The mechanism by which agonist‐evoked cytosolic Ca2+ signals are terminated has been investigated. We measured the Ca2+ concentration inside the endoplasmic reticulum store of pancreatic acinar cells and monitored the cytoplasmic Ca2+ concentration by whole‐cell patch‐clamp recording of the Ca2+‐sensitive currents. When the cytosolic Ca2+ concentration was clamped at the resting level by a high concentration of a selective Ca2+ buffer, acetylcholine evoked the usual depletion of intracellular Ca2+ stores, but without increasing the Ca2+‐sensitive currents. Removal of acetylcholine allowed thapsigargin‐sensitive Ca2+ reuptake into the stores, and this process stopped when the stores had been loaded to the pre‐stimulation level. The apparent rate of Ca2+ reuptake decreased steeply with an increase in the Ca2+ concentration in the store lumen and it is this negative feedback on the Ca2+ pump that controls the Ca2+ store content. In the absence of a cytoplasmic Ca2+ clamp, acetylcholine removal resulted in a rapid return of the elevated cytoplasmic Ca2+ concentration to the pre‐stimulation resting level, which was attained long before the endoplasmic reticulum Ca2+ store had been completely refilled. We conclude that control of Ca2+ reuptake by the Ca2+ concentration inside the intracellular store allows precise Ca2+ signal termination without interfering with store refilling.
Cytosolic Ca2+ signals are generated in many different cell types by liberation of Ca2+ stored in the endoplasmic reticulum (ER) through special Ca2+ release channels known as inositol trisphosphate (IP3) and ryanodine receptors (Berridge, 1993; Clapham, 1995). The mechanisms by which Ca2+ release is controlled have been studied in considerable detail (for reviews, see Berridge, 1993, 1997; Petersen et al., 1994; Bootman and Berridge, 1995; Clapham, 1995), but much less information is available about the equally important control of the mechanism for precisely terminating cytosolic Ca2+ signals. An important element in the termination of short‐lasting Ca2+ spikes, is the negative feedback effect of Ca2+ on the IP3 receptor closing the Ca2+ release channel (Bezprozvanny et al., 1991). Ca2+ lost from the ER store must be taken up again, and it has been shown that even for the very shortlasting IP3‐evoked local Ca2+ spikes in the secretory granule area of pancreatic acinar cells, the duration of individual spikes is prolonged significantly by a specific inhibitor of the ER Ca2+ pump (Petersen et al., 1993). With regard to sustained cytosolic Ca2+ elevations evoked by sustained high agonist levels, the precise mechanism underlying signal termination is far from clear, but must involve ER Ca2+ reuptake (Camello et al., 1996).
Active Ca2+ uptake into intracellular stores was discovered by studying the nature of muscle relaxing factor (Kumagai et al., 1955; Ebashi and Lipmann, 1962). The active principle is a Ca2+, Mg2+‐activated ATPase in the sarco‐endoplasmic reticulum (SR/ER) membrane (Ebashi and Lipmann, 1962), and these enzymes are now generally referred to as SERCA pumps (sarco‐endoplasmic reticulum Ca2+‐ATPases) (Pozzan et al., 1994). The general principle of operation is simple: when the cytosolic Ca2+ concentration ([Ca2+]i) has been elevated due to release from intracellular stores, the SERCA pumps will be activated (by the rise in [Ca2+]i), and as soon as the SR/ER Ca2+ release channels have been closed, net Ca2+ reuptake will occur. When [Ca2+]i has been reduced to the resting (pre‐stimulation) level, the activation of the SERCA pumps ceases.
There could be an additional control mechanism operating on the luminal side of the SR/ER membrane. Studies of Ca2+ uptake into isolated SR or ER vesicles indicate that the SERCA pump‐mediated rise in the Ca2+ concentration in the intravesicular lumen leads to an inhibition of the SERCA pump in both muscle (Inesi and DeMeis, 1989) and non‐muscle cells, where a highly supralinear feedback inhibition of Ca2+ uptake by the Ca2+ load of ER vesicles has been described (Fauvre et al., 1996).
