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The Journal of Neuroscience, May 15, 1999, 19(10):3711-3722
A Current Activated on Depletion of Intracellular
Ca2+ Stores Can Regulate Exocytosis in Adrenal Chromaffin
Cells
Alla F.
Fomina and
Martha C.
Nowycky
Department of Neurobiology and Anatomy, Medical College of
Pennsylvania Hahnemann University, Philadelphia, Pennsylvania 19129
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ABSTRACT |
Exocytosis in excitable cells is strongly coupled to
Ca2+ entry through voltage-gated channels but can be
evoked by activation of membrane receptors that release
Ca2+ from inositol 1,4,5-trisphosphate-sensitive
internal stores. In many cell types, depletion of
Ca2+ stores activates Ca2+ influx
across the plasma membrane, a process known as capacitative or
store-operated Ca2+ entry. This influx is mediated
by a number of voltage-independent, Ca2+-selective
currents. In addition to replenishing Ca2+ stores,
these currents are hypothesized to play an important role in
agonist-evoked secretion in nonexcitable cells, although this has not
been confirmed experimentally. The existence and physiological function
of such currents in excitable cells is not known. Using the capacitance
detection technique to monitor exocytosis, we provide direct
experimental evidence that a similar mechanism exists in bovine adrenal
chromaffin cells. Depletion of intracellular Ca2+
stores with thapsigargin, a SERCA pump inhibitor, or with BAPTA, an
exogenous Ca2+ chelator, activates a
small-amplitude, voltage-independent current that is carried by
Ca2+ and Na+ ions.
Ca2+ entry through this pathway is sufficient to
stimulate exocytosis at negative membrane potentials. In addition,
depolarization-evoked exocytosis is markedly facilitated on activation
of the current. These data suggest that excitable cells possess a
store-operated Ca2+ influx mechanism that may both
directly trigger exocytosis and modulate excitation-secretion coupling.
Key words:
exocytosis; calcium-secretion coupling; store-operated
current; capacitance detection; synaptic plasticity; chromaffin cell,
capacitative Ca2+ entry
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INTRODUCTION |
Exocytosis of neurotransmitters,
neuroactive peptides, and hormones at synapses and in excitable
secretory cells is triggered by elevation of intracellular
Ca2+
([Ca2+]i) (Katz, 1962 ; Douglas
and Rubin, 1963 ). Opening of voltage-gated Ca2+
channels constitutes the major pathway for rapid
Ca2+ influx in excitable cells (Augustine et al.,
1987 ). However, alternative pathways can contribute to
Ca2+ elevation, such as Ca2+
influx through ligand-gated ion channels (Mollard et al., 1995 ; Gray et
al., 1996 ) or Ca2+ release from intracellular stores
(Berridge, 1998 ). The relative significance and interactions among
these Ca2+ sources are not well understood.
Adrenal chromaffin cells are developmentally related to sympathetic
neurons, and their main function is the synthesis, storage, and release
of catecholamines. Exocytosis of catecholamine-containing large
dense-cored vesicles is evoked by Ca2+ entry through
voltage-gated channels, but also can be triggered by stimulation of
membrane receptors coupled to inositol 1,4,5-trisphosphate (IP3) formation and Ca2+ release
from intracellular stores (Burgoyne, 1991 ). In voltage-clamped chromaffin cells, exocytosis can be evoked in the absence of
depolarization by photolysis of caged IP3 (Robinson et al.,
1996 ) or by stimulation of membrane receptors with bradykinin
(Augustine and Neher, 1992 ).
In many cell types, [Ca2+]i elevation
in response to IP3-generating agonists is biphasic: an
initial transient rise caused by Ca2+ release from
stores is followed by a second prolonged phase that requires
extracellular Ca2+ influx (Berridge, 1995 ). In some
excitable cells, the prolonged phase can be at least partially
supported by increased activity of voltage-gated
Ca2+ channels (Fomina and Levitan, 1995 ; Li et al.,
1997 ). In nonexcitable cells, partial or complete depletion of
intracellular Ca2+ stores activates
voltage-independent Ca2+ influx ("capacitative
Ca2+ entry") (Putney, 1986 , 1990 ).
Although the signal generated by store-depletion remains elusive,
progress has been made in characterizing capacitative
Ca2+ influx in nonexcitable cells. The best-studied
mechanism is the Ca2+ release-activated
Ca2+ current (ICRAC)
found in mast cells, lymphocytes, and leukemia cells (Penner et al.,
1988 ; Lewis and Cahalan, 1989 ; Hoth and Penner, 1992 , 1993 ).
ICRAC is a small-amplitude, highly
Ca2+-selective current that is activated by various
agents that deplete intracellular Ca2+ stores,
including inhibitors of endoplasmic reticulum
Ca2+/ATPases (SERCA pumps) and high concentrations
of Ca2+ chelators (Fasolato et al., 1994 ; Parekh and
Penner, 1997 ). Several other currents activated on store depletion have
been described in nonexcitable cells that differ from
ICRAC in certain biophysical properties, such as
ion selectivity or kinetics. Collectively, such currents are called
"store-operated currents" (SOCs) (Clapham, 1995 ). The existence of
capacitative Ca2+ entry in secretory excitable
cells, including chromaffin, pituitary, and pancreatic -cells, has
been suggested, but the underlying mechanisms have not been
characterized (Robinson et al., 1992 : Villalobos and Garcia-Sancho,
1995 ; Powis et al., 1996 ; Liu and Gylfe, 1997 ).
In addition to replenishing intracellular Ca2+
stores, SOCs play a critical role in gene expression in nonexcitable
cells (Fanger et al., 1995 ; Dolmetsch et al., 1998 ). It has also been
proposed, although not demonstrated directly, that
Ca2+ influx through SOCs is a central element in
agonist-evoked secretion in mast cells (Zhang and McCloskey, 1995 ).
However, in mast cells, Ca2+ is merely a cofactor
for secretion, and Ca2+ elevation is not strictly
required (Neher, 1988 ). Thus, the significance of SOCs in secretion in
nonexcitable cells remains unclear. In excitable cells, in which the
secretory machinery is highly sensitive to Ca2+, the
role of SOCs has not been studied. Here, we examine the existence,
properties, and functional significance of a SOC in adrenal chromaffin cells.
