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Department of Neurophysiology, University of Cologne, D-50931 Cologne, Germany
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ABSTRACT |
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Mechanical strain applied to prostate cancer cells induced an intracellular Ca2+ (Cai2+) wave spreading with a velocity of 15 µm/s. Cai2+ waves were not dependent on extracellular Ca2+ and membrane potential because propagation was unaffected in high-K+ and Ca2+-free solution. Waves did not depend on the cytoskeleton or gap junctions because cytochalasin B and nocodazole, which disrupt microfilaments and microtubules, respectively, and 1-heptanol, which uncouples gap junctions, were without effects. Fluorescence recovery after photobleaching experiments revealed an absence of gap junctional coupling. Cai2+ waves were inhibited by the purinergic receptor antagonists basilen blue and suramin; by pretreatment with ATP, UTP, ADP, UDP, 2-methylthio-ATP, and benzoylbenzoyl-ATP; after depletion of ATP by 2-deoxyglucose; and after ATP scavenging by apyrase. Waves were abolished by the anion channel inhibitors 5-nitro-2-(3-phenylpropylamino)benzoic acid, tamoxifen, 4,4'-diisothiocyanatostilbene-2,2'-disulfonic acid, niflumic acid, and gadolinium. ATP release following strain was significantly inhibited by anion channel blockers. Hence, ATP is secreted via mechanosensitive anion channels and activates purinergic receptors on the same cell or neighboring cells in an autocrine and paracrine manner, thus leading to Cai2+ wave propagation.
calcium wave; adenosine 5'-triphosphate release; purinergic receptor; anion channel
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INTRODUCTION |
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CALCIUM WAVES HAVE BEEN OBSERVED in various excitable and nonexcitable cells where they coordinate physiological responses within the respective tissues. In nonexcitable cells the most intensively investigated mechanism for wave propagation is based on strain-induced inositol trisphosphate [Ins(1,4,5)P3] formation and diffusion though gap junctional pores. Ins(1,4,5)P3 then releases intracellular Ca2+ from Ins(1,4,5)P3-sensitive Ca2+ stores in the neighboring cells (2, 36, 37). Recent studies on basophil leukemic cells, hepatocytes, and osteoblastic cell lines (21) have shown that intracellular Ca2+ (Cai2+) waves may be alternatively propagated via activation of purinergic receptors of the G protein-coupled P2Y class that activate phospholipase C (PLC), resulting in the generation of Ins(1,4,5)P3 and intracellular Ca2+ release from Ins(1,4,5)P3-sensitive Ca2+ stores. Although it has been speculated that purinergic receptor activation and Cai2+ wave propagation may be mediated by ATP release from the mechanically stimulated cells, the molecular mechanism of purinergic receptor stimulation following mechanical strain remains poorly defined. ATP release triggered by mechanical strain has been recently reported and apparently did not involve the cystic fibrosis transmembrane regulator (CFTR) (47). Furthermore, it has been demonstrated that connexins regulate, via a still unraveled mechanism, strain-mediated Ca2+ signaling by controlling ATP release. In this study ATP release was inhibited by anion channel blockers (12).
The present study reports on mechanical strain-elicited
Cai2+ waves in confluent prostate cancer cells
of the DU-145 cell line, which were independent of intercellular
communication because they persisted after uncoupling of gap junctions.
Cai2+ wave propagation could be inhibited by
antagonists of purinergic receptors and by preincubation with several
nucleotides, indicating that activation of multiple purinergic
receptors, including P2Y2 receptors, which have been
previously shown to be present in DU-145 prostate cancer cells
(46), may underlie wave propagation. In hypotonic solution
these cells secreted ATP. Because ATP release could be inhibited by
blockers of anion channels, we concluded that purinergic receptor
activation during Cai2+ wave propagation is
mediated via ATP release through volume-activated Cl
channels. ATP released by mechanical strain will diffuse radially in
the extracellular space and will propagate a
Cai2+ wave spreading up to a distance of ~300
µm from the stretched cell area.