In intact cells, it is clear that in the period of Ca2+ reuptake into stores following an agonist‐induced release phase, [Ca2+]i will be falling, whereas the Ca2+ concentration in the lumen of the ER store ([Ca2+]Lu) must be rising. It is therefore not easy to determine whether the control from the inside or the outside is the most important or whether both are necessary. In the present study, we tested as directly as possible the hypothesis that Ca2+ reuptake into depleted Ca2+ stores may be regulated by changes in [Ca2+]Lu. We measured [Ca2+]Lu directly with a Ca2+‐sensitive fluorescent probe in the store lumen and were able, with the help of the whole‐cell recording configuration of the patch‐clamp technique, to clamp the cytosolic Ca2+ concentration at the resting level by a high buffer concentration. The effectiveness of the cytosolic Ca2+ clamping was confirmed directly by measurement of the Ca2+‐sensitive ion currents. We show that under such experimental conditions, in which acetylcholine (ACh) failed to evoke any rise in [Ca2+]i, even very close to the plasma membrane, Ca2+ stores are effectively depleted and upon ACh removal vigorous Ca2+ reuptake occurs that is totally dependent on a thapsigargin‐sensitive Ca2+ pump. In the Ca2+ reuptake period, where [Ca2+]i continues to be clamped, the rate of Ca2+ reuptake falls as [Ca2+]Lu rises and stops when the store is full. We have studied the relationship between the rate of active Ca2+ reuptake and [Ca2+]Lu. Whereas the Ca2+ leak is almost independent of [Ca2+]Lu at relatively high levels of [Ca2+]Lu, the Ca2+ reuptake decreases sharply with an increase of [Ca2+]Lu in the same range. It is therefore the steep dependence of the Ca2+ reuptake rate on [Ca2+]Lu that determines the ER calcium content. In experiments in which [Ca2+]i was not clamped, we show that after ACh removal [Ca2+]i returns quickly to the pre‐stimulation level which is attained long before [Ca2+]Lu has reached its steady‐state level. The control of Ca2+ reuptake by [Ca2+]Lu explains how a cytosolic Ca2+ signal can be terminated abruptly without preventing complete refilling of intracellular Ca2+ stores.
ACh‐evoked Ca2+ loss from intracellular stores and Ca2++ reuptake
Hofer and collaborators (Hofer and Machen, 1993; Hofer et al., 1995; Hofer and Schulz, 1996) described a technique to measure [Ca2+]Lu in permeabilized cells by loading the stores with the Ca2+‐sensitive fluorescent probe Mag‐fura 2. In intact cells, there is a problem with this technique since the probe would be present not only inside the stores, but also in the cytosol. Agonist stimulation would inevitably give rise to a complex signal due to the rise in [Ca2+]i and the fall in [Ca2+]Lu. We therefore used the whole‐cell recording configuration of the patch‐clamp technique (Hamill et al., 1981) to wash out the fluorescent probe molecules from the cytosol, after the loading of the cell, into the large volume of the patch pipette (Figure 1). In this way, the probe molecules were effectively only remaining inside the intracellular stores, and stimulation with a high concentration of ACh evoked a marked increase in the Ca2+‐sensitive fluorescence intensity at the excitation wavelength 380 nm, signalling a marked reduction in [Ca2+]Lu (Figure 1). The patch‐clamp whole‐cell recording configuration was useful not only for washing out the Ca2+‐sensitive probe from the cytosol, but also for allowing us to monitor changes in [Ca2+]i, by recording the current through the Ca2+‐sensitive ion channels (Osipchuk et al., 1990; Petersen, 1992).
