eq. 2), which does not take into account the binding of intracellular ATP inside the pore at positive potentials (k21(V)
0) (dashed line in Fig. 4 C).
![]() | (2) |
The values of Kd(0) = 1.0 ± 0.3 mM,
= 0.42 ± 0.02, r = 0.42 ± 0.16 (n = 9) obtained with Eq. 2 are similar to those obtained with Eq. 1. We have therefore used this simplified equation in subsequent fits (see below).
The value of r = 0.38 indicates that the transition of ATP from the cytoplasm to its binding site in the membrane and vice versa represents the rate limiting step for ATP permeation though the membrane. The probability that ATP bound to its site in the pore will be released to the extracellular side rather than into the cytosol at 0 mV is given by k10(0)/[k10(0)+k12(0)] = 1/(1 + r) = 0.72; i.e. 72% of the total amount of cytosolic ATP entering the pore and binding at its intramembrane site will be released into the extracellular space and contribute to net ATP release at 0 mV. This fraction will be even larger at the resting potential of BAEC cells of about -15 mV, as assessed from the reversal potential of the VRAC current.
Effects of other Nucleotides on VRAC Current in BAEC
The three-dimensional structure of ATP is similar to that of other negatively charged triphosphate nucleotides (UTP, GTP, and CTP) present in the cell. We therefore used the same protocol as in Fig. 4 to examine whether these nucleotides as well as other adenine nucleotides with a reduced number of phosphate residues (ADP, AMP, and adenosine) also permeate through VRAC. We have always used a total concentration of 1 mM for these nucleotides.
All molecules except adenosine inhibited the outward component of the VRAC current (Fig. 5). The block of AMP was weakly voltage-dependent, but all other nucleotides exerted a substantial voltage-dependent block. The current inhibition by all nucleotides except adenosine and AMP could be fitted to Eq. 2, which indicates that they permeate through VRAC (Fig. 5 B). The values of Kd(0),
, and r for the various nucleotides from the fits to Eqs. 1 and 2 are summarized in Table I.
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| DISCUSSION |
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VRAC inhibitors are not very specific, and their effects on ATP release appear to be cell specific in the sense they inhibit ATP release in some tissues but are ineffective in others, e.g., NPPB suppressed ATP release in prostate cancer cells (Sauer et al., 2000
) and cultured ciliary epithelial cells (Mitchell et al., 1998
), whereas tamoxifen was effective in prostate cancer cells (Sauer et al., 2000
) but not in ciliary epithelial cells (Mitchell et al., 1998
). The effects of these substances on VRAC currents are also quite heterogeneous, and the concentrations for half-maximal inhibition of VRAC currents range, depending on the cell-type, from a few µM to 1 mM (for review see Nilius et al., 1997a
). For instance, tamoxifen is a very potent inhibitor in most tissues, but did not significantly inhibit VRAC currents in BC3H1 and C2C12 cells at concentrations up to 100 µM (Voets et al., 1997
). These heterogeneous responses therefore seem to point to a family of VRAC channels with different biophysical and pharmacological properties. Hazama et al. (1999)
reported a number of experimental findings in a cultured human epithelial cell line that seem to contradict the correlation between VRAC currents and ATP release in this cell type, indicating that ATP release may not be a general property of all VRAC channels. It might therefore be useful to analyze the voltage-dependence of ATP block of VRAC in this cell type, as well as in other cell types, such as intestinal epithelium (Tsumura et al., 1996
), glioma cells (Jackson and Strange, 1995
), and Xenopus oocytes (Ackerman et al., 1994
), in which ATP exerts a voltage-dependent block of VRAC.
Sabirov et al. (2001)
reported recently that ATP release in cultured mouse mammary C127i cells occurs through a large conductance anion channel (400pS). It is, however, unlikely that this large conductance anion channel contributes to ATP release in BAEC, because (a) glibenclamide inhibits HTS-induced ATP release (Fig. 1 C) but not the large conductance anion channel (Sabirov et al., 2001
), and (b) tamoxifen, which activates a similar large conductance anion channel (368 pS) in porcine aortic endothelial cells (Li et al., 2000
), inhibits HTS-induced ATP release (Fig. 1 C).