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MATERIALS AND METHODS |
Electrical recording techniques
Bovine adrenal chromaffin cells were cultured as described
previously (Vitale et al., 1991 ; Engisch and Nowycky, 1996 ). Most recordings were performed with perforated-patch voltage-clamp techniques using an Axopatch 200A amplifier (Axon Instruments, Foster
City, CA) and programs written in Axobasic (Axon Instruments, Foster
City, CA). Experiments were performed at 30°C.
Recording protocols. Time was set to zero on seal formation,
and data acquisition during perforated-patch experiments was initiated
after 5-10 min when the series resistance stabilized at 6-15 M .
The initial cell capacitance ranged from 4 to 8 pF. Exocytosis was
monitored as changes in membrane capacitance
(Cm) using a computer-based
phase-detection technique as described previously (Lim et al., 1990 ;
Seward et al., 1995 ). The membrane potential was held at 90 mV;
Cm and combined membrane and series conductance
(G) values were calculated from sets of 10 sine
waves, 1.2 kHz, 15 mV root mean square. The sets were separated by ~2 msec for data calculation and storage, resulting in a final temporal resolution of ~12 msec per data point. Capacitance data were acquired in 11.8 sec segments; the Cm and G
phase angles were reset at the beginning of each segment. The holding
current (Ihold) was measured at 90 mV
between sets of sine waves. Five measurements of
Ihold at 160 msec intervals were obtained every
11.8 sec. In some experiments, voltage ramp pulses ( 120 to 60 mV,
200 msec duration) were applied every 11.8 sec. In the figures, the
current is shown over the range of 115 to 60 mV to exclude the
capacitative transient. Voltage-gated Ca2+ entry was
evoked by single brief depolarizing pulses ( 90 mV to 10 or +10 mV;
20-80 msec duration) that were administered once every 1-4 min.
Data analysis. For calculation of the rate of
depolarization-independent Cm changes, 200-1000
points of a Cm trace were averaged, and the
resulting plot was then differentiated. Depolarization-evoked exocytosis was calculated as the difference in
Cm value before and after depolarization by
averaging 3 Cm data points. The amount of
Ca2+ influx during depolarization was calculated by
integration of voltage-gated Ca2+ currents using
limits that excluded the voltage-gated Na+ current
and is expressed in charge units (QCa).
Tetrodotoxin (TTX) was not used, because Na+
channels in bovine chromaffin cells are relatively insensitive to TTX,
and TTX contributes a capacitative artifact attributable to slowing of
Na+ channel gating current (Horrigan and Bookman,
1994 ). Holding current is presented as the five-point average and SEM
of current samples obtained at 160 msec intervals within an 11.8 sec segment.
Data analysis was performed with Axobasic programs and Origin 4.1 (Microcal, Northhampton, MA) software. All statistics are presented as
mean ± SEM. The number of experiments reported in the text varies
somewhat, because not all parameters
(FCa, ITg, and Cm) could be successfully measured
in all cells. Early experiments did not monitor
Ihold but are included in statistics for changes in FCa and Cm.
Solutions
Extracellular recording solutions. The recording
solutions consisted of the following (in mM): (1) standard
solution: 55 NaCl, 70 NaOH, 5 Ca(OH)2, 0.8 MgCl2, 20 TEA-OH, 10 HEPES, 10 glucose; (2) low
Ca2+ solution: 55 NaCl, 70 NaOH, 0.5 or 1.0 Ca(OH)2, 5 MgCl2, 20 TEA-OH, 10 HEPES, 10 glucose; (3) low Cl solution: standard
solution with 10 NaCl, 115 NaOH. The pH of external solutions 1-3 was
adjusted to 7.35 with methanesulfonic acid; and (4) nominally
Na+-free solution: standard solution with equimolar
replacement of Na+ with
N-methyl-D-glucamine (NMDG+), pH
adjusted to 7.35 with HCl.
Pipette solutions. (1)For perforated-patch experiments, the
solution consisted of the following (in mM): 130 Cs-glutamate, 10 CsCl, 5 MgCl2, 10 Na-HEPES, pH
adjusted to 7.2 with CsOH (ICN, Aurora, OH). Amphotericin B
(Calbiochem, La Jolla, CA) at a final concentration of 0.4-0.5 mg/ml
(stock solution in DMSO: 125 mg/ml) was used for perforation. (2) For
whole-cell recordings, the solution consisted of the following (in
mM): 130 Cs-glutamate, 2 Mg-ATP, 10 HEPES, 9.5 NaCl, 10 BAPTA, pH adjusted to 7.2 with CsOH.
Thapsigargin (Tg) (Calbiochem, La Jolla, CA) was stored at 20°C for
up to 1 month as a 10 mM stock solution in DMSO. Recording solutions and drugs were applied using a perfusion pipette with a tip
diameter of ~50 µm placed ~50 µm from the cell. Five barrels were inserted close to the pipette tip, and solution exchange was
controlled by manual valves. A complete exchange of solution in the
vicinity of the patched cell was achieved within 5 sec.
Unless otherwise noted, all compounds were from Sigma (St. Louis, MO).
Measurement of Ca2+-sensitive
dye fluorescence
For perforated-patch experiments, cells were preloaded with the
ester forms of nonratiometric (Oregon Green 488 BAPTA-1/AM or Fluo-3
AM; Molecular Probes, Eugene, OR) or ratiometric (fura-2 AM; Molecular
Probes) Ca2+-sensitive fluorescent dyes. The
dye-loading solution contained (in mM): 150 NaCl, 1.8 CaCl2, 0.8 MgCl2, 2.5 KCl, 10 Na-HEPES, 10 glucose, pH 7.3. The culture media was replaced with
loading solution containing 2.5 µl/ml of Oregon Green 488 BAPTA-1/AM
or Fluo-3 AM stock (0.8 mM in DMSO) or 1 µl/ml of fura-2
AM stock (1.5 mM in DMSO) and 5 µl/ml of 10% Pluronic
F-127 solution in DMSO. Cells were incubated with the dye-containing
solution for 10-30 min at 37°C, washed, and then held in the loading
solution for at least 30 min at 37°C to allow cleavage of the
acetoxymethyl ester. Fluorescence images of nonratiometric dyes were
acquired with the Bio-Rad MRC-600 laser scanning confocal imaging
system (Bio-Rad, Hercules, CA) using single wavelength excitation (488 nm line of argon-krypton laser) and a 520 nm long-pass barrier filter
and were processed off-line with NIH Image analysis software. Unless
indicated otherwise, the image sampling interval was 700 msec during
and immediately after depolarizing pulses and 10 sec at other times.