There are two Ca2+‐activated currents in pancreatic acinar cells carried by the Ca2+‐sensitive non‐selective cation channels (Maruyama and Petersen, 1982) and the Ca2+‐sensitive Cl− channels (Wakui et al., 1989). In our experiments, the recorded current at a membrane potential of −30 mV (Wakui et al., 1989; Osipchuk et al., 1990) will be a mixture of Cl− and monovalent cation currents (Thorn and Petersen, 1992). The time course of this combined current is well correlated with the time course of changes in [Ca2+]i under a variety of conditions including stimulation with ACh (Osipchuk et al., 1990). Patch–clamp current recording is actually a more sensitive indicator of [Ca2+]i changes near the cell membrane than fluorescence measurements, as shown by Osipchuk et al. (1990) who could demonstrate Ca2+‐dependent current spikes in response to low doses of ACh which were not associated with any detectable changes in the bulk [Ca2+]i. With digital imaging, it could be shown that the short‐lasting Ca2+‐dependent current spikes evoked by low ACh concentrations were due to local cytosolic Ca2+ rises in the secretory pole (Thorn et al., 1993). With regard to the recordings presented here, it is important to emphasize that current measurements, also on a slow minute time scale, are extremely well correlated with [Ca2+]i, even at low levels of [Ca2+]i elevation. Thus, in experiments in which a slow intracellular Ca2+ infusion was followed by a slow infusion of the Ca2+ chelator EGTA, it could be shown that in the [Ca2+]i range 100–300 nM the current is slightly more sensitive to small changes in [Ca2+]i than the fura‐2 fluorescence ratio. The time courses of the [Ca2+]i changes measured simultaneously with the two methods were virtually identical (see Figure 8 in Osipchuk et al., 1990).
As seen in Figure 1, representing an experiment where a low Ca2+ buffer concentration (0.25 mM EGTA) had been included in the pipette solution, ACh evoked a marked rise in the whole‐cell inward current in the period where [Ca2+]Lu fell, demonstrating the normally expected rise in [Ca2+]i. [Ca2+]Lu remained low during the period of ACh stimulation but, after ACh removal, [Ca2+]Lu rose slowly and a sharp reduction in the Ca2+‐sensitive current was apparent, demonstrating the abrupt termination of the cytosolic Ca2+ signal. In seven experiments with a Ca2+ buffer (EGTA) concentration of 1 mM in the pipette, ACh still evoked a clear increase in the Ca2+‐sensitive current and induced a marked drop in [Ca2+]Lu from 152 ± 34 μM (SE) to 44 ± 7 μM. Removal of ACh resulted in a restoration of the pre‐stimulation Ca2+ level in the store lumen within a 1–2 min period. The maximal apparent rate of Ca2+ reuptake was 198 ± 27 μM/min (n = 7).
Ca2+ reuptake is due to a thapsigargin‐sensitive Ca2+ pump
In order to investigate the nature of the Ca2+ reuptake process, the effect of thapsigargin, the specific inhibitor of SERCA pumps (Thastrup et al., 1990), was tested. As seen in Figure 2, thapsigargin abolished Ca2+ reuptake in all regions of the acinar cells, indicating that we were, in these experiments, mainly studying Ca2+ release and reuptake into ER stores. Three experiments of this type giving similar results were carried out. The slightly lower [Ca2+]Lu in the apical region may reflect a contribution from Ca2+ in secretory granules. In a previous study of isolated granules, an average [Ca2+] of ∼50 μM was found in these organelles (Gerasimenko et al., 1996). We chose to base all quantification on results obtained from the basal (non‐nuclear) region, as this part of the cell is densely packed with ER (Kern, 1993; Gorelick and Jamieson, 1994). The similarity of the ACh‐evoked [Ca2+]Lu change in the different regions of the cell shown in Figure 2 does not contradict the previously clearly documented polarization of the agonist‐evoked cytosolic Ca2+ signals (Kasai et al., 1993; Thorn et al., 1993; Mogami et al., 1997). This phenomenon is seen most clearly when low agonist concentrations are used. When a supramaximal ACh concentration is used, as in the experiments reported here, Ca2+ is released all over the cell, but the [Ca2+]i rise occurs first in the apical region and then spreads across the cell. Under normal conditions, it takes 1–2 s for the Ca2+ wave to move from the apical region to the base of the cell (Kasai and Augustine, 1990; Toescu et al., 1992a). The new experiments described here were not designed to study this phenomenon and, because we wanted to study the slower uptake processes and therefore needed long recordings, our experiments did not have sufficient time resolution to reveal differences in the time course of Ca2+ release in different regions.
We also used thapsigargin in another protocol. In the experiment shown in Figure 3A, ACh induced, as usual, a marked reduction in [Ca2+]Lu and, after ACh removal, Ca2+ reuptake occurred. When [Ca2+]Lu had risen to a level close to the pre‐stimulation state, thapsigargin was added. This resulted in a gradual reduction of [Ca2+]Lu which became slower and slower as the store was emptied (Figure 3A). Thapsigargin evoked a slow, but complete Ca2+ release (to the same extent as ACh), following a Ca2+ reaccumulation period of the type shown in Figure 3A, in six experiments.