Our data also exclude a membrane traffickingmediated ATP release (Maroto and Hamill, 2001
) in BAEC, since brefeldin A did not affect ATP release or VRAC currents (Fig. 3). In addition, we have reported previously that disruption of the actin cytoskeleton with cytochalasin B does not inhibit HTS-induced ATP release (Koyama et al., 2001
).
The analysis of the ATP-induced, voltage-dependent inhibition of VRAC currents (Fig. 4) provides more direct evidence for permeation of ATP through VRAC. It is unlikely that these effects result from the activation of purinergic receptors, resulting in the activation of protein kinase C and/or Ca2+ mobilization, because these intracellular messengers do not affect VRAC (Nilius et al., 1996
). The Kd(0) value of ATP binding of 1.0 mM is within a reasonable range considering the millimolar concentration of intracellular ATP. Also, the value of r (= k12(0)/k10(0) = 0.38) indicates that 72% of cytosolic ATP that binds to the channel permeates through the membrane at 0 mV. The three-dimensional structure of ATP consists of a centered ribose with arms of adenine (9.2 Å) and triphosphate (13.5 Å) residues. Permeation of ATP through the VRAC pore is therefore also compatible with the lower and upper limits of the cross-sectional area of 11 x 12 and 12 x 17 Å2 of the VRAC pore, as derived from the permeation properties of calixarenes in endothelium (Droogmans et al., 1999
). From these evidences for ATP permeation through VRAC, we conclude that this channel is the major candidate of the ATP release pathway during hypotonic stimulation in BAEC. This model also predicts that the interaction of intracellular ATP with the channel may account for the outward rectification of VRAC currents.
CTP, GTP, UTP, and ADP also showed a bell-shaped voltage-dependent inhibition of VRAC current, that could be fitted to the permeating blocker model (Fig. 5), suggesting that these nucleotides permeate through VRAC by binding to a common site that is located at
40% of the electrical field (Table I). The observation that adenosine does not inhibit VRAC currents indicates that the negatively charged phosphate residues of the nucleotides might be essential for their interaction with the binding site in the VRAC pore. This is also consistent with the weak voltage dependence of the inhibition by AMP. Since these nucleotides, at least ADP and UTP, have been reported to induce Ca2+ transients in endothelium (Viana et al., 1998
), the release of nucleotides other than ATP may also contribute to the HTS-induced Ca2+ transients (Fig. 2 A, a) and NO production (Fig. 2 B, a) in BAEC.
Because of the skinning effects of high extracellular ATP concentrations, we were unable to directly demonstrate ATP permeation through VRAC. However, our experimental data with high ADP concentrations provide compelling evidence for the nucleotide permeability of VRAC. Together with the observed close correlation between inhibition of VRAC currents and HTS-induced ATP release and the voltage-dependent inhibition of VRAC currents by ATP and other nucleotides, our data provide unequivocal evidence that VRAC provides a pathway for HTS-induced release of ATP and presumably of other purinergic agonists in BAEC. It might be the subject of future investigations to find out whether VRAC is also the pathway for ATP release induced by other mechanical stimuli, such as shear stress (Bodin et al., 1991
) and mechanical strain (Sauer et al., 2000
), since it has been reported that shear stress activates a chloride conductance similar to VRAC in vascular endothelial cells (Barakat et al., 1999
).
| FOOTNOTES |
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| ACKNOWLEDGMENTS |
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This study was carried out as a part of "Ground Research Announcement for Space Utilization" promoted by the National Space Development Agency of Japan and Japan Space Forum (M. Oike).
Submitted: 5 December 2001
Revised: 8 April 2002
Accepted: 22 April 2002
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