Changes in intracellular Ca2+ are expressed as
fluorescence intensity (F) normalized to the value at
the beginning of the experiment (F0).
Fura-2 fluorescence was monitored using the Multipoint Imaging
Photometer system (Dromaretsky et al., 1997 ) with signal acquisition at
360/380 nm excitation wavelengths every sec. For fura-2 experiments the
ratio F360/F380 is presented.
Dopamine- -hydroxylase immunocytochemistry and
confocal microscopy
Cells were washed in normal recording solution and incubated for
2 min at 37°C in the standard recording solution containing 5 µM Tg or vehicle alone (control). After rinsing three
times with PBS, PBS was replaced with fixative (4%
paraformaldehyde/0.4% saponin in PBS, pH 7.4) for 10 min at room
temperature. Fixed cells were washed three times with PBS and then
incubated for 20 min with 10% goat serum (Jackson ImmunoResearch
Laboratories, West Grove, PA) to reduce nonspecific staining. After
rinsing, cells were labeled with a 1:1000 dilution of polyclonal
anti-dopamine- -hydroxylase (D H) antibodies (Chemicon, Temecula,
CA) for 1 hr and rinsed again with PBS containing 10% goat serum.
Cells were incubated with goat anti-rabbit IgG FITC-conjugated
secondary antibodies (1:200, Jackson ImmunoResearch Laboratories) for 1 hr. Nonspecific fluorescence was assessed by incubating cells with the
secondary fluorescent antibodies only. After fluorescent labeling,
cells were rinsed three times with 10% goat serum and PBS, preserved under 4% p-phenylenediamine in glycerol, and stored at
20°C until examination.
Immunofluorescent staining was visualized with a Bio-Rad MRC-600 laser
scanning confocal imaging system (see above) with a 63× oil objective
(numerical aperture 1.4). Single confocal sections were taken with
pin-hole aperture settings of 2 at the plane of maximal nuclear
diameter. FITC emission was excited using the argon laser 488 nm line
and filtered with a 520 nm long-pass barrier filter. Images of randomly
selected cells from stimulated and control groups were recorded at the
same settings, and the average fluorescence intensity value was measured.
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RESULTS |
To investigate the presence and potential physiological role of a
capacitative Ca2+ entry pathway in adrenal
chromaffin cells, we combined voltage clamp and fluorometric techniques
to monitor simultaneously membrane conductance, intracellular
Ca2+
([Ca2+]i), and exocytosis in
single bovine chromaffin cells. To preserve essential cytoplasmic
regulatory elements, most experiments were performed using the
perforated-patch-clamp method (Rae et al., 1991 ) at elevated
temperature (~30°C). Changes in
[Ca2+]i were monitored by measuring
the fluorescence of a Ca2+-sensitive dye preloaded
into the cells (FCa). Exocytosis was assayed with a software-based capacitance detection technique as
changes in cell surface area ( Cm)
(Neher and Marty, 1982 ; Joshi and Fernandez, 1988 ; Fidler and
Fernandez, 1989 ). Intracellular Ca2+ stores were
depleted with Tg, which inhibits SERCA pumps and thereby prevents the
reuptake of cytoplasmic Ca2+ passively released from
the stores in many cell types, including bovine chromaffin cells
(Thastrup et al., 1990 ; Robinson and Burgoyne, 1991 ; Zerbes et al.,
1998 ).
Thapsigargin-induced changes in membrane conductance, intracellular
Ca2+, and exocytosis
Tg application (1-5 µM) activated a relatively
small amplitude inward current at negative holding potentials (Fig.
1A,
Ihold) and produced a rise in
FCa (Fig. 1A,
F/F0) in 23 of 31 cells. The onset of the
Tg-activated current (ITg) and the rise
in FCa were simultaneous within the limits of
our experimental resolution (~10 sec) and usually began 1-2 min
after Tg application (Fig. 1C). ITg
often had complex kinetics with periodic partial declines in amplitude.
These slow current oscillations were correlated with oscillations in
the FCa signal. ITg
reached a maximal value after several minutes that, on average, was
15.2 ± 2.7 pA at 90 mV (n = 18; here and
elsewhere, n = number of cells where the
parameter of interest could be accurately measured).
ITg inactivated fully in the continuous presence
of Tg, returning to the prestimulatory level within several minutes;
FCa declined with a similar time course.
Subsequent application of higher doses of Tg resulted in reactivation
of ITg and produced an additional rise in
FCa (data not shown). Voltage-gated
Ca2+ currents that evoked large-amplitude
FCa transients (Fig. 1A-C, vertical bars) never elicited
ITg-like inward currents either before or after
Tg application, suggesting that ITg is not
activated by a rise in [Ca2+]i.

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Figure 1.
Effects of thapsigargin on intracellular
[Ca2+], membrane conductance, and exocytosis.
Simultaneous recordings in individual cells of
Ca2+-sensitive dye fluorescence
(FCa), current at 90 mV
(Ihold), and changes in membrane
capacitance ( Cm). Vertical
bars indicate timing of depolarizing pulses. In standard
recording solution, brief depolarizations evoked voltage-gated
Ca2+ currents, rapid FCa
transients, and abrupt increases in Cm (also
see Fig. 2A,B) that reflect exocytosis of
catecholamine-containing large dense-cored vesicles (Chow et al., 1992 ;
Engisch and Nowycky, 1998 ). A, Tg application induced a
rise in FCa
(F/F0), activated a transient inward
current (Ihold), and evoked
depolarization-independent exocytosis
( Cm). The bottom
panel is the calculated rate of depolarization-independent
exocytosis (Rate). Tg (2.5 µM) was applied
continuously as indicated. Fluorescent dye: Oregon Green BAPTA-1 AM.
B, Tg application activated an inward current that was
not accompanied by changes in FCa or
depolarization-independent exocytosis
( Cm). Panels as in
A. Tg (0.2 µM Tg) was applied as
indicated. Slow Cm drifts (maximal rate <1
fF/sec) were often observed during prolonged recording (Engisch and
Nowycky, 1998 ) but had no consistent correlation with Tg application.
