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INTRODUCTION |
The physiological response to a stimulus is often transduced by
oscillations of the cytosolic free Ca2+ concentration
([Ca2+]c). In electrically nonexcitable cells,
[Ca2+]c oscillations are mainly driven by
antiparallel changes of the Ca2+ concentration within
intracellular Ca2+ stores. In electrically excitable cells,
[Ca2+]c oscillations are generally produced by
intermittent influx of Ca2+ through
voltage-dependent Ca2+ channels in the plasma
membrane. In some of these cells, such as muscle cells and neurons,
release of Ca2+ from intracellular stores can also
contribute to the changes in [Ca2+]c (1, 2).
The insulin-secreting pancreatic B-cell is electrically excitable. Its
main physiological stimulus, glucose, triggers insulin secretion by
increasing [Ca2+]c through the following steps.
Acceleration of glucose metabolism increases the ATP/ADP ratio, which
closes ATP-sensitive K+ channels (KATP
channels) in the plasma membrane (3). This closure decreases the
K+ conductance, which allows a yet unknown current to
depolarize the plasma membrane, leading to opening of
voltage-dependent Ca2+ channels, stimulation of
Ca2+ influx, and eventually a rise in
[Ca2+]c. In the presence of 10-15 mM
glucose, B-cells display [Ca2+]c oscillations
that result mainly from intermittent Ca2+ influx (4, 5).
However, it has been speculated that Ca2+- or inositol
1,4,5-trisphosphate
(IP3)1-induced
Ca2+ release might contribute to each
[Ca2+]c oscillation induced by glucose
(6-10).
The aim of the present study was to investigate the possible role of
intracellular Ca2+ stores in [Ca2+]c
oscillations induced by Ca2+ influx in normal pancreatic
B-cells. Strategies using targeted Ca2+-sensitive proteins
(11, 12) or trapped fluorescent low-affinity Ca2+
indicators (13-15) have recently been developed to measure directly the free Ca2+ concentration within intracellular
organelles. However, these techniques suffer from drawbacks such as
difficult transfection procedures of photoproteins, very low light
emission and Ca2+-induced degradation of aequorin, and
contamination of the trapped fluorescence of low-affinity
Ca2+ indicators by the cytosolic signal, which severely
limit their use in intact primary cells. We, therefore, used the
classical technique of Ca2+ measurement within the cytosol,
which is not invasive and is applicable to single or electrically
coupled B-cells. The results demonstrate that
[Ca2+]c oscillations occurring spontaneously
during stimulation by glucose, or artificially induced by pulses of
high K+, are accompanied by cycles of rapid uptake and
subsequent slow release of Ca2+ by the endoplasmic
reticulum (ER). Thapsigargin-sensitive Ca2+-ATPases (SERCA
pumps) are responsible for the sequestration process during the
upstroke of the [Ca2+]c transient, whereas the
subsequent phase of release does not involve depolarization-,
Ca2+- or IP3-mediated processes and likely
results from leakage from the ER. This suggests that the
Ca2+ concentration within the endoplasmic reticulum
([Ca2+]ER) oscillates. As the filling state
in Ca2+ of the ER may modulate the membrane potential of
B-cells (16), it is possible that [Ca2+]ER
oscillations play a role in the control of the oscillations of the
membrane potential.
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EXPERIMENTAL PROCEDURES |
Solutions and Drugs
Except for patch-clamp measurements and the experiments
illustrated in Fig. 4D (see below), the medium used was a
bicarbonate-buffered solution that contained 120 mM NaCl,
4.8 mM KCl, 0.5-10 mM CaCl2, 1.2 mM MgCl2, 24 mM NaHCO3
and 0-20 mM glucose as indicated. When the concentration
of KCl was increased, that of NaCl was decreased accordingly to keep
the osmolarity of the medium unchanged. Ca2+-free solutions
were prepared by substituting MgCl2 for CaCl2 and were supplemented with 0.5 or 2 mM EGTA as indicated in
the legends to Figs. 2, 3, and 5.
In the experiments illustrated in Fig. 4D, it was important
to minimize changes in the activity of the
Na+/Ca2+ exchange between solutions containing
various K+ concentrations. Therefore, KCl was not replaced
with NaCl but with choline chloride to keep a similar Na+
concentration in all solutions. The low K+ solution
contained: 79.8 mM NaCl, 4.8 mM KCl, 40.2 mM choline chloride, 2.5 mM CaCl2,
1.2 mM MgCl2, 24 mM
NaHCO3, and 0.01 mM atropine, which prevented
activation of muscarinic receptors by choline. The solutions containing
higher K+ concentrations were prepared by substituting KCl
for choline chloride.
All solutions were gassed with O2/CO2 (94:6) to
maintain a pH of 7.4 at 37 °C. Except for electrophysiological
recordings, they were supplemented with 1 mg/ml bovine serum albumin
(fraction V; Roche Molecular Biochemicals).
Thapsigargin was obtained from Sigma or from Alomone Laboratories
(Jerusalem, Israel). Ryanodine was from RBI (Natick, MA) or from
Alomone Laboratories, diazoxide was from Schering-Plough Avondale
(Rathdrum, Ireland), caffeine was from Merck A.G. (Darmstadt Germany),
and ruthenium red was from Alexis Corp. (San Diego, CA). All other
chemicals were from Sigma.
Preparation of Islets and Cells
All experiments were performed with tissue from fed female NMRI
mice (25-30 g). Pancreatic islets were isolated aseptically after
collagenase digestion of the pancreas, and when needed, they were
dispersed into cells as described previously (17). Cells were allowed
to attach to 22-mm circular coverslips and cultured for 2-3 days.
Intact islets were maintained in culture for 1-3 days. When the
membrane potential of B-cells was to be measured with an intracellular
microelectrode, the islets were allowed to attach to the coverslip by a
culture period of at least 2 days. The culture medium was RMPI 1640 medium containing 10 mM glucose, 10% heat-inactivated
fetal calf serum, 100 IU/ml penicillin, and 100 µg/ml streptomycin.