Ca2+ reuptake still occurs when [Ca2+]i is clamped near the resting level
When the Ca2+ buffer EGTA was present in the patch pipette solution in a concentration of 1 mM, it did not prevent ACh, in a maximally activating concentration (10 μM), from evoking an increase in the Ca2+‐sensitive ion currents across the plasma membrane. In order to clamp [Ca2+]i effectively, we therefore replaced the relatively slowly reacting EGTA with the faster Ca2+ buffer BAPTA (Tsien, 1980; Roberts, 1993) and also increased the buffer concentration to 10 mM. When the pipette was filled with a nominally Ca2+‐free solution containing 10 mM BAPTA, there was no response in two experiments and only a small response to ACh in one of the three experiments carried out and therefore also only a small Ca2+ reuptake following ACh removal in that same cell. Clearly, in this series, [Ca2+]i had been clamped at a level well below the normal resting concentration, probably preventing normal filling of the Ca2+ store.
In order to create better conditions for Ca2+ release and reuptake, we added 2 mM Ca2+ to the 10 mM BAPTA solution in the pipette. When [Ca2+]i was measured with the help of the fluorescent probe fura‐2 in the cytoplasm, a mean value of 96 ± 3.6 nM (n = 5) was obtained, which corresponds to the normal resting level in intact cells. In this condition, ACh (10 μM) evoked a sharp and very marked reduction in [Ca2+]Lu from 286 ± 63 μM (n = 6) to 38 ± 2 μM. After ACh removal, [Ca2+]Lu increased, first steeply and then more slowly as the store was being filled (Figure 3A). In this, as well as the other five experiments of the same type, [Ca2+]i had been effectively clamped, since the electrophysiological recording showed that ACh failed to induce any measurable change in the Ca2+‐sensitive ion current (Figure 3B). At the end of the experiments, the Ca2+ ionophore ionomycin evoked a sharp increase in the inward current, demonstrating the normal operation of the Ca2+‐sensitive ion channels. Comparing the response to ACh in Figures 1 and 3, it is clear that the time course of the Ca2+ release was different in the two experimental situations. In the experiments where the cytoplasmic Ca2+ buffer concentration was relatively low and where [Ca2+]i rose after ACh stimulation (Figures 1 and 2), it is apparent that the Ca2+ loss occurred in two phases: an initial fast Ca2+ liberation followed by a very much slower outflow. In contrast, when [Ca2+]i was clamped near the resting level by a high BAPTA concentration (Figure 3), this late and very slow release phase was completely absent. The rise in [Ca2+]i that normally occurs provides a negative feed‐back for the Ca2+ release channels (Bezprozvanny et al., 1991; Berridge, 1993; Clapham, 1995), and our finding illustrates that removal of this effect by heavily buffering the cytoplasmic compartment prevents the slowing down of the Ca2+ release process. A similar conclusion has been reported very recently by Montero et al. (1997).
In spite of the data shown in Figure 3B indicating that the [Ca2+]i clamp is effective (since there is no activation of Ca2+‐dependent ion current during the ACh‐evoked Ca2+ loss from the ER), it might be postulated that there could be small domains of elevated [Ca2+]i near the inner mouths of the store‐operated Ca2+ channels in the plasma membrane that could play a functional role in activating the Ca2+ pumps in the ER. We therefore tested the effect of removing external Ca2+ immediately after discontinuing ACh stimulation. In each of these four experiments, the Ca2+ reuptake proceeded as normal (with a time course similar to what is shown in Figure 3), indicating that with the well‐buffered pipette solution, the availability of Ca2+ for reuptake into the stores did not depend on Ca2+ in the external solution. In these experiments, there cannot of course exist local domains of elevated Ca2+ concentration near the inner mouths of the Ca2+ channels as there was no supply of external Ca2+. The Ca2+ for the refilling of stores in these experiments is therefore provided by the Ca2+ in the BAPTA/Ca2+ mixture in the large volume of the patch pipette.