In this particular experiment, the fluorescence signal was sampled
every 20 sec; therefore, the FCa responses
to depolarizations are truncated. Fluorescent dye: Fluo-3 AM.
C, Superimposed traces from
1A of FCa ( ),
Ihold on a reversed axis ( ), and
Cm (line) on an expanded
time scale. Cm and
Ihold values were normalized to the maximal
values after Tg application and are presented on the same scale. The
FCa trace was scaled to match the time
course of the initial rise of ITg.
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In all cells with a Tg-induced rise in
FCa, the cell surface area increased in
the absence of voltage-gated Ca2+ entry (Fig.
1A,C, Cm)
(n = 23). The onset of the Cm
increase was clearly delayed relative to the onset of
ITg and rise in FCa (42.9 ± 8.32 sec; n = 18) (Fig. 1C;
also see Fig. 4B). Depolarization-independent exocytosis proceeded at a slow rate (17.3 ± 4.3 fF/sec,
n = 16) but was substantial (930.1 ± 187.9 fF,
n = 10, compare with 4-8 pF initial cell capacitance).
The Cm increase often terminated before the
decline of FCa and
ITg, and the total
Cm increase may be underestimated because of
contaminating endocytosis. The occurrence and kinetics of endocytosis
were variable, had no obvious correlation with changes in
ITg or FCa, and
were not analyzed further.
In a subset of experiments, ITg was activated
without a concurrent rise in global FCa (Fig.
1B) (8 of 31 cells at [Tg] from 1 to 5 µM and 4 of 11 cells at [Tg] from 0.1 to 1 µM). In these cells, ITg was
smaller, with a maximal current increase over control levels of ~5
pA. The kinetics were more complex as the current periodically decayed
to the prestimulatory levels, but current oscillations persisted for
the duration of the experiment (Fig. 1B,
Ihold). Depolarization-independent
exocytosis was never detected when Tg application failed to evoke a
global FCa rise (n = 12 of 12).
In these cells, Cm increases were detected only
in response to depolarizations that activated voltage-gated
Ca2+ channels (Fig. 1B).
Exocytosis evoked by voltage-gated Ca2+ entry was
potently enhanced in all cells in which ITg was
activated (Fig. 2) (n = 35). In control conditions, changes in Cm evoked
by brief depolarizations (20-80 msec) were small (10-50 fF) (Fig.
2A,B; same cells as in Fig. 1A,B,
respectively), and the relationship between
Cm and the amount of voltage-gated
Ca2+ influx (QCa) was
satisfactorily described by a linear function over this restricted
range of stimulus parameters (Fig. 2C,D). After Tg
application, Cm responses were enhanced,
despite a reduction in the amplitude of voltage-gated
Ca2+ currents (Fig. 2A,B). The
facilitated responses were substantially larger than predicted by the
linear Cm/QCa
relationship (Fig. 2C,D). Facilitation had a different time
course and magnitude in cells with (Figs. 1A,
2A) and without (Figs. 1B,
2B) a detectable rise in FCa.
In cells with an FCa rise, both
ITg and facilitation were transient, subsiding
by 9-12 min (Fig. 2E). Before Tg application, the
Ca2+ efficacy
( Cm/QCa)
was ~1.5 fF/pC. Maximal facilitation occurred at ~3 min, where the
average Cm/QCa
value was >10 fF/pC. In cells without a detectable
FCa rise, both ITg and
facilitation were sustained even at 20 min after Tg application (Fig.
2F). The average maximal efficacy of ~4 fF/pC was
reached after ~5-6 min. Thus, in both groups of cells, the time
course of facilitation corresponded to that of
ITg, and the magnitude of facilitation
was approximately proportional to the current amplitude.

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Figure 2.
Facilitation of depolarization-evoked exocytosis
by thapsigargin. A, B, Capacitance
changes ( Cm, top
traces) and corresponding voltage-gated Ca2+
currents (ICa, bottom
traces) evoked by depolarizations before and after application
of Tg (2.5 µM in A; 0.2 µM
in B) on an expanded time scale. Data from the same
cells as in Figure 1 A,B. Numbers in
parentheses above the Cm traces
indicate the corresponding depolarizations in Figure 1,
A and B, respectively. C,
D, Relationship between the depolarization-evoked
Ca2+ influx expressed in charge units
(QCa) and corresponding capacitance
changes ( Cm) before ( ) and
after ( ) application of 2.5 µM [C(3)]
or 0.2 µM (D) Tg. Single
depolarizations to +10 and 10 mV, 40 msec duration, separated by 3-4
min intervals, were given before Tg to establish the
Cm/QCa
relationship in control conditions. The straight line is
the linear regression fit for control data obtained by minimizing
2. After Tg application all depolarizations were to +10
mV, 40 msec duration. The reduced QCa values
are caused by inhibition of voltage-gated Ca2+
currents by Tg. Similar reduction of amplitude of voltage-gated
Ca2+ currents has been described previously for
other cell types (Nelson et al., 1994 ; Buryi et al., 1995 ).
E, F, Averaged time courses of Tg-induced
changes in
Cm/QCa
values ( ) and ITg ( ).
E, Data from 14 cells in which Tg application produced a
rise in FCa and triggered
depolarization-independent exocytosis. F, Data from 12 cells in which Tg evoked an inward current but did not cause a
detectable rise in FCa and did not trigger
depolarization-independent exocytosis.
Cm/QCa
points are the mean ± SEM values of four to six measurements from
different cells that fell within a given 1 min interval.
Ihold values were calculated by first
averaging all current samples for each cell at 1 min intervals (see
Materials and Methods) and then determining the mean ± SEM for
all cells. In F, the number of experiments declined from
12 at time = 0 to 4 at time = 22 min because of the loss of
gigaseals during prolonged recordings.
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Mechanisms underlying thapsigargin-induced modulation
of exocytosis
We consistently observed depolarization-independent exocytosis in
all cells in which global [Ca2+]i was
elevated by Tg application. The lack of an FCa
rise in cells with a small amplitude ITg might
indicate that Tg-induced Ca2+ discharge from the
stores and/or Ca2+ influx are compensated by other
uptake, extrusion, or buffering systems. Facilitation of
depolarization-evoked exocytosis in these cells, however, suggests that
local, submembrane Ca2+ changes may occur even in
the absence of a detectable FCa rise. We tested
whether the major source of Ca2+ underlying the
FCa rise and the depolarization-independent
exocytotic response was intracellular or extracellular.