Measurements of [Ca2+]i
Cultured islets were loaded with 2 µM fura-PE3/AM
(Teflabs, Austin, TX) for 90-120 min at 37 °C in a
bicarbonate-buffered solution containing 10 mM glucose.
Cultured cells were loaded with 1 µM fura-2/AM (Molecular
Probes, Eugene, OR) for 60 min in a similar bicarbonate-buffered
medium. The tissue was then transferred into a temperature-controlled
(37 °C) perifusion chamber of ~1 ml (Intracell, Royston, Herts,
United Kingdom) with a bottom made of a glass coverslip and mounted on
the stage of an inverted microscope. The flow rate of the perifusion
was approximately 2 ml/min. When rapid exchange of solutions was
required, a ~250-µl chamber was used and solutions were changed by
Iso-Latch valves (Parker Hannifin, Fairfield, NY).
[Ca2+]i was directly measured in cells attached
to the coverslip or in islets held in place close to the coverslip by
gentle suction with a glass micropipette. In some experiments, cultured
cells were pressure-injected with an 5242 Eppendorf microinjector
(Hamburg, Germany). The injected solution contained either 6-10
mM fura-2 K+ salt or 10 mM
fura-dextran K+ salt (molecular weight, 3000) (Molecular
Probes) dissolved in H2O, and it was supplemented or not
with test substances. The techniques used to monitor
[Ca2+]c have been described previously (4).
Flash-Photolysis
Clusters of B-cells were incubated with 5 µM
nitrophenyl-EGTA AM and 1.5 µM fura-2 AM (Molecular
Probes) for 60 min at 37 °C. Photolysis of nitrophenyl-EGTA was
performed by two or three consecutive 1-ms UV flashes of 240 J (Xenon
flashlamp system XF-10, Hi-Tech, Hamburg, Germany).
Electrophysiology
Membrane Potential Recordings--
The islets were mounted in a
perifusion chamber (7 ml/min at 37 °C) following attachment to glass
coverslips. The membrane potential of a single cell within the islet
was continuously measured with a high resistance microelectrode.
Patch-Clamp Recordings--
Voltage-clamp experiments were
performed on single B-cells using the perforated patch-whole cell
configuration and an EPC-7 patch-clamp amplifier (List Elektronik,
Darmstadt, Germany). The holding potential was
70 mV, and the cells
were submitted either to 100-ms depolarizations to 0 mV or to bursts of
100-ms depolarizations (2 Hz) from
50 mV to
10 mV for 12 s.
The associated changes in [Ca2+]i were measured
using an IonOptix fluorescence imaging system (IonOptix, Inc., Milton,
MA). The extracellular solution contained 138 mM NaCl, 5.6 mM KCl, 1.2 mM MgCl2, 2.6 mM CaCl2, 5 mM HEPES (pH 7.4 with
NaOH), and 10 mM glucose. The pipette solution contained 76 mM Cs2SO4, 10 mM NaCl,
10 mM KCl, 1 mM MgCl2, and 5 mM HEPES (pH 7.35 with CsOH). Electrical contact with the cell interior was established by adding 0.24 mg/ml amphotericin B to
the pipette solution, and the voltage-clamp was considered satisfactory
when the series conductance (Gseries) was >35-40 nano Siemens. All experiments were performed at 33 °C, and the zero-current potential of the pipette was adjusted with the pipette in
the bath solution.
Presentation of Results
The experiments are illustrated by recordings that are averaged
or representative traces of results obtained with the indicated number
of cells or islets from at least three different cultures. The
statistical significance of differences between means was assessed by
unpaired Student's t test.
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RESULTS |
[Ca2+]c Oscillations Induced by Glucose Are
Followed by Ca2+ Release from the ER--
B-cells within
intact islets display a rhythmic electrical activity when perifused
with a medium containing an insulin-releasing glucose concentration (10 mM) and 10 mM Ca2+ (Fig.
1A). These bursts of
electrical activity consist of sharp depolarizing waves of the membrane
potential with superimposed spikes reflecting Ca2+ influx
through voltage-dependent Ca2+ channels (18).
Under these conditions, [Ca2+]c also oscillates,
but, in contrast to the fast, monophasic repolarization of the
oscillations of membrane potential, the descending phase of each
Ca2+ oscillation clearly displays two components (Fig.
1B). Whereas the initial fast one appears to coincide with
the closure of voltage-dependent Ca2+ channels
following rapid repolarization of the plasma membrane, the second, much
slower phase appears to occur during the repolarized intervals.

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Fig. 1.
Glucose induces sharp oscillations of the
membrane potential (A), whereas the accompanying
oscillations in [Ca2+]c (B-D)
display a slow recovery phase that is abolished by SERCA pump
inhibitors in pancreatic B-cells. A-C, whole islets
were perifused with a medium containing 10 mM glucose and
10 mM Ca2+ throughout. In the experiment shown
in C, the medium used for the loading with fura-PE3 was
supplemented with 1 µM TG. D, a cluster of
islet cells was perifused with 15 mM glucose and 2.5 mM Ca2+ throughout. CPA was added to the
perifusion medium when indicated. The traces are representative of
results obtained in 13 (A), 36 (B), and 18 (C) islets and 15 clusters of cells (D).
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Previous experiments have shown that intracellular Ca2+
stores of whole islets are efficiently emptied by thapsigargin (TG), a
specific inhibitor of the SERCA pump (19), but that this emptying requires preincubation of the islets with the drug (17). In islets
pretreated with 1 µM TG, the amplitude of
[Ca2+]c oscillations was much larger than in
control islets, and the descending phase of each
[Ca2+]c oscillation was surprisingly very fast
with no slow second phase (Fig. 1C). This suggests that the
slow phase observed in control islets results from a release of
Ca2+ from the ER, rather than from a slow Ca2+
extrusion from the cytosol.