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MATERIALS AND METHODS |
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Chemicals. Fluo 3-acetoxymethyl ester (AM) and 5-carboxyfluorescein diacetate (5-CFDA) were purchased from Molecular Probes (Eugene, OR). ATP, ADP, UTP, UDP, 2-methylthio-ATP (2-MeS-ATP), benzoylbenzoyl-ATP (Bz-ATP), apyrase, 2-deoxyglucose, 1-heptanol, tamoxifen, niflumic acid, suramin, basilen blue, 4,4'-diisothiocyanatostilbene-2,2'-disulfonic acid (DIDS), U-73122, histamine, and GdCl3 were from Sigma (Deisenhofen, Germany). 5-Nitro-2-(3-phenylpropylamino)benzoic acid (NPPB) and glibenclamide were from RBI (Natick, MA).
Cell culture.
The human prostate cancer cell line DU-145 was kindly provided by Dr.
J. Carlsson (Uppsala, Sweden). Cells were cultivated in
25-cm2 tissue culture flasks (Costar, Fernwald, Germany) in
5% CO2 and humidified air at 37°C with Ham's F-10
medium (GIBCO, Life Technologies, Gaithersburg, MD) supplemented with
10% fetal calf serum (Boehringer Mannheim, Mannheim, Germany), 2 mM
glutamine, 0.1 mM
-mercaptoethanol, 2 mM minimal essential
medium, 100 IU/ml penicillin, and 100 µg/ml streptomycin (ICN
Flow, Meckenheim, Germany). For the experiments, cells grown to
confluency in tissue culture flasks were enzymatically dissociated in
Ca2+-free phosphate-buffered saline supplemented with
0.05% EGTA and 0.1% trypsin. Single cells were plated to coverslips
and cultivated to confluency.
Bioluminescence experiments.
ATP release from confluent DU-145 cells was determined using a
luciferin-luciferase assay (Sigma) in a chemiluminescence apparatus (Bioluminiscence Analyzer XP2000, SKAN, Basel, Switzerland) under dim
light. For data sampling, the output of the photomultiplier tube of the
setup was connected to a multimeter (Voltcraft M-3610D, Conrad
Electronics, Hirschau, Germany) and a Tandon 286/N personal computer
(Tandon, Moorpark, CA). Cells grown to confluency on 20 × 20-mm
coverslips were washed five times in F-10 cell culture medium, which
resulted in a background luminescence signal that was not significantly
different from the signal obtained with cell culture medium in the
absence of cells. Cells were subsequently immersed in 1 ml of F-10 cell
culture medium that was diluted 1:1 with distilled water, resulting in
an osmolality of 150 mosmol/kgH2O. In control experiments,
cells grown to confluency on coverslips were immersed in an equal
volume of isotonic medium. For the experiments with anion channel
inhibitors, cells were preincubated for 5 min in isotonic F-10 cell
culture medium that was supplemented with the respective inhibitor.
Subsequently, cells were immersed in 1 ml of hypotonic F-10 medium
supplemented with inhibitors. After different times, during which the
cells were gently shaken, a 200-µl aliquot was removed and pressure
injected via a light-tight access into a 3-ml glass cuvette containing
50 µl of the ATP assay mix and 1.5 ml of ATP assay mix dilution
buffer (Sigma). Calibration measurements with ATP were performed in a
concentration range of 0-100 nM. The lowest concentration of ATP
that could be detected under the applied experimental conditions was
0.5 nM. From these calibration curves the total picomoles of ATP
released per 105 cells were calculated. Each of the applied
anion channel inhibitors was tested for its effects on the activity of
luciferase enzyme activity. No significant effects of the compounds on
luciferase enzyme activity were observed. Furthermore, dilution of F-10
cell culture medium to yield an osmolality of 150 mosmol/kgH2O did not affect luciferase activity
(n = 3 for each experimental condition) (see Fig.
1). The chemiluminescence output curve
was integrated, and the resulting values were set in relation to the
calibration curve. To correlate ATP release to the cell number, the
cells from which ATP release had been determined were enzymatically dissociated with a 0.2% trypsin-0.05% EDTA solution, and the
cells were counted using an automated cell counter (Cell Analyzer Casy 1, Schärfe System, Reutlingen, Germany).