To examine the contribution of Ca2+ released from
intracellular stores, Tg was applied in external solutions containing
low Ca2+. Exchange to a nominally
Ca2+-free external solution (no added
Ca2+) caused the appearance of a large-amplitude,
inward current. This resembled a current described by Armstrong and
Lopez-Barneo (1987) in squid neurons that is thought to arise from the
loss of gating and selectivity of voltage-gated ion channels in
Ca2+-free solution. Low concentrations of
Ca2+ prevented the appearance of this current and
were used in all further perforated-patch experiments.
Exchange from normal (5 mM) to low Ca2+
(0.5 mM) external solution resulted in a rapid decline in
the FCa signal (data not shown). This is
probably attributable to a combination of a decrease in the driving
force for Ca2+ entry through leak channels
(Obejero-Paz et al., 1998 ) and the activity of a number of
Ca2+ extrusion mechanisms, including the Na-Ca
exchanger and plasma membrane Ca2+ pump (Chern et
al., 1992 ). When cells were exposed to a low Ca2+
solution containing high doses of Tg (5-14 µM), there
was an initial decline in the FCa signal,
followed by a delayed, slow rise in FCa that did
not reach levels recorded before solution exchange (Fig.
3). The small rise in
FCa probably reflects Ca2+
accumulation after block of Ca2+ reuptake by Tg.
However, it was not associated with detectable activation of
ITg or a significant increase in
Cm. Thus, under our experimental conditions,
passive discharge from intracellular stores is not sufficient to
elevate [Ca2+]i above control levels
or to initiate depolarization-independent exocytosis, even in the
presence of very high concentrations of Tg.

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Figure 3.
Effects of thapsigargin in
low-Ca2+ external solution on intracellular
[Ca2+], membrane conductance, and exocytosis.
Simultaneous recordings of FCa
(F/F0), current at 90 mV
(Ihold), and capacitance changes
( Cm) in a single cell. The
bottom panel is the calculated rate of
depolarization-independent exocytosis (Rate).
Low-Ca2+ solution (0.5 mM) containing Tg
(8 µM) was applied as indicated; vertical
bars indicate timing of depolarizations. The
FCa signal declined rapidly in
low-Ca2+ solution, and depolarizations no longer
produced an FCa rise or exocytosis because
of the reduction of voltage-gated Ca2+ currents.
Fluorescent dye: Oregon Green BAPTA-1 AM.
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If the FCa rise and exocytotic responses are
caused by extracellular Ca2+ entry,
ITg may be the Ca2+-carrying
current. In this case, pharmacological block of
ITg or lowering of extracellular
Ca2+ should inhibit
[Ca2+]i elevation and exocytosis. To
test this hypothesis, we varied the composition of the external
solution after activation of ITg in normal
recording solution. Only cells that responded to Tg with a detectable
rise in FCa were included in the analysis.
Zn2+ is an inorganic blocker of SOCs in mast cells
and other nonexcitable cells (Hoth and Penner, 1993 ; Zhang and
McCloskey, 1995 ), but it has little direct effect on the exocytotic
mechanisms of permeabilized bovine chromaffin cells when applied at
millimole concentrations (Tomsig and Suszkiw, 1996 ). All Tg-induced
responses were reversibly blocked by extracellular application of
Zn2+ (2-4 mM, n = 8).
Figure 4A,B illustrates
a cell with typical FCa,
Ihold, and Cm
responses to Tg. On Zn2+ application, both
ITg and depolarization-independent exocytosis ceased abruptly, whereas FCa declined more
slowly (Fig. 4A). During voltage ramps,
ITg exhibited a linear current-voltage
(I-V) relationship between 120 and 60 mV, and
Zn2+ blocked the current throughout this potential
range (Fig. 4C). Return to control solutions resulted in an
abrupt increase in ITg that was correlated with
rapid increases in FCa and exocytosis. The
amplitude of ITg after washout of
Zn2+ was always much greater than in Tg alone (Fig.
4A) ( 151.6 ± 24.2 pA; n = 8),
and the current was blocked by reapplication of
Zn2+. The cause of ITg
enhancement is not understood, but it was correlated with a
substantially greater rate of exocytosis (83.5 ± 22.7 fF/sec, n = 7), suggesting that the rate of exocytosis may be
proportional to the amplitude of ITg.

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Figure 4.
Inhibition by Zn2+ of the
thapsigargin-induced increase in intracellular
[Ca2+], inward current, and exocytosis.
A, Simultaneous recordings of
FCa
(F/F0), current at 90 mV
(Ihold), and capacitance changes
( Cm) in a single cell. The
bottom panel is the calculated rate of
depolarization-independent exocytosis (Rate). Tg (2.5 µM) and Zn2+ (2 and 4 mM)
were applied as indicated. Vertical bars indicate timing
of depolarizations. Fluorescent dye: Oregon Green BAPTA-1 AM.
B, Superimposed traces of FCa
( ), Ihold on a reversed axis ( ), and
Rate (dashed line) on an expanded time
scale. For scaling information, see Figure 1C.
C, Currents recorded during voltage ramps from 120 to
60 mV, 200 msec duration, before Tg application
(Control), 2 min after Tg (2.5 µM Tg), and 1 min after addition of 2 mM
Zn2+ (2.5 µM Tg, 2 mM Zn2+). Each trace is the average
of three ramps. Activation of ITg was
consistently associated with an increase in current noise.
|
|
Substitution of Na+ in the external solution with
NMDG+ reduced the amplitude of
ITg by 58.2 ± 6% (Fig.
5A) (n = 10).
This effect is clearly seen in the I-V relationship during
a ramp from 120 to 60 mV (Fig. 5B) and indicates that a
fraction of ITg is carried by
Na+ ions. Despite the reduced current amplitude, the
FCa signal usually exhibited an additional rise
in Na+-free solution (9 of 10 substitutions). The
increases in FCa are consistent with a reversal
or block of the Na-Ca exchanger (Pan and Kao, 1997 ). In normal
recording solutions, an active Na-Ca exchanger would generate an
inward current at negative potentials that might contribute to
ITg but would tend to lower
[Ca2+]i. In some cells, the rate of
increase of Cm was slightly enhanced on
exchange to Na+-free solution. However, the effect
of Na-Ca exchange on exocytosis is beyond the scope of the present
study and was not pursued further.