The effect of intracellular Ca2+ store depletion on
[Ca2+]c oscillations was also investigated in
clusters of islet cells, a preparation in which the SERCA pump can be
blocked by an acute addition of TG or cyclopiazonic acid (CPA). CPA is
an inhibitor structurally unrelated to TG (19) and has also been shown
to empty the ER of Ca2+ in pancreatic B-cells (20). In the
presence of 15 mM glucose and 2.5 mM
Ca2+, [Ca2+]c oscillated slowly and
regularly (Fig. 1D). Addition of 50 µM CPA to
the medium accelerated the oscillations, which increased in amplitude
and frequency and became sharper mainly because of the disappearance of
the slow recovery phase. Similar results were obtained in clusters of
islet cells treated by TG (not shown).
Ca2+ Release from the ER Can be Detected after Pulses
of High K+--
In this series of experiments,
glucose-induced [Ca2+]c oscillations were
inhibited by diazoxide, which, by opening KATP channels,
clamps the membrane potential at a hyperpolarized level.
[Ca2+]c oscillations were then reinduced by
rhythmically depolarizing the plasma membrane with high
K+.
Raising the K+ concentration of the perifusion medium from
4.8 to 45 mM rapidly depolarized the plasma membrane from
70 ± 2 mV to
22 ± 3 mV in control islets
(n = 4; Fig. 2A,
dotted line). The amplitude of this depolarization was not
affected by TG pretreatment of the islets (
71 ± 3 to
22 ± 3 mV, n = 4). The time required to clamp the plasma
membrane at a new, stable potential was also similar in both groups, as
follows. Controls: 31 ± 2 s from 4.8 to 45 mM
K+ (t1/2 = 4 ± 0 s) and
34 ± 1 s from 45 to 4.8 mM K+
(t1/2 = 5.7 ± 0.5 s), n = 4; TG-treated islets: 31 ± 1 s from 4.8 to 45 mM
K+ (t1/2 = 4.5 ± 0.3 s) and
34 ± 1 s from 45 to 4.8 mM K+
(t1/2 = 5.7 ± 0.5 s),
n = 4.

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Fig. 2.
Pulses of 45 mM K+
induce [Ca2+]c oscillations with a slow recovery
phase that is prevented by SERCA pump inhibition in pancreatic
B-cells. The medium contained 10 mM glucose and 250 µM diazoxide in all experiments. 30-s pulses of 45 mM K+ were applied as shown by bars.
The Ca2+ concentration of the perifusion medium was either
10 mM throughout (A) or was changed as indicated
(B-C). A and B, whole islets were
used. In A, solid lines show changes in
[Ca2+]c, whereas the dotted lines
illustrate associated changes of the membrane potential recorded in
separate islets. For the traces labeled thapsigargin in A
and B, the islets were incubated with 1 µM TG
during the loading procedure with fura-PE3
([Ca2+]c measurements) or during a 90-120-min
preincubation in the culture medium prior the experiments (membrane
potential measurements). C, a single pancreatic B-cell was
used; it was injected with fura-2 dextran. TG was applied when
indicated. Ca2+-free solutions were supplemented with 2 mM EGTA. The traces are representative of results obtained
in 12 (A) ([Ca2+]c), 4 (A)
(MP), and 7 (B) islets and 4 single cells
(C).
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In control islets, high K+ pulses (for 30 s) induced
[Ca2+]c oscillations characterized by a
descending phase that displayed an initial fast component concomitant
with rapid repolarization of the plasma membrane, followed by a slow
decline (Fig. 2A, solid line). In TG-pretreated islets,
[Ca2+]c oscillations were higher than in control
islets (467 ± 21 versus 352 ± 11 nM,
n = 10, p < 0.01) and devoid of a slow recovery phase. Similar results were obtained after pretreatment of the
islets with 50 µM CPA.
The effects of TG on voltage-dependent Ca2+
current were evaluated in single B-cells using the perforated patch
configuration. Under control conditions, a 100-ms voltage-step from
70 to 0 mV elicited a peak Ca2+ current of 52 ± 6 pA (n = 8) that was not significantly affected by a
5-min exposure to 1 µM TG (48 ± 3 pA). The
integrated whole-cell Ca2+ current was similarly unaffected
by TG (data not shown). This excludes the possibility that the larger
rise in [Ca2+]c induced by high K+ in
TG-treated islets results from an increased Ca2+ current.
We also verified that the slow [Ca2+]c recovery
is not a peculiarity observed only in a medium containing 10 mM Ca2+. To this end, 30-s pulses of 45 mM K+ were applied in the presence of various
concentrations of external Ca2+ (0.5-10 mM)
(Fig. 2B). The amplitude of the resulting
[Ca2+]c peaks clearly depended on the
Ca2+ concentration of the medium, but a slow decaying
phase, prevented by TG pretreatment, was observed at all external
Ca2+ concentrations tested. The observation that TG
suppresses the slow recovery after [Ca2+]c
oscillations of various amplitude also excludes the possibility that TG
might increase the rate of Ca2+ extrusion from the cytosol
due to a high Ca2+ signal.
The slow [Ca2+]c recovery phase could be
artifactual and reflect changes in the Ca2+ concentration
within the ER if fura-PE3 is compartmentalized. To exclude this
possibility, single B-cells were microinjected with fura-dextran, a
Ca2+ probe that is exclusively localized in the cytosol
(21). High K+ pulses induced [Ca2+]c
oscillations with a slow recovery phase (Fig. 2C). Addition
of TG to the medium induced a transient increase in
[Ca2+]c reflecting intracellular Ca2+
pool emptying. Subsequent depolarization by pulses of high
K+ triggered [Ca2+]c oscillations
that were of much larger amplitude than before addition of the SERCA
pump inhibitor and that lacked a slow [Ca2+]c
recovery phase. These observations strongly support the conclusion that
the slow decaying [Ca2+]c phase results from
release of Ca2+ from the ER.
Characteristics and Kinetics of Ca2+ Exchanges between
the ER and the Cytosol--
Application of high K+ pulses
every 5 min triggered a train of [Ca2+]c
oscillations with a slow decaying phase, which indicates that the
phenomenon is not a transient one (Fig.