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Fluorescence recovery after photobleaching. Cell cultures were incubated with 20 µM 5-CFDA for 20 min and postincubated in the absence of 5-CFDA for a further 10 min. Excitation of 5-CFDA was provided by the 488-nm line of the argon ion laser of the confocal setup. Emission was recorded using a long-pass LP 515 filter set. Single cells were selected using an overlay mask. 5-CFDA fluorescence was photobleached in the selected cells using the "point scan" mode of the confocal setup. By switching the attenuation filter wheel of the confocal setup, we elevated the laser power from 0.125 to 12.5 mW for 3 s, which resulted in photobleaching of the dye. After photobleaching, the microscope settings were returned to the recording configuration, and fluorescence recovery in the photobleached cell was monitored every 10 s.
Ca2+ imaging and confocal laser scanning microscopy. Measurement of Cai2+ was performed using the fluorescent Ca2+ indicator fluo 3-AM. Cells adherent to 20 × 20-mm-diameter glass coverslips were incubated for 60 min at 37°C in cell culture medium containing 10 µM fluo 3-AM dissolved in dimethylsulfoxide (final concentration 0.1%) and Pluronic F-127 (final concentration <0.025%; Molecular Probes). After loading, the coverslips were rinsed in E1 buffer containing (in mM) 135 NaCl, 5.4 KCl, 1.8 CaCl2, 1 MgCl2, 10 glucose, and 10 HEPES (pH 7.4 at 37°C) and mounted to the bottom of an incubation chamber that was fixed to the table of an inverted confocal laser scanning microscope (LSM 410, Zeiss, Jena, Germany). Fluorescence was excited by the 488-nm line of an argon-ion laser. Emission was recorded using a long-pass LP 515 filter set. The experiments were performed with a ×25 objective (NA 0.85; Neofluar, Zeiss). Processing of images was carried out with the Time software facilities of the confocal setup. The minimum, maximum, mean, standard deviation, and integrated sum of the pixel values in a region of interest (selected using an overlay mask) were written to a data file and routinely exported for further analysis to the commercially available SigmaPlot (Jandel Scientific, Erkrath, Germany) graphics software. Data are presented in arbitrary units as percentages of fluorescence variation (F/F0) with respect to the resting level fluorescence (F0).
For the quantification of Cai2+ concentrations, calibration experiments were performed as described previously (22), assuming a dissociation constant of 1,100 nM at vertebrate ionic strength. Cai2+ waves were induced by stimulating a group of 8-10 cells with a blunt-end (tip diameter 50 µm) borosilicate glass pipette affixed to a Narishige micromanipulator (Narishige International, Tokyo, Japan). Images were recorded in 1-s intervals. Conduction velocities of Cai2+ waves were measured by determining the distance and the amount of time required for the wave to spread from the mechanically stretched cells (0 µm) to cells within a distance of 100 and 200 µm, respectively.Statistical analysis. Data are given as means ± SE, with n denoting the number of experiments. Student's t-test for unpaired data was applied as appropriate. A value of P < 0.05 was considered significant.
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RESULTS |
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DU-145 prostate cancer cells propagate
Cai2+ waves upon mechanical
strain.
When confluent cells of the prostate cancer cell line DU-145 were
mechanically stimulated with the tip of a glass pipette, a transient
rise of Cai2+ from 109 ± 38 nM
(n = 16 cells in 5 independent experiments) under
resting conditions to 440 ± 61 nM (n = 17 cells
in 5 independent experiments) upon mechanical strain occurred with a
delay of 1-3 s after the cell membrane was stretched
(n = 8) (Fig.