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Figure 5.
Effects of nominally Na+-free
solution on intracellular [Ca2+],
ITg, and exocytosis.
A, Simultaneous recordings of
FCa
(F/F0), current at 90 mV
(Ihold), and capacitance changes
( Cm) in a single cell. The
bottom panel is the calculated rate of
depolarization-independent exocytosis (Rate). Tg (5 µM) was applied as indicated. The horizontal dark
bar indicates exchange for nominally
Na+-free solution; vertical bars
indicate timing of depolarizations. Note the small rise in the
FCa signal when Na+-free
solution is applied. Fluorescent dye: Oregon Green BAPTA-1 AM.
B, Current recorded during voltage ramps from 120 to
60 mV, 200 msec duration, before Tg application
(Control), after Tg application in standard
recording solution (5 µM Tg, 150 Na+), and after exchange with nominally
Na+-free external solution (5 µM
Tg, 0 Na+). Each trace is the average of three
ramps.
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|
Application of a Na+-free,
low-Ca2+ (0.5-1 mM) solution decreased
the total inward current (not leak-subtracted) by 82 ± 6%
(n = 3), which reduced Ihold to
values even lower than before Tg application (Fig.
6). Simultaneously with
ITg inhibition, FCa declined, and the rate of depolarization-independent exocytosis was
reduced (Fig. 6). All effects were reversed on return to standard recording solution. Perfusion with low Cl external
solution (10 mM Cl ; see Materials and
Methods) had no effect on ITg,
FCa, or exocytosis (n = 3; data not shown), confirming that ITg is a
cation-selective current.

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Figure 6.
Effects of Na+-free,
low-Ca2+ extracellular solution on the
thapsigargin-induced changes in intracellular
[Ca2+], ITg, and
exocytosis. Plots are of ratio of fura-2 AM fluorescence at 360 and 380 nM excitation wavelengths
(FCa), current at 90 mV
(Ihold), and capacitance changes
( Cm) in a single cell. The
bottom panel is the calculated rate of
depolarization-independent exocytosis (Rate). Tg (2.5 µM) was applied as indicated. The horizontal dark
bars indicate exchange first for nominally
Na+-free solution with 5 mM
Ca2+, then for Na+-free solution
with 1 mM Ca2+. Vertical
bar indicates timing of depolarization.
|
|
The experiments described above (Figs. 3-6) provide strong evidence
that a component of ITg is carried by
extracellular Ca2+ and Na+ ions
and that this pathway is the major source of Ca2+
for elevation of [Ca2+]i and
depolarization-independent exocytosis in these experimental conditions.
It is likely that ITg is also responsible for
facilitation of depolarization-evoked exocytosis, but this could not be
tested directly because voltage-gated Ca2+ currents
were inhibited by Zn2+ and diminished in
low-Ca2+ solution.
A current resembling ITg is
evoked by chelating intracellular Ca2+
with BAPTA
The results presented so far are compatible with the hypothesis
that in chromaffin cells Tg application activates a
Ca2+-carrying current component that may be operated
by intracellular Ca2+ stores. To obtain additional
evidence for the presence and properties of a SOC in these cells, we
performed conventional whole-cell recordings with 10 mM
BAPTA in the patch pipette. BAPTA depletes intracellular
Ca2+ stores by chelating cytosolic
Ca2+ and thereby preventing store refilling (Hoth
and Penner, 1992 ) and has been widely used for activating SOC in
various cell types (Parekh and Penner, 1997 ). In addition, chelation of
cytosolic Ca2+ should minimize the activity of the
Na-Ca exchanger (Chern et al., 1992 ).
An example of an inward current activated by intracellular perfusion
with 10 mM BAPTA (IBAPTA) is
illustrated in Figure 7. IBAPTA began to develop within 2-4 min of
membrane rupture (n = 6 of 11 cells) and reached a
maximal amplitude ( 11.0 ± 1.3 pA at 90 mV; n = 6) within several minutes. The kinetics of activation and
inactivation of IBAPTA were smoother and more
uniform than those of ITg, which is
expected if there is less contamination by Na-Ca exchanger current.
Similar to ITg,
IBAPTA often inactivated within several minutes
and had a linear I-V relationship between 120 and 60 mV
(Fig. 7B). Substitution of Na+ in the
external solution with NMDG+ reduced the amplitude
of IBAPTA by only 26.4 ± 4.5%
(n = 6) (Fig. 7A,B), consistent with the
hypothesis that ITg may include both a SOC and a
Na-Ca exchanger component. Removing both Ca2+ and
Na+ ions from the external solution reduced
IBAPTA by 83.5 ± 3.8% (eight solution
exchanges for six cells; the large amplitude, nonspecific current did
not develop when cells were perfused with the BAPTA-containing pipette
solution). Application of 2 mM Zn2+
completely blocked IBAPTA (n = 3; data not shown). Application of Tg to cells after
IBAPTA inactivation evoked an additional inward
current (ITg) but had no effect on
membrane capacitance (n = 3; data not shown),
confirming that the Tg-evoked depolarization-independent exocytosis is
mediated by elevation of [Ca2+]i.

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Figure 7.
Current activated by intracellular perfusion with
10 mM BAPTA. A, Holding current recorded at
90 mV in whole-cell configuration. The patch pipette contained 10 mM BAPTA. break-in indicates moment of
membrane rupture. Horizontal bars indicate exchange of
external solution from the standard (5 mM
Ca2+, 150 mM Na+), to
Na+-free solution (5 mM
Ca2+, 150 mM NMDG+),
to a solution that contained no added Ca2+ or
Na+ (0 Ca2+, 150 mM
NMDG+). Numbered arrows indicate
timing of voltage ramps shown in B. B,
Currents recorded during voltage ramps from 120 to 60 mV, 200 msec
duration acquired just after break-in
(1), at maximum development of an inward current
(2), in Na+-free, but
Ca2+-containing solution (3),
and in nominally Na+- and
Ca2+-free solution (4).