The rates of Ca2+ reuptake and Ca2+ leak depend on the Ca2+ concentration in the store lumen
Experiments of the type shown in Figure 3, where thapsigargin application after the period of Ca2+ reuptake allowed calculation of the apparent passive Ca2+ leak, could be used to derive the relationship between the apparent rate of active Ca2+ reuptake into the stores and [Ca2+]Lu. Figure 3C shows the graph representing this relationship, derived from the experimental record displayed in Figure 3A. The apparent rate of Ca2+ reuptake was high when [Ca2+]Lu was low, and was reduced gradually as [Ca2+]Lu increased. The apparent Ca2+ leak was almost independent of [Ca2+]Lu above a concentration of 100 μM, whereas in this range the apparent Ca2+ reuptake rate still displayed a relatively steep dependency on [Ca2+]Lu. In the [Ca2+]Lu range 40–100 μM, the apparent leak rate was strongly dependent on [Ca2+]Lu, rising initially sharply and then more slowly with a rise in this parameter. The maximal leak rate, when the Ca2+ store was full, was surprisingly high (19 ± 4 μM/min; n = 6), but nevertheless, relatively small compared with the maximal reuptake rate following ACh removal (95 ± 7 μM/min). The apparent rate of active Ca2+ uptake, mediated by the SERCA pumps, can therefore be increased by a factor of 5 from the resting minimum when the ER store is maximally depleted. The leak rate is, as expected, very small compared with the very rapid loss of Ca2+ from the store immediately after ACh application (27 ± 8 μM/s). It is an important assumption underlying the calculation of the Ca2+ uptake and leak rates that the thapsigargin action is exclusively on the pump and that it has no effect on the leak. Furthermore, it is important that thapsigargin acts quickly. We used a high concentration of thapsigargin to ensure an immediate effect. On the time scale relevant to our experiments, the action of thapsigargin would appear to be virtually instantaneous (Sagara et al., 1992). There is also clear experimental evidence showing that thapsigargin, in contrast to several other SERCA pump inhibitors, has no effect on passive Ca2+ permeability across the ER membranes (Missiaen et al., 1992).
We analysed the four experiments in which the [Ca2+]Lu range 100–200 μM had been fully explored. Figure 3D shows the mean values obtained for apparent Ca2+ reuptake (leak corrected) and apparent Ca2+ leak. Irrespective of whether linear or exponential extrapolation is used, the curves will cross, giving an equilibrium value for [Ca2+]Lu. Figure 3D indicates that this equilibrium would be reached between 260 and 330 μM, which is consistent with the resting [Ca2+]Lu values measured in this series of experiments (Figure 3A).
All the [Ca2+]Lu measurements described so far in this report have been based on the use of the Ca2+‐sensitive fluorescent probe Mag‐fura‐2. This probe is, however, also sensitive to Mg2+ (although with a much lower affinity than for Ca2+), and we therefore decided to carry out some experiments with the Ca2+‐selective probe fura‐2FF. These five experiments gave results of the type shown in Figure 3. The [Ca2+]i was clamped exactly as in the Mag‐fura 2 experiments (10 mM BAPTA/2 mM Ca2+). Following ACh‐evoked Ca2+ store depletion, removal of ACh led to a fast Ca2+ reuptake into the ER. The apparent rate of uptake declined sharply as [Ca2+]Lu approached the normal resting (equilibrium) level, whereas the leak was virtually linear at [Ca2+]Lu above ∼50 μM. The maximal apparent Ca2+ uptake rate was 138 ± 40 μM/min (n = 5), whereas the maximal apparent leak rate was 19 ± 4 μM/min (n = 5).
Ca2+ reuptake into intracellular stores, after agonist‐evoked depletion, is potentially the most powerful mechanism for terminating a cytosolic Ca2+ signal (Petersen et al., 1994; Pozzan et al., 1994; Camello et al., 1996). We have now demonstrated that this Ca2+ reuptake cannot be prevented by clamping [Ca2+]i at the resting level. This indicates that there must be control of Ca2+ store reuptake from the inside of the store membrane. We have provided direct evidence for the effectiveness of our [Ca2+]i clamp and excluded the possibility that store reloading depends on local domains of elevated Ca2+ near the inner mouths of store‐operated Ca2+ channels in the plasma membrane. Our findings, that Ca2+ reuptake does not depend on an elevated cytosolic Ca2+ level (Figure 3) and largely occurs during a period when [Ca2+]i has already returned to the pre‐stimulation resting level (Figure 1), should not be taken to indicate that the ER Ca2+ pumps cannot be stimulated by a rise in [Ca2+]i. The initial apparent maximal Ca2+ reuptake rate was higher in the experiments where [Ca2+]i was not clamped (∼200 μM/min) than in the experiments where [Ca2+]i was clamped at the resting level (∼100–150 μM/min). Under normal conditions, the elevated [Ca2+]i that still exists immediately after cessation of agonist exposure most likely provides an additional stimulus for the ER Ca2+ pump.