2A). The Cai2+ signal spread radially from the stretched
area with a velocity of ~15 µm/s and declined within a distance of
200-300 µm. Cai2+ waves could be elicited
from the same stretched area up to three times (n = 3)
(Fig. 2B), indicating that cell membranes were not ruptured
during mechanical stimulation. However, the distance covered by the
Cai2+ wave declined with repetitive mechanical
strain. After two periods of mechanical strain of the same cell area, a
third application of mechanical strain elicited a transient
Cai2+ response that was restricted to the
stretched area but did not spread to more distant parts of the
coverslip. The absence of Cai2+ wave propagation
was not caused by the desensitization of purinergic receptors upon
mechanical strain because exogenous addition of 10 µM ATP elicited a
pronounced transient Cai2+ response
(n = 3) (Fig. 2C). Furthermore,
Ins(1,4,5)P3
consumption following repetitive mechanical strain could be excluded
because 50 µM histamine, which uses the
Ins(1,4,5)P3
signal transduction pathway, transiently raised
Cai2+ in the cell area that had been stretched
three times (n = 4) (Fig. 2D).
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Wave propagation is not dependent on membrane potential,
extracellular Ca2+, an intact
microfilament/microtubular network, or functional gap junctions.
To evaluate whether the mechanism for wave propagation was a
strain-induced membrane depolarization, cells were superfused with a
solution containing 140 mM K+ to depolarize the membrane
potential. Figure 3A shows
that under these conditions wave propagation and the amplitude of the
Cai2+ response in the mechanically stretched
cell area (see Fig. 3G) were not impaired (n = 3). Because superfusion with high-K+ solution in the
absence of mechanical strain did not raise
Cai2+, we concluded that no voltage-dependent
Ca2+ channels were present in DU-145 cancer cells (data not
shown). The source of the Cai2+ response
following mechanical strain was further evaluated by superfusion with
nominally Ca2+-free solution. Figure 3B
demonstrates that under this experimental condition neither wave
propagation nor the amplitude (see Fig. 3G) of the
Cai2+ response in the mechanically stretched
cell area was impaired, suggesting an involvement of intracellular
Ca2+ stores in the Cai2+ response
elicited by mechanical stimulation (n = 3). After
preincubation with thapsigargin, which depletes intracellular
Ca2+ stores and inhibits the Ca2+-ATPase of the
sarcoplasmic reticulum (42), Cai2+
wave propagation upon mechanical strain was abolished
(n = 3) (Fig. 3C) and the amplitude (see
Fig. 3G) of the Cai2+ response in the
mechanically stretched cell area was significantly reduced to 169 ± 60 nM (n = 3).
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Involvement of purinergic receptor activation in the propagation of
mechanical strain-induced
Cai2+ waves.
Cai2+ wave propagation has been recently shown
to be mediated by purinergic receptor activation (21). The
presence of P2Y2 receptors in the DU-145 prostate cancer
cell line used in the present study has been previously demonstrated
(46). To investigate the types of purinergic
receptors present in DU-145 cells in more detail,
Cai2+ transients following treatment with 10 µM ATP (Fig. 5A), UTP (Fig.
5B), ADP (Fig. 5C), UDP (Fig. 5D),
2-MeS-ATP (Fig. 5E), or Bz-ATP (Fig. 5F) were
recorded. All applied reagents elicited a transient
Cai2+ response in DU-145 cells, suggesting the
presence of multiple P2 receptors in DU-145 prostate cancer cells
(n = 3 for each experimental condition).
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Inhibition of Cai2+ waves
by anion channel inhibitors.
It has been previously demonstrated that ATP is secreted via anion
channels. CFTR or P-glycoprotein has been described as a possible
candidate for ATP release (1, 32). It is,
however, also likely that other, not-yet-characterized volume-sensitive anion channels are able to conduct ATP. To evaluate a possible role of
anion channels for the mediation of ATP release, DU-145 cells were
incubated for 10 min with NPPB (100 µM; n = 8) (Fig. 8A), DIDS
(500 µM; n = 10) (Fig. 8B), niflumic acid
(100 µM; n = 5) (Fig. 8C), or tamoxifen
(50 µM; n = 8) (Fig. 8D). The latter compound is known to inhibit anion channels but, in addition, exerts
inhibitory effects of protein kinase C (34). Additionally, cells were treated with gadolinium (n = 5) (Fig.