3A). The experiments depicted
in Fig. 3B were designed to explore the temporal
requirements for refilling the intracellular Ca2+ stores
responsible for the slow decay in [Ca2+]c. The
islets were repetitively depolarized by 30-s pulses of high
K+. Extracellular Ca2+ (10 mM) was
present before and during the depolarization (first and last pulses) or
only during the depolarization (second to seventh pulses). The slow
recovery phase was present and not attenuated by Ca2+
omission during the repolarization phases (compare Fig. 3, A and B). This shows first that it does not result from
Ca2+ influx, and second that Ca2+ entry during
depolarization is sufficient to refill the pools from which
Ca2+ is slowly released.

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Fig. 3.
Ca2+ is rapidly taken up by the
ER during the upstroke of each [Ca2+]c
oscillation and is released at the end of each oscillation. All
solutions contained 10 mM glucose and 250 µM
diazoxide. The Ca2+ concentration of the perifusion medium
was changed when indicated. Ca2+-free solutions were
supplemented with 2 mM EGTA. 100 µM ACh and
30-s (A-D) or 20-s (E) pulses of 45 mM K+ were applied when indicated. The traces
are representative of results obtained in 11 (A), 12 (B), 4 (C), 8 (D), and 4 (E) islets.
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However, no slow recovery phase was observed when high K+
pulses were applied in the continuous presence of acetylcholine (ACh), a potent IP3-producing agent in pancreatic B-cells (Fig.
3C). This is likely due to the fact that Ca2+
cannot accumulate into the ER because it immediately exits from the ER
into the cytosol through IP3 receptors that are maintained opened by the continuous presence of ACh.
The ability of the ER to take up Ca2+ rapidly was next
tested (Fig. 3D). Islets perifused with a
Ca2+-free medium were submitted to three pulses of 100 µM ACh applied at 12.5-min intervals. A 30-s pulse of
high K+/high Ca2+ was applied between the
second and the third pulses of ACh. Whereas the first application of
ACh triggered a large [Ca2+]c peak, the second
one induced only a small rise in [Ca2+]c
suggesting that intracellular Ca2+ stores were nearly
completely emptied already by the first application of ACh. However,
the third application of ACh in a Ca2+-free medium after
the short pulse with high K+/high Ca2+ induced
a transient rise in [Ca2+]c that was much larger
than that seen after the second application of ACh. This indicates
further that intracellular Ca2+ pools rapidly refill
during the large [Ca2+]c rises triggered by high
K+ pulses.
If the slow recovery phase reflects release of Ca2+ from
the ER, its characteristics should depend on the filling state of the ER. This was tested by emptying the ER with ACh between two series of 3 pulses of high K+/high Ca2+ of 20 s
duration (Fig. 3E). The first three
[Ca2+]c oscillations were all characterized by a
slow recovery phase. In contrast, the first two oscillations following
intracellular Ca2+ pool depletion by ACh were of lower
amplitude and displayed a much smaller slow recovery phase than before
ACh application. Because the pulses were of constant duration, the
lower amplitude of [Ca2+]c oscillations post-ACh
is unlikely to result from a decreased Ca2+ influx. It may
rather be explained by a more avid sequestration of Ca2+
into an emptied than into a filled ER. Because the first high K+/high Ca2 pulse did not carry enough
Ca2+ to fully refill the ER, no slow recovery phase could
be seen, and three pulses were needed to refill the ER enough to see a slow recovery phase of an amplitude similar to that observed at the end
of the first series of [Ca2+]c oscillations.
These data demonstrate that the buffering capacity of the ER permits a
rapid control of [Ca2+]c and that its ability to
release Ca2+ is affected by its filling state.
Comparison of the [Ca2+]c changes induced by a
pulse of high K+ in control and TG-treated islets permits
estimation of the kinetics of Ca2+ uptake and release from
the ER (Fig. 4A). After
normalization of resting [Ca2+]c before each
[Ca2+]c oscillation the averaged
[Ca2+]c oscillation of TG-treated islets was
subtracted from the averaged [Ca2+]c oscillation
of control islets (Fig. 4B). The downward deflection of the
curve reflects Ca2+ uptake by the ER, whereas the
upward deflection reflects release from the ER. This shows that the
uptake is very fast, whereas the release is comparably slow and
lasts several minutes.

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Fig. 4.
A and B, kinetics of uptake
and release of Ca2+ by the ER during and after high
K+-induced [Ca2+]c oscillations. All
solutions contained 10 mM Ca2+, 10 mM glucose and 250 µM diazoxide throughout. A
30-s pulse of 45 mM K+ was applied when
indicated by the bar. A illustrates averaged
traces from 10 [Ca2+]c oscillations recorded in
control islets (solid line) or islets treated with 1 µM TG during the period of loading with fura-PE3
(dotted line). The trace in B was obtained by
subtracting the average TG trace from the average control trace.
C, rate of [Ca2+]c change as a
function of [Ca2+]c in control and TG-treated
islets. The data points were taken from the averaged
[Ca2+]c oscillations induced by high
K+ and illustrated in A. The time between data
points is 1.6 s. The curved arrow indicates the
temporal sequence of [Ca2+]c changes during the
[Ca2+]c oscillations. D, the
Ca2+ concentration of the ER depends on
[Ca2+]c. Clusters of islet cells were perifused
with a medium containing 10 mM glucose, 250 µM diazoxide, and various concentrations of
K+ (4.8 to 45 mM). The Ca2+
concentration of the perifusion medium was 2.5 mM except in
two sets of experiments for which the medium was a
Ca2+-free medium supplemented with 500 µM
EGTA (Ca0). The Na+ concentration was kept constant between
the different media tested (see under "Experimental Procedures").