Our finding has considerable implications for the Ca2+ signalling process. Figure 4 summarizes our conclusions. A prolonged cytosolic Ca2+ signal generated by a maximal agonist concentration is illustrated. We focus attention on the four main Ca2+ transport events across the plasma and ER membranes in the various phases. In the steady‐state resting situation (1), the Ca2+ fluxes are at a minimum, [Ca2+]i is ≈100 nM and [Ca2+]Lu is at its maximum (100–300 μM). ACh evokes opening of the Ca2+ release channels in the ER, elevating [Ca2+]i. The elevated [Ca2+]i activates the plasma membrane (PM) Ca2+ pumps markedly enhancing the extrusion rate (Tepikin et al., 1992a, b). The fall in [Ca2+]Lu will remove an inhibitory influence on the ER Ca2+ reuptake mechanism, but because the Ca2+ release channels remain open during agonist application, there is no net Ca2+ reuptake (Camello et al., 1996) (2). When the agonist is removed, the ER Ca2+ release channels close. Because [Ca2+]Lu is low, Ca2+ reuptake is maximal and net uptake can now occur. [Ca2+]i falls rapidly and has returned to the resting pre‐stimulation level at a point in time when [Ca2+]Lu is still far from its resting pre‐stimulation level (3). In order to understand this, it is necessary to appreciate that a major proportion of the Ca2+ lost from the store is not in the cytosol, but has been removed from the cell by the PM Ca2+ pumps. Phase (3) in Figure 4 illustrates the crucial point established by our new results. Because Ca2+ reuptake proceeds vigorously at resting [Ca2+]i, the cytosolic Ca2+ signal can be terminated very sharply upon agonist removal (Figure 1) (as indeed documented in very many investigations, for example, Yule et al., 1991; Toescu et al., 1992b; Camello et al., 1996) without impairing Ca2+ refilling of the store, which continues after [Ca2+]i has returned to the pre‐stimulation level (Figure 1). In this phase (3), Ca2+ for store refilling comes from the external solution, due to opening of the capacitative Ca2+ entry channel (store‐operated Ca2+ channel) (Putney, 1990; Berridge, 1997). The quick termination of the cytosolic Ca2+ signal after agonist removal is not only essential from the point of view of signalling precision but, because it terminates Ca2+ extrusion by the PM Ca2+ pumps, it is also energy saving and enhances the rate of net Ca2+ entry thereby helping to supply the Ca2+ necessary for refilling the store. As [Ca2+]Lu increases, the degree of capacitative Ca2+ entry decreases and the rate of Ca2+ reuptake slows down until phase (4), which is identical to (1), has been reached.
Figure 4 makes it clear that the at first sight surprising observation, that Ca2+ reuptake does not require an elevated [Ca2+]i, is in fact an essential feature of effective Ca2+ signal termination. If Ca2+ reuptake could only occur at an elevated [Ca2+]i, the cytosolic Ca2+ signal could not be fully terminated until the store had been entirely refilled and the ER Ca2+ reuptake pump would compete with the PM Ca2+ extrusion pump. Our results also point to an important correlation between the Ca2+ reuptake into the ER and the capacitative Ca2+ entry process. In our model, these two transport events cannot be dissociated. During the refilling phase (phase 3 in Figure 4), the rates of Ca2+ reuptake into the ER and the capacitative Ca2+ entry must be exactly matched at all levels of [Ca2+] in the ER store.