8E), which is known to be an antagonist of stretch-activated
cation channels but has also been described to inhibit
Ca2+-activated (43) and stretch-activated
Cl
channels (33, 48). All
applied anion channel blockers inhibited Cai2+
wave propagation upon mechanical strain. However, a
Cai2+ transient not significantly different in
amplitude compared with the control was observed in the cell area
mechanically distorted by the patch pipette (Fig. 8I). To
evaluate a possible role of CFTR and P-glycoprotein in ATP release,
cells were preincubated for 10 min with verapamil (90 µM) (Fig.
8F) and quinidine (50 µM) (Fig. 8G), which
inhibit P-glycoprotein-associated Cl
channels, as well as
with glibenclamide (100 µM) (Fig. 8H), which inhibits
CFTR. However, none of these agents impaired
Cai2+ waves elicited upon mechanical strain
(n = 3 for each experimental condition).
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ATP release via Cl
channels following hypotonic
incubation.
To obtain stronger evidence of a mechanism of ATP release,
bioluminescence experiments were performed to directly access the amount of released ATP in the supernatant. In this series of
experiments, mechanical strain was applied by incubating cells in
hypotonic medium, and aliquots of the supernatant were analyzed.
Incubation of DU-145 cells in hypotonic medium increased the medium
concentration of ATP within 10 s. Maximum ATP was yielded within 2 min, whereas longer incubation times resulted in a gradual decay of the
ATP concentration, presumably because of ATP consumption or degradation (Fig. 9A). The effects of
anion channel inhibitors were evaluated after 2 min of hypotonic
incubation (Fig. 9B). The absolute amount of ATP released
within 2 min after swelling was 1.57 ± 0.5 pmol/105
cells (n = 8). Preincubation of cells for 10 min with
niflumic acid (100 µM; n = 3), NPPB (100 µM;
n = 3), tamoxifen (50 µM; n = 4), and
gadolinium (100 µM; n = 3) reduced ATP release by 51 ± 7%, 87 ± 4%, 84 ± 5%, and 55 ± 12%,
respectively. It has been previously estimated that the local ATP
concentration at the plasma membrane upon hypotonic stimulation should
be in the micromolar range (25). Concentrations of
externally added ATP exceeding 1 µM elicit transient
Cai2+ responses in DU-145 cancer cells (M. Wartenberg, unpublished results). Interestingly, DIDS (500 µM;
n = 3) did not significantly impair ATP release
following hypotonic incubation.
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DISCUSSION |
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The present study reports on Cai2+ waves elicited by mechanical strain in confluent prostate DU-145 cancer cells. The mechanism of wave propagation did not operate via diffusion of Ins(1,4,5)P3 or Ca2+ through gap junctional pores because chemical uncoupling of cells did not impair wave propagation and because FRAP experiments revealed that gap junctional coupling in DU-145 cells was marginal. This observation is in line with recent results of Carruba et al. (6a), who investigated cell-cell communication in different cultured human prostate tumor cell lines and demonstrated only minor intercellular communication in these preparations. The transient Cai2+ response was apparently mediated by Ca2+ release from intracellular stores because it persisted in nominally Ca2+-free solution but was abolished after store depletion with the Ca2+-ATPase inhibitor thapsigargin. The signal transduction pathway connecting the primary stretch site and the intracellular Ca2+ store, furthermore, did not require an intact cytoskeleton because pretreatment with cytochalasin B, which destroys the microfilament network, and nocodazole, which depolymerizes microtubules, were without any effect on wave propagation.
The data of the present study strongly support the notion that the mechanism underlying wave propagation operated via ATP release, because receptor desensitization with exogenous nucleotides, incubation with suramin and basilen blue (which are antagonists of purinergic receptors), intracellular ATP depletion by preincubation with 2-deoxyglucose, and the presence of apyrase in the incubation medium abolished the observed effects.