TG was added as indicated. The traces are representative of results
obtained in 30-57 clusters of cells. E and F,
glucose buffers the [Ca2+]c rise during a pulse
of high K+ and enhances the amplitude of the subsequent
slow [Ca2+]c recovery phase. All solutions
contained 10 mM Ca2+ and 250 µM
diazoxide throughout, and no glucose (G 0) or 20 mM of the sugar (G 20). A 30-s pulse of 45 mM K+ was applied when indicated by the bar.
E illustrates averaged traces from
[Ca2+]c oscillations recorded in control islets
perifused without glucose (n = 11) or with 20 mM of the sugar (n = 8). The traces in
F were obtained by subtracting, at each glucose
concentration, the average TG trace (obtained in islets preincubated
with 1 µM TG during the period of time they were loaded
with fura-PE3) from the average control trace. Only the fragment of the
traces reflecting release of Ca2+ is represented.
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The role of the ER during the whole [Ca2+]c
oscillation is best demonstrated by the comparison of the rates of
[Ca2+]c changes as a function of
[Ca2+]c in control and TG-treated islets (Fig.
4C). It clearly shows that the ER strongly buffers the rate
of [Ca2+]c changes during the whole
[Ca2+]c oscillation, thereby preventing any
abrupt large change in [Ca2+]c.
Modulation of Ca2+ Exchanges between the ER and the
Cytosol--
The above results suggest that the amount of
Ca2+ that is taken up by the ER is directly proportional to
[Ca2+]c. This was indirectly verified by
measuring the amplitude of the [Ca2+]c peak that
occurred upon addition of TG to clusters of cells in which
[Ca2+]c was clamped artificially at different
levels with various concentrations of K+ (4.8-45
mM). The amplitude of the [Ca2+]c
peak directly depended on the steady-state level of [Ca2+]c before TG addition (Fig. 4D),
suggesting that the Ca2+ loading of the ER is directly
proportional to the level of [Ca2+]c. This did
not result from a K+ effect, as the amplitude of the rise
in [Ca2+]c was similar in clusters perifused with
a Ca2+-free medium containing 4.8 or 45 mM
K+. The large rise in [Ca2+]c
produced by TG in the presence of high K+ and
Ca2+ is in agreement with the large slow
[Ca2+]c decay observed after depolarizing pulses
with high K+.
The effect of glucose was also tested. 30-s pulses of high
K+ induced a larger [Ca2+]c rise in
the absence of glucose than in the presence of 20 mM
glucose (Fig. 4E). By contrast, the slow
[Ca2+]c recovery phase was more pronounced in a
glucose-containing than in a glucose-free medium. It was prevented by
TG pretreatment (not shown). To estimate the amplitude and the kinetics
of Ca2+ release from the ER in glucose-containing and
glucose-free medium, the averaged [Ca2+]c
oscillation of TG-treated islets was subtracted from the averaged
[Ca2+]c oscillation of control islets in the
presence and in the absence of glucose (Fig. 4F). This
revealed a much larger [Ca2+]c release phase in
the presence of 20 mM glucose than in its absence.
Mechanisms of the Slow Ca2+ Release Process from the
ER--
In skeletal muscle cells, depolarization of the plasma
membrane alone can trigger release of Ca2+ from
intracellular stores (22). However, this process does not seem to be
operative in pancreatic B-cells, as no [Ca2+]c
increase could be detected when the islets were depolarized by pulses
of high K+ in a Ca2+-free medium supplemented
with 2 mM EGTA (Fig.
5A). This lack of effect of
high K+ did not result from exhaustion of intracellular
Ca2+ pools by EGTA present in the medium because ACh could
still trigger Ca2+ mobilization after 2 inefficient pulses
of high K+.

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Fig. 5.
The slow [Ca2+]c
recovery phase following high K+-induced
[Ca2+]c oscillations does not involve
depolarization- or IP3-induced Ca2+ release and
a similar slow decay is observed after an abrupt rise in
[Ca2+]c triggered by uncaging
Ca2+ by flashes of UV light. A, whole
islets loaded with fura-PE3. B, clusters of islet cells
loaded with fura-2 and nitrophenyl-EGTA. C, single cells
injected with fura-2, with or without heparin. All perifusion solutions
contained 10 mM glucose and 250 µM diazoxide
throughout. The Ca2+ concentration of the medium was either
constant throughout the whole experiment (B), or it was
changed and test agents (100 µM ACh or 1 µM
TG) were added when indicated (A and C).
[Ca2+]c was increased by uncaging
Ca2+ from nitrophenyl-EGTA with two or three flashes of UV
light (arrows in B) or by 30-s pulses of 45 mM K+ (bars in A-C). In
A and C, Ca2+-free solutions were
supplemented with 2 mM EGTA. In B, interruption
of the trace corresponds to a period during which 1 µM TG
was applied. The traces are representative of results obtained in 10 islets (A), 3 clusters of cells (B), and 4 (control) and 6 (heparin) single cells (C).
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Depolarization is not sufficient and even not necessary, as shown by
the following experiment. Pancreatic B-cells were loaded with the caged
Ca2+ compound, nitrophenyl-EGTA, whereas
[Ca2+]c was kept at basal levels by the presence
of 4.8 mM K+ and 250 µM diazoxide
in the medium. Flashes of UV light induced a large rise in
[Ca2+]c, which then decreased in two phases, an
initial fast one followed by a slow recovery to basal levels (Fig.
5B). Brief depolarization with 45 mM
K+ was followed by a similar biphasic response. After
addition of TG, a second series of UV flashes triggered a new increase
in [Ca2+]c followed by a rapid decrease that now
lacked the slow recovery phase. These experiments clearly demonstrate
that the rise in [Ca2+]c is sufficient to induce
a slow recovery phase, even in the absence of membrane depolarization.
Two well characterized mechanisms can trigger Ca2+ release
from intracellular Ca2+ stores: Ca2+-induced
and IP3-induced Ca2+ release (2, 23). High
concentrations (5-20 mM) of caffeine are known to induce
or to potentiate Ca2+-induced Ca2+ release and
to inhibit IP3-induced Ca2+-release (24).