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|
Thapsigargin stimulates exocytosis of
catecholamine-containing vesicles
The capacitance detection technique accurately reports changes in
cell surface area but does not provide information on the type of
membrane added. To verify that Tg stimulates exocytosis of
catecholamine-containing vesicles, we labeled control and Tg-stimulated cells with antibodies against D H and examined cells with confocal microscopy after fixation. D H is a membrane-attached enzyme located exclusively on the inner surface of catecholamine-containing vesicles and is exposed on the cell exterior only when the vesicles undergo exocytosis (Phillips et al., 1983 ; Wick et al., 1997 ). As described above, depolarization-independent Cm increases
were initiated within 1-2 min after Tg application (1-5
µM). Exposure of nonvoltage-clamped cells to 5 µM Tg for 2 min resulted in the appearance of fluorescent patches corresponding to D H immunoreactivity on the cell surface (Fig. 8; shown in black in
inverted images), indicating exocytosis of catecholamine-containing
vesicles.

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Figure 8.
Thapsigargin stimulates exocytosis of
catecholamine-containing large dense-cored vesicles. A,
B, Images of chromaffin cells in transmitted light
superimposed with inverted fluorescent images of D H
immunofluorescence of the same cells. A, Unstimulated
control; B, cell stimulated with 5 µM Tg
for 2 min. D H immunofluorescent staining appears as a ring of
black patches on the surface of Tg-stimulated cell.
C, Mean fluorescent intensity (F)
of confocal images of nonstimulated cells (Control,
n = 11) and Tg-stimulated cells (After
Tg, n = 11). Background fluorescence was
not subtracted. The two groups are significantly different
(p < 0.001, Student's t
test).
|
|
 |
DISCUSSION |
In this report, we describe a Ca2+- and
Na+-carrying current activated on intracellular
Ca2+ store depletion. Ca2+ influx
via this pathway can provide sufficient Ca2+ to
elevate global [Ca2+]i and trigger
exocytosis in bovine chromaffin cells. In addition, depolarization-evoked exocytosis is strongly facilitated when the
current is activated.
Tg and BAPTA activate similar Ca2+- and
Na+-carrying currents
Application of the SERCA pump inhibitor Tg or intracellular
perfusion with the Ca2+ chelator BAPTA evoked
transient inward currents at negative holding potentials. Both
ITg and IBAPTA developed
and inactivated slowly over several minutes and had similar average
maximal amplitude, ion selectivity, and linear I-V
relationship between 120 and 60 mV. ITg and
IBAPTA share some properties with
ICRAC, including receptor-free activation
by depletion of intracellular stores, Ca2+
permeability, and block by Zn2+ (Hoth and Penner,
1993 ; Lewis and Cahalan, 1995 ; Parekh and Penner, 1997 ). Because Tg and
BAPTA have different mechanisms of action but share the property of
decreasing the Ca2+ content of intracellular stores
(Hoth and Penner, 1992 ), we conclude that ITg
and IBAPTA in chromaffin cells are members of
the family of SOCs.
Our experiments eliminate several alternative activation mechanisms for
these currents. ITg and
IBAPTA are not Ca2+-activated
currents, because depolarizing pulses evoked large-amplitude Ca2+ currents and a rapid rise in
FCa that was sustained for several tens of
seconds but was never accompanied by an additional inward current.
Also, an inward current developed in 10 mM BAPTA, and subsequent application of Tg reactivated a similar current, although high concentrations of a Ca2+ chelator with rapid
binding kinetics prevent opening of Ca2+-operated
channels (Marty and Neher, 1985 ; Roberts, 1993 ). Neither ITg nor IBAPTA are caused
by insertion of channel-containing membrane, because all exocytosis was
abolished in cells perfused with 10 mM BAPTA.
ITg and IBAPTA are not
caused by nonspecific interactions of Tg or BAPTA with the plasma
membrane, because both currents are transient in the continuous
presence of either compound.
The SOCs described here are not as highly Ca2+
selective as ICRAC. Removal of extracellular
Na+ decreased the amplitude of
ITg by 58%, suggesting a relatively high
permeability for Na+. However,
Na+ removal consistently produced a concurrent rise
in [Ca2+]i. In intact chromaffin
cells, Na+-free solutions cause elevation of
[Ca2+]i because of the reversal of the
plasma membrane Na-Ca exchanger (Chern et al., 1992 ; Pan and Kao,
1997 ). In our standard experimental conditions, the Na-Ca exchanger
should function in forward mode at negative holding potentials. Because
the exchanger is electrogenic, a component of
ITg may consist of Na-Ca exchanger current. A
more accurate measure of the ion selectivity was obtained for
IBAPTA, because activation of the Na-Ca
exchanger is prevented by high concentrations of
Ca2+ chelators (Hilgemann, 1990 ).
IBAPTA was reduced by only 26% in Na+-free solution, consistent with the hypothesis
that ITg has both store-operated and Na-Ca
exchanger current components. The combined results suggest that the
Ca2+-Na+ selectivity of the SOCs
in chromaffin cells is comparable to, or higher than, other SOCs
described previously in MDCK cells (Delles et al., 1995 ) and in cells
expressing the insect trp gene product channel (Vaca et al.,
1994 ).
There are several unresolved issues concerning both the ion selectivity
and kinetics of ITg and
IBAPTA. The I-V relationships of
these currents were determined between 120 to 60 mV to avoid activation of voltage-gated currents. Linear extrapolation of the
I-V plot yielded an unexpectedly negative reversal
potential. A possible explanation is that the I-V
relationship is nonlinear over a broad potential range. Indeed, the
I-V plot for ICRAC exhibits strong
curvature, with inward rectification at negative potentials and
reversal at positive membrane potentials (Hoth and Penner, 1992 ;
Kerschbaum and Cahalan, 1998 ).
Another difficulty is that the currents recorded at negative holding
potentials may be contaminated by undetermined "leak" conductances
in addition to the Na-Ca exchanger current. These may account for the
reduction of ITg to below prestimulatory levels in low-Ca2+, Na+-free solution,
and the incomplete inhibition of IBAPTA in
nominally Ca2+- and Na+-free
external solution. Alternatively, the ionic composition of solutions
may have direct regulatory effects on the currents. Several previous
studies have demonstrated that extracellular and intracellular divalent
cation binding sites modulate the kinetics and ion selectivity of SOCs
in nonexcitable cells (Delles et al., 1995 ; Christian et al., 1996 ;
Zweifach and Lewis, 1996 ; Kerschbaum and Cahalan, 1998 ).