The secreted ATP may subsequently stimulate multiple purinergic P2 receptors, which were demonstrated to be present in DU-145 cells. Interestingly, a synergism of different purinergic receptors seems to be necessary for the initiation of wave propagation, because receptor desensitization with agonists of P2Y subtypes and P2X receptors abolished wave propagation upon mechanical strain. This finding indicates that the activation of multiple receptors is required for Ca2+ wave propagation and explains why the inhibition of PLC, which is involved in the Ins(1,4,5)P3 signaling pathway following binding of nucleotides to subtypes of P2Y receptors, abolished wave propagation despite the possible presence of P2X receptors in the investigated cell line. It should, however, be mentioned that the nucleotides used in the present study are not conclusively selective and that a contamination of the commercial preparations with either ATP or UTP could not be excluded. Interestingly, under most conditions in which Ca2+ wave propagation was inhibited, a transient Cai2+ response persisted in the cell area that was mechanically distorted by the glass pipette. This points toward the notion that Ca2+ wave initiation in the stretched cell area may operate via a direct Ins(1,4,5)P3 release from the plasma membrane upon mechanical strain. Strain-induced increases of Ins(1,4,5)P3 have been previously reported for several preparations (13, 15), and the possibility that PLC may act as a mechanotransducer mediating Ins(1,4,5)P3 generation following mechanical perturbation has been discussed (4, 18, 41). Because in the DU-145 cell line used in the present study, Ins(1,4,5)P3, due to the absence of gap junctional communication, cannot diffuse to neighboring cells. The Cai2+ response remained restricted to the stretched cell area. It was furthermore observed that the Cai2+ transient in the stretched cell area was significantly reduced in amplitude after preincubation with ATP and UTP, which involves the Ins(1,4,5)P3, signal transduction pathway, whereas it remained unchanged when cells were pretreated with ADP, UDP, 2-MeS-ATP, or Bz-ATP. This points toward the notion that ATP and UTP desensitized purinergic receptors in the stretched cell area more efficiently than the latter nucleotides and argues against the notion that Ins(1,4,5)P3 had been consumed by the externally added purinergic receptor agonists. Whereas externally added nucleotides apparently inhibited wave propagation via receptor desensitization, inactivation of receptors did not occur after repetitive mechanical strain, because addition of ATP to the incubation medium elicited a transient Cai2+ response. Furthermore, depletion of intracellular Ins(1,4,5)P3 by repetitive stimulation could be obscured because histamine transiently raised Cai2+ in all cells under investigation, including the cells that had been stretched by the glass pipette. We therefore concluded that the lack of wave propagation following repetitive mechanical strain was caused by depletion of intracellular ATP in the stretched cell area.
There is increasing evidence for extracellular pathways of
Ca2+ wave propagation and intercellular communication based
on ATP release. Ca2+ wave propagation via ATP release has
been previously reported for rat mast cells and basophil leukemic cells
(27), hepatocytes (38), osteoblastic cell
lines (21), C6 glioma cells, HeLa cells, and U373
glioblastoma cells (12). Furthermore, ATP release following mechanical strain or hypotonic swelling has been demonstrated for several preparations, including urinary bladder epithelial cells
(14), guinea pig ileal smooth muscle (24),
hepatoma cells (45), tracheal epithelial cells
(26), and red blood cells (40). The
physiological significance of ATP release has not yet conclusively been
unraveled. However, the possibility that ATP release mediated by
hypotonic stimulation of ciliary epithelial cells may modulate aqueous
humor flow by paracrine and/or autocrine mechanisms within the two cell
layers of this epithelium (25) has been discussed. In
liver cells (45) and bilary epithelial cells
(35), recovery from swelling is mediated by an autocrine
pathway involving conductive release of ATP. In endometrial,
intestinal, and epididymal epithelial cells, regulation of
Cl
release is mediated by extracellular ATP
(8, 18). The ATP release observed in urinary
bladder epithelial cells by changes in hydrostatic pressure has been
suggested as a sensory mechanism for the degree of distension of the
urinary bladder (14). A similar sensor mechanism may be
true in prostatic epithelial tissues.