However, 10 mM caffeine was without effect on the slow
recovery phase observed at the end of a 30-s pulse of 45 mM
K+ (data not shown). Ryanodine is a potent modulator of
Ca2+-induced Ca2+ release. It activates this
process at low concentrations (
1 µM) but blocks it at
high concentrations (
10 µM) (24, 25). Here, the islets
were treated acutely, preincubated, or cultured with different
concentrations of ryanodine (1-100 µM). In no case did
we observe an effect of ryanodine on basal
[Ca2+]c, on peak
[Ca2+]c-induced by high K+ pulses, or
on the subsequent slow recovery phase (data not shown). Microinjection
of B-cells with 10 mM ryanodine was also ineffective (n = 3, data not shown).
In many tissues, including pancreatic B-cells, phospholipase C can be
activated directly by a rise in [Ca2+]c or by
depolarization of the plasma membrane (8, 26). It is therefore possible
that a [Ca2+]c rise increases IP3
levels, which in turn trigger Ca2+ release. To test this
hypothesis, pancreatic B-cells were microinjected with heparin, a
blocker of the IP3 receptor in various tissues, including
pancreatic B-cells (27). In B-cells microinjected with fura-2 free
acid alone, a pulse of high K+ induced a large
[Ca2+]c oscillation characterized by a slow
recovery phase (Fig. 5C). Subsequent addition of 100 µM ACh triggered a large and transient increase in
[Ca2+]c. Emptying the ER with TG induced a
further rise in [Ca2+]c and prevented the slow
recovery phase of the [Ca2+]c oscillation induced
by a subsequent pulse of high K+. Heparin microinjection
(molecular weight 6000; 200 mg/ml) completely prevented the ACh-induced
[Ca2+]c rise without affecting the response to TG
(Fig. 5C). As heparin did not affect the slow recovery phase
of the [Ca2+]c oscillation induced by high
K+, it is clear that this phase is not induced by an
IP3-mediated Ca2+ release.
A delayed, slow return of [Ca2+]c to basal level
after a depolarization-induced [Ca2+]c rise has
been observed in neurons and chromaffin cells (28-31) and attributed
to a slow release of Ca2+ from mitochondria. No similar
process seems to be operative in B-cells. Thus, microinjection of
B-cells with 1 mM ruthenium red (giving a final cytosolic
concentration >1 µM) did not affect the slow recovery
[Ca2+]c phase after a pulse of high
K+ (n = 3, data not shown), although the
drug is regarded as a potent and selective inhibitor of the
mitochondrial Ca2+ uniporter at ~ 1 µM
(32).
These experiments indicate that the release of Ca2+
observed after a rise in [Ca2+]c originates from
the ER; that it is not triggered by depolarization-, IP3-,
or Ca2+-induced Ca2+ release; and that none of
these three mechanisms contribute to the [Ca2+]c
rise induced by high K+.
Effect of Intracellular Ca2+ Pool Depletion under More
Physiological Conditions--
Ideally, release of Ca2+ at
the end of [Ca2+]c oscillations induced by
glucose in a physiological medium containing 2.5 mM
Ca2+ should now be sought for. Unfortunately, this was not
possible because emptying of intracellular Ca2+ pools by TG
transformed oscillations of the membrane potential of whole islets
induced by 10 mM glucose into a sustained depolarization with continuous spike activity (Fig.
6A).

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Fig. 6.
A, inhibition of the SERCA pump by TG
transforms oscillations of the membrane potential into a sustained
depolarization with spikes in pancreatic B-cells perifused with 10 mM glucose and 2.5 mM Ca2+. In the
right panel, the islet was pretreated for 90 min with 1 µM TG in the culture medium. The traces are
representative of results obtained in 29 (control) and 11 (TG) islets.
B, TG increases the amplitude of the
[Ca2+]c rise and suppresses the slow phase of
[Ca2+]c recovery in voltage-clamped pancreatic
B-cells submitted to trains of 100-ms depolarizations designed to mimic
glucose-induced bursts of action potentials. The traces are
representative of results obtained in eight cells.
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We therefore tested the effect of intracellular Ca2+ pool
depletion in voltage-clamped single B-cells subjected to trains of 100-ms depolarizations (2 Hz for 12 s) from
50 to
10 mV
(holding potential,
70 mV) designed to mimic glucose-induced bursts
of action potentials (Fig. 6B). This induced a large rise in
[Ca2+]c that was followed by a slow recovery to
basal levels upon repolarization to
70 mV. Once
[Ca2+]c had returned to basal levels, TG was
applied for 5 min, and the cell was again subjected to a burst of
depolarizations. This raised [Ca2+]c to a higher
level than before TG addition (776 ± 64 versus
577 ± 53 nM, respectively; p < 0.05;
n = 8). Importantly, the time constant of the falling
phase was much shorter (3.1 ± 2.1 versus 13 ± 2.4 s, respectively; p < 0.01). This suggests that intracellular Ca2+ stores play a role in the
oscillations in [Ca2+]c during bursts of action
potentials induced by glucose.
 |
DISCUSSION |
The present study demonstrates that rapid uptake and release of
Ca2+ by the ER contributes to [Ca2+]c
oscillations induced by Ca2+ influx through
voltage-dependent Ca2+ channels in pancreatic
B-cells.
Nature of the Intracellular Ca2+ Store Taking up and
Releasing Ca2+ in Response to a Rise in
[Ca2+]c Triggered by Ca2+
Influx--
A fast and strong [Ca2+]c buffering
has been documented in patch-clamped B-cells (33). Two observations in
the present study ascribe this property to the ER. First, a 30-s pulse
of high K+ could replenish nearly completely emptied
ACh-sensitive stores. Second, the rise in [Ca2+]c
induced by depolarization was faster and larger in TG and CPA-treated
islets than in controls, although the Ca2+ current was not
increased. This is in agreement with the recent report that 20 mM K+ raises [Ca2+]ER
in INS-1 rat insulinoma cells expressing aequorin in the ER (34). The
ER is also the source of Ca2+ that is released into the
cytoplasm after a rise in [Ca2+]c, because
inhibition of the SERCA pump by TG or CPA or opening of
IP3 receptors by ACh completely abolished the slow [Ca2+]c recovery phase. Furthermore, the filling
state of the ER profoundly affected the characteristics of the slow
recovery phase.