Finally, the kinetic properties of SOCs are complex (for review, see
Parekh and Penner, 1997 ). SOCs are regulated by numerous factors,
including the degree and rate of store depletion (Fasolato et al.,
1998 ; Hofer et al., 1998 ), second messengers such as protein kinase C (Parekh and Penner, 1995 ), and Ca2+ passage
through the CRAC channel (Zweifach and Lewis, 1995a ,b ; Parekh, 1998 ).
Multiple regulatory mechanisms may account for the complex time course
and activation and inactivation properties of
ITg and IBAPTA. Further
work is required to fully characterize the properties of the SOCs in
bovine chromaffin cells.
The results presented here contradict the conclusion of a previous
brief report that Tg or Ca2+ chelators do not induce
depletion-activated Ca2+ currents in bovine
chromaffin cells (Bodding and Penner, 1996 ). There are three major
differences in experimental conditions that may account for the
discrepancy: (1) our use of perforated-patch instead of whole-cell
recording for all Tg experiments; (2) inclusion of 10 mM
BAPTA rather than 10-20 mM EGTA in whole-cell recordings; and (3) recording at higher temperature. Because of the complex, poorly
understood regulation of SOCs, activation may require specific experimental conditions that were not met in the previous study.
Ca2+ influx via a store-operated current can
trigger and facilitate exocytosis in bovine chromaffin cells
Although the SOC in bovine chromaffin cells requires further
characterization, the key finding of the present study is that store-operated Ca2+ influx may have profound effects
on exocytosis in excitable cells. A possible modulatory role of
capacitative Ca2+ entry on exocytosis in chromaffin
cells has been suggested based on experiments that did not control for
other pathways of Ca2+ influx (Powis et al., 1996 ).
Here we demonstrate directly that receptor-free activation of a SOC is
sufficient to trigger and/or facilitate exocytosis in bovine chromaffin cells.
In agreement with previous observations (Cheek and Thastrup, 1989 ), we
found that Tg application stimulates the appearance of the intraluminal
enzyme D H on the cell surface of intact cells within 2 min, which
corresponds to the onset of depolarization-independent capacitance
increases in voltage-clamped cells. This suggests that the capacitance
increases observed after store depletion reflect exocytosis of
catecholamine-containing large dense-cored vesicles.
Several lines of evidence indicate that depolarization-independent
exocytosis at negative potentials is caused by Ca2+
influx through ITg. Exocytosis ceased when
extracellular Ca2+ was lowered or when
ITg was blocked by extracellular application of
Zn2+, an inorganic inhibitor of SOCs in nonexcitable
cells (Hoth and Penner, 1993 ; Zhang and McCloskey, 1995 ).
Depolarization-independent exocytosis was never seen when lower
concentrations of Tg evoked a smaller amplitude inward current that was
insufficient to increase the [Ca2+]i.
Even very high Tg concentrations did not evoke
ITg or trigger exocytosis when applied in an
extracellular solution containing low Ca2+.
Facilitation of depolarization-evoked exocytosis was observed in all
cells with a Tg-activated current. In cells with detectable [Ca2+]i elevation, the
Ca2+ efficacy in evoking exocytosis
( Cm/QCa)
rose and declined in parallel with ITg and the
FCa signal. In cells without measurable [Ca2+]i elevation,
ITg and facilitation were sustained for up to
20-25 min. The parallel time course and magnitude of the inward
current and facilitation strongly suggests that Ca2+
influx through ITg is responsible for facilitation.
The amplitude of ITg is approximately 50- to
100-fold less than that of voltage-gated Ca2+
currents in bovine chromaffin cells. The ability of a SOC to trigger or
facilitate Ca2+-dependent exocytosis in chromaffin
cells probably is caused by its prolonged activation. During single
depolarizing pulses, exocytosis in these cells is initiated within
milliseconds and can proceed at rates as high as 500-1000 fF/sec
(Augustine and Neher, 1992 ). Tg-induced depolarization-independent
exocytosis occurs at slow rates (~17 fF/s) and with a significant
delay (~45 sec) after activation of ITg and
elevation of FCa. Despite the slow rate, the
total membrane addition was substantial (~1000 fF; range, 500-2000
fF), representing the fusion of ~300-400 large dense-cored vesicles
(assuming ~2.5-3 fF/vesicle) (Plattner et al., 1997 ). This
considerably exceeds the predicted size of the release-ready vesicle
pool in chromaffin cells (Gillis et al., 1996 ). Sustained Ca2+ influx may saturate Ca2+
binding sites and buffers, eventually resulting in substantial local
Ca2+ elevation. Additionally, prolonged
Ca2+ influx will probably cause changes in the
Ca2+ dependence of exocytosis by priming vesicles or
the secretory machinery, possibly via activation of second messengers
or Ca2+-dependent cytoskeletal rearrangements (Cheek
and Burgoyne, 1991 ; Heinemann et al., 1993 ; Vitale et al., 1995 ; Gillis
et al., 1996 ).
In excitable cells, store-operated Ca2+-permeable
currents may be activated by stimulation of IP3-linked
receptors. Hyperpolarization, which is often associated with receptor
stimulation (Artalejo et al., 1993 ), would amplify
Ca2+ influx via SOCs. This influx, possibly combined
with Ca2+ released from intracellular stores, may be
sufficient to trigger exocytosis at negative holding potentials. Under
physiological conditions, cation influx may also contribute to
subsequent depolarization and opening of voltage-gated
Ca2+ channels (Luthi and McCormick, 1998 ). Finally,
Ca2+ influx through SOCs may facilitate exocytosis
induced by bursts of action potentials. Thus, SOCs in excitable cells
may underlie several forms of long-lasting modulation of
stimulus-secretion coupling.
 |
FOOTNOTES |
Received Dec. 1, 1998; revised March 2, 1999; accepted March 4, 1999.
This work was supported by Grant NS22281 from the National Institute of
Neurological Diseases and Stroke. We thank Drs. N. I. Chernevskaya, K. L. Engisch, and R. Nichols for comments on this
manuscript, Dr. M. Cahalan for reading an earlier version of this
manuscript, A. Dromaretsky for technical assistance and computer
programming, and Irina Chernysh for immunohistochemistry.
Correspondence should be addressed to Dr. Martha C. Nowycky, Department
of Pharmacology and Physiology, University of Medicine and Dentistry of
New Jersey, 185 South Orange Avenue, Newark, NJ 07103.
Dr. Fomina's present address: Department of Physiology and Biophysics,
University of California, Irvine, CA 92697.
 |
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