In the present study ATP release was significantly inhibited by the
Cl
channel blockers tamoxifen, NPPB, niflumic acid, and
gadolinium. Consequently, propagation of Ca2+ waves was
inhibited in the presence of anion channel inhibitors. This points
toward the notion that ATP released through Cl
conductive
pathways by mechanical strain activates P2 receptors in the plasma
membrane. This results in transient Cai2+
responses in cells that are distant to the area directly touched by the
glass pipette. Interestingly, DIDS inhibited
Cai2+ wave propagation but did not impair ATP
release upon hypotonic stimulation. An increase of ATP release in the
presence of DIDS following hypotonic incubation has been recently
reported (25) and has been interpreted as inhibition of
ecto-ATPases, which rapidly degrade extracellular ATP. The inhibitory
effects of DIDS on Cai2+ wave propagation
therefore may be explained by its previously demonstrated effect as an
antagonist of purinergic receptors (5, 11,
29).
The molecular mechanisms of ATP release are still a matter of debate.
Some evidence suggests that ATP release from mammalian epithelial cells
can proceed through members of the ATP-binding cassette family of
proteins such as the cAMP-activated CFTR or P-glycoprotein, which plays
a pivotal role in multidrug resistance (1, 6,
28, 30, 32, 38).
These observations have been challenged by others (16,
23, 31, 47). In the present study these pathways were excluded because the P-glycoprotein antagonist cyclosporin A (data not shown) and the 4E3 antibody, which
is directed against an extracellular domain of the transporter (data
not shown), as well as verapamil and quinidine, which inhibit the
P-glycoprotein-associated Cl
conductance, failed to
inhibit wave propagation. Likewise, glibenclamide, which interferes
with CFTR Cl
channels, was without any affect on wave
propagation. However, it has been recently shown that the permeation
pathway associated with CFTR-modulated ATP release is independent of
the Cl
conductance pathway in the channel pore
(20). A comparable mechanism may likewise hold true for
P-glycoprotein. Because it has been recently demonstrated that CFTR may
regulate other epithelial ion channels such as the epithelial
Na+ channel and the outward rectifying Cl
channel (ORCC), an indirect effect of CFTR and P-glycoprotein on ATP
release through other swell-activated anion channels cannot be
excluded. A recent publication (38) demonstrating that
CFTR regulates the ORCC through pathways that involve P2Y receptors points in this direction.
The data of the present study support a model by which mechanical
strain raises Cai2+ via
Ins(1,4,5)P3
generation in the cell area touched by the glass pipette. The
mechanical strain opens volume-sensitive Cl
channels,
which either directly release ATP or activate associated, not-yet-described release mechanisms for ATP. The released ATP then
activates P2 receptors in neighboring cells, which results in a
Cai2+ wave that spreads radially from the
stretched cell area. A strain-induced release mechanism for ATP may
provide a sensor for the distension of the prostate tissue.
Furthermore, an autocrine/paracrine model of humor formation, as has
been recently proposed for ciliary epithelial cells (25),
likewise may hold true for prostate epithelial cells. In this model
released ATP is hydrolyzed by membrane ectoenzymes to adenosine, which
stimulates aqueous humor formation by activating Cl
channels in the nonpigmented epithelial cell layer. In the pigmented cell layer, extracellular ATP stimulates aqueous humor formation by
directly activating anion conductances. The purinergic regulation of
anion secretion may involve Cai2+ mobilization
including Cai2+ waves, as has been recently
demonstrated for pancreatic duct cells and retinal pigment epithelium
(7, 28). Cai2+ waves
may provide a means to transduce a localized strain event into an
extended signaling cascade in distant cell layers that are not affected
by the mechanical strain. By this signal transduction cascade,
Cai2+ waves may trigger fluid secretion in the
tissue of the prostate gland.
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FOOTNOTES |
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Address for reprint requests and other correspondence: M. Wartenberg, Dept. of Neurophysiology, Robert-Koch-Str. 39, D-50931 Cologne, Germany (E-mail: hs{at}physiologie.uni-koeln.de).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.
Received 9 August 1999; accepted in final form 16 March 2000.
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