Uptake of Ca2+ by mitochondria during a rapid rise in
[Ca2+]c has been documented in various cell
types, including neurons, chromaffin cells, and insulin-secreting cells
(28-31, 35, 36). However, we found that the slow decay of
[Ca2+]c following an abrupt rise was unaffected
by ruthenium red, a blocker of the mitochondrial Ca2+
uniporter (32). These observations clearly establish that mitochondria are not primarily responsible for the slow
[Ca2+]c decay.
Regulation of Ca2+ Uptake--
Uptake of
Ca2+ by the ER directly depends on
[Ca2+]c. Indeed, the amount of Ca2+
that was released from the ER by TG was proportional to the
steady-state level of [Ca2+]c in clusters of
cells depolarized with various concentrations of K+. Such a
Ca2+ dependence of the uptake has been clearly demonstrated
in various cells (14, 37, 38). Pancreatic B-cells express SERCA-2B and
SERCA-3 isoforms (39), SERCA-2B being the most sensitive to
Ca2+ among all SERCA isoforms (40).
Uptake of Ca2+ by the ER is also modulated by the glucose
concentration of the medium. A smaller influx of Ca2+
through voltage-dependent Ca2+ channels cannot
explain why high K+-induced [Ca2+]c
oscillations were smaller in the presence of 20 mM glucose
than 0 mM glucose because glucose enhances
voltage-dependent Ca2+ currents in B-cells
(41). The difference rather results from an increased buffering
capacity of the ER in the presence of glucose. This is in agreement
with the observation that stimulation of B-cells with glucose causes an
initial drop in [Ca2+]c that is blocked by TG
(42). Other studies have shown that the amount of Ca2+
taken up by the ER of permeabilized RINm5F insulinoma cells depends on
the ATP/ADP ratio (37). The longer [Ca2+]c
recovery phase observed in the presence of glucose therefore reflects a
larger release of Ca2+ from the ER into which glucose has
promoted Ca2+ sequestration during influx of the ion.
Mechanism of Ca2+ Release--
Three mechanisms of
Ca2+ release from intracellular Ca2+ stores
have been described: depolarization-, Ca2+-, and
IP3-induced Ca2+ release (2, 22, 23). We did
not detect any depolarization-induced Ca2+ release from
filled Ca2+ stores in mouse pancreatic B-cells, but we
showed that a rise in [Ca2+]c is sufficient to
induce slow release of the ion from the ER when
[Ca2+]c decreases. Ca2+- and/or
IP3-induced Ca2+ release has been suggested to
play a role in glucose-induced [Ca2+]c changes
(6-10). Pancreatic B-cells express very low levels of type 2 ryanodine
receptors (9) responsible for Ca2+-induced Ca2+
release (2) and high amounts of IP3 receptors. We used
heparin, caffeine, and ryanodine, three established modulators of
Ca2+- or IP3-induced Ca2+ release
(24, 25, 27), to investigate the possible contribution of these
processes to [Ca2+]c oscillations induced by high
K+ pulses. None of these compounds affected the
oscillations. Moreover, if a depolarization-, Ca2+-, or
IP3-induced Ca2+ release participated in high
K+-induced [Ca2+]c rise in pancreatic
B-cells, the latter would be reduced by depletion of intracellular
pools with TG. The results show exactly the opposite. Taken together,
our experiments suggest that the release of Ca2+ observed
after a rise in [Ca2+]c is not triggered by
depolarization-, IP3- or Ca2+-induced
Ca2+ release and that none of these three mechanisms
contribute to the [Ca2+]c rise induced by high
K+.
Ca2+ release from the ER at the end of
[Ca2+]c oscillations more likely corresponds to a
slow release of Ca2+ from the organelle, which slowly
adapts its Ca2+ concentration to
[Ca2+]c. Release of Ca2+ through the
same pathway may explain the rise in [Ca2+]c that
occurs upon blockade of the SERCA pump with TG. Because of its high
Ca2+ permeability, this pathway has often been referred to
as leak from the ER. Although it has been observed in many cell types, its exact nature has not been determined (14, 43).
Sequence of Events--
Many processes regulating
[Ca2+]c are directly influenced by
[Ca2+]c and [Ca2+]ER.
The plasma membrane Ca2+-ATPase (PMCA) is strongly
stimulated when [Ca2+]c increases (38, 43). The
Ca2+-ATPase of the ER is proportionally more stimulated by
cytosolic Ca2+ than the PMCA (38), but it is inhibited by
luminal Ca2+ (14). Ca2+ leakage through the ER
seems only mildly stimulated by luminal Ca2+ (14). On the
other hand, there is an interplay between the rate at which
Ca2+-ATPases work and the available energy. It is indeed
possible that changes in the pumping rate of Ca2+-ATPases
during [Ca2+]c oscillations modulate the ATP/ADP
ratio, which in turn modulates the activity of Ca2+-ATPases
(44). We have recently shown that the ATP/ADP ratio drops rapidly when
[Ca2+]c is raised and increases when
[Ca2+]c falls (45). Periodic release and reuptake
of Ca2+ from the ER of permeabilized RINm5F cells
supplemented with an oscillating glycolytic cell-free muscle extract
have been reported (46).
Basal [Ca2+]c is set by a balance between
processes that increase [Ca2+]c (leak entry of
Ca2+ from the extracellular space and leak release of
Ca2+ from the ER) and processes that decrease
[Ca2+]c (extrusion mechanisms that remove
Ca2+ from the cytosol) (Fig.
7B). When
[Ca2+]c increases abruptly as a result of
Ca2+ influx through voltage-dependent
Ca2+ channels, Ca2+ extrusion out of the cell
by the PMCA is stimulated, and Ca2+ uptake by the ER occurs
at a higher rate than Ca2+ release (Fig. 7C). As
[Ca2+]c rises, the ATP/ADP ratio decreases (45),
perhaps because of ATP consumption by these ATPases. When
repolarization of the plasma membrane closes
voltage-dependent Ca2+ channels,
Ca2+ influx abruptly stops. This, together with rapid
uptake by the ER and extrusion out of the cell, produces a fast drop in
[Ca2+]c that corresponds to the first phase of
[Ca2+]c decrease (Fig. 7D). As
[Ca2+]c decreases, the PMCA is less stimulated.
In the ER, Ca2+ release predominates over Ca2+
uptake because the latter is inhibited by high luminal
[Ca2+] (14) and by the lowering of the ATP/ADP ratio.
This corresponds to the beginning of the slow phase of
[Ca2+]c decrease that lasts until release and
uptake reach a new equilibrium. As the PMCA extrudes Ca2+
less efficiently than the SERCA pumps it into the ER (38), Ca2+ could even cycle between the cytosol and the ER, which
would prolong the slow [Ca2+]c decrease.

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Fig. 7.
Model of the interplay between
[Ca2+]c and [Ca2+]ER,
and of the role of [Ca2+]ER in the control of
the membrane potential during [Ca2+]c
oscillations induced by glucose. A illustrates a
typical [Ca2+]c oscillation induced by 10 mM glucose in a medium containing 10 mM
Ca2+. Below are the expected changes of
[Ca2+]ER. B-D schematize
Ca2+ movements and major ionic currents at the times
indicated by the corresponding arrows in A. The
thickness of the arrows shown with solid lines is
proportional to the rate of pumping or intensity of the current. The
size of the symbols is proportional to the concentration of
Ca2+ or the ATP/ADP ratio. The size of the negative
sign is proportional to the amplitude of the inhibitory effect of
the modulatory pathways. See under "Discussion" for
explanation.
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Previous studies have clearly demonstrated that glucose-induced
[Ca2+]c oscillations of single pancreatic B-cells
or clusters of islet cells do not require the participation of the ER
(17, 47, 48). Our present data do not contradict these observations, but they strongly support the hypothesis that
[Ca2+]ER oscillations occur synchronously
with and in parallel to glucose-induced [Ca2+]c
oscillations. The parallel nature of these oscillations strikingly
contrasts with the antiparallel changes of IP3-induced [Ca2+]c and [Ca2+]ER
oscillations (13, 49, 50).
Physiological Implications--
In many cell types, emptying of
intracellular Ca2+ pools activates various types of
currents with distinct ion selectivity (Ca2+,
K+, or Na+) through a family of channels that
have been termed store-operated channels (51-54). It has recently been
demonstrated that the magnitude of the current activated by
intracellular pool emptying correlates with the extent of store
depletion and that it can be activated even by small decreases in
[Ca2+]ER (55). In pancreatic B-cells,
intracellular Ca2+ pool depletion activates a small
Ca2+ entry and induces a depolarizing current, possibly
carried by Na+, that potentiates the activation of
voltage-dependent Ca2+ channels (17, 56). This
was evidenced in the present study by the observation that in the
presence of 2.5 mM Ca2+ in the medium, TG
transformed oscillations of the membrane potential into a sustained
depolarization. It is therefore likely that oscillations of the
Ca2+ concentration within the ER rhythmically activate a
depolarizing current.
The model that we suggest is presented in Fig. 7. The membrane
potential of B-cells is controlled by several conductances, among which
the KATP current (IKATP) and the store-operated
current (ISOC) play major roles. In the presence of a
nonstimulating concentration of glucose, ISOC is too small
to counteract the overwhelming repolarizing current through
KATP channels. At stimulating glucose concentrations, IKATP is much reduced and can be counteracted by
ISOC (Fig. 7B). When
[Ca2+]c increases, the ER fills with
Ca2+, leading to decrease of ISOC and
repolarization of the plasma membrane (Fig. 7C).
Ca2+ influx through voltage-dependent
Ca2+ channels then stops, [Ca2+]c
decreases, and the ER starts to release more Ca2+ than it
takes up (Fig. 7D). The subsequent slow emptying of
intracellular Ca2+ pools reactivates ISOC and
the plasma membrane depolarizes again (Fig. 7B). This
increases [Ca2+]c, and a new cycle starts again.
The model depicted in Fig. 7 thus suggests that glucose controls the
membrane potential of B-cells partly indirectly, by modulating the
buffering capacity of the ER. It is fully compatible with our recent
model (45) indicating that IKATP might also oscillate
during [Ca2+]c oscillations. Before the onset of
[Ca2+]c oscillations, IKATP would be
small, when ISOC is large. At the end of
[Ca2+]c oscillations, it would be large, when
ISOC is small. Some mathematical models of the bursting
electrical activity of the pancreatic B-cell (57) also include a
mechanism by which oscillations of the Ca2+ concentration
within the ER concomitant with [Ca2+]c
oscillations control slow waves of the membrane potential. In contrast,
our model differs from that proposed by Dukes et al. (58),
which involves a depolarization- or IP3-induced emptying of
intracellular Ca2+ stores during the upstroke of
[Ca2+]c oscillation.
Conclusions--
The present study demonstrated that in pancreatic
B-cells, the ER plays a dual role during [Ca2+]c
oscillations. It attenuates [Ca2+]c rises by
rapidly taking up Ca2+ and delays
[Ca2+]c decreases by slowly releasing
Ca2+. Buffering the fast rise in
[Ca2+]c could protect the cell from
Ca2+ overload, whereas buffering the decrease in
[Ca2+]c prolongs the Ca2+ signal in
the cytosol. It is likely that oscillations of [Ca2+] in
the ER occur synchronously with [Ca2+]c
oscillations. They may have a major impact on the control of the
oscillations of the membrane potential and consequently on
[Ca2+]c oscillations themselves.