Our findings may also be relevant to a situation in which part of the Ca2+ released from the ER has been taken out of the cytosol by uptake into the mitochondria (Pozzan et al., 1994). Ca2+ refilling of the ER store from mitochondria could occur without any [Ca2+]i elevation and would stop exactly when the ER store was full, due to the steep dependence of Ca2+ reuptake on [Ca2+]Lu (Figure 3C and D). If ER Ca2+ reuptake were dependent on a [Ca2+]i elevation, Ca2+ accumulated in the mitochondria could not be given back to the ER without generating at least local Ca2+ signals, and this process might involve an undesirable activation of PM Ca2+ pumps.
Although the ER operates as one luminally continuous store for both Ca2+ (Renard‐Rooney et al., 1993; Mogami et al., 1997) and macromolecules (Subramanian and Meyer, 1997), there can be differences in the Ca2+ transport characteristics in different parts of the cell. In the polarized pancreatic acinar cells, the Ca2+ release mechanism operates with the highest sensitivity in the apical granule region, and low agonist concentrations can evoke cytosolic Ca2+ signals that are confined entirely to this part of the cell (Kasai et al., 1993; Thorn et al., 1993). It is possible to create conditions under which the Ca2+ reuptake into the store, that has been depleted primarily in the apical granule region, occurs exclusively in the basal part of the cell without causing any [Ca2+]i rise there (Mogami et al., 1997). Our new results explain how this is possible. The process whereby substantial Ca2+ reuptake into the ER can take place in the absence of any [Ca2+]i elevation ensures that Ca2+ signals only occur where and when Ca2+ release channels open and not during phases of Ca2+ store refilling in places where Ca2+ signals are not intended. It is helpful in this respect that the crucial Ca2+ export from the pancreatic acinar cells during the phase of agonist‐induced Ca2+ release from internal stores (phase 2 in Figure 4) occurs preferentially in the apical region (Belan et al., 1996, 1997; Lee et al., 1997) close to the primary Ca2+ release sites (Kasai and Augustine, 1990; Toescu et al., 1992a; Kasai et al., 1993; Thorn et al., 1993, 1996; Mogami et al., 1997).
The Ca2+ leak from the ER to the cytosol is substantial. The apparent maximal leak rate is only about five times smaller than the apparent maximal uptake rate. This means that there must be considerable energy expenditure in order to ensure the high [Ca2+]Lu that is necessary in order both to achieve rapid messenger‐mediated Ca2+ mobilization (Montero et al., 1995) and to prevent accelerated protein degradation (Wileman et al., 1991). It is possible that the translocons (Simon and Blobel, 1991) in the rough ER, which dominates the basolateral regions of the pancreatic acinar cells where the major Ca2+ release (leak) following thapsigargin inhibition occurs (Toescu et al., 1992a; Gerasimenko et al., 1996), impose limitations on the degree of impermeability to ions, but we do not know the nature of the leak pathway. Since the Ca2+ content of the ER is so important for preserving essential proteins (Wileman et al., 1991), it must be finely regulated. Our study shows that it is the relatively steep dependence of the Ca2+ reuptake rate on [Ca2+]Lu that determines the store Ca2+ content (Figure 3D). In this context, the high Ca2+ leak rate, although slightly uneconomical, is helpful in defining [Ca2+]Lu relatively precisely.
Materials and methods
Single isolated mouse pancreatic acinar cells were prepared using collagenase (Worthington) digestion as described previously (Osipchuk et al., 1990).
The extracellular (bath) solution contained (mM): NaCl 140, KCl 4.7, MgCl2 1.13, CaCl2 1, glucose 10 and HEPES‐NaOH 10 (pH 7.3). In some experiments, CaCl2 was not included (Ca2+‐free solution). Pipette solution I contained (mM): KCl 120, NaCl 20, MgCl2 1.13, ATP 2 and HEPES‐KOH 10 (pH 7.2). [Ca2+] was buffered with EGTA (0.25 or 1 mM). Pipette solution II contained (mM): KCl 110, NaCl 20, MgCl2 1.13, ATP 2 and HEPES‐KOH 10 (pH 7.2). [Ca2+] was clamped using a BAPTA/Ca2+ mixture containing 10 mM BAPTA and 2 mM CaCl2. The cells, placed on a glass coverslip attached to an open perifusion chamber, were perifused continuously from a gravity‐fed system. Bath solution changes at the cell occurred after <7s in this system. All experiments were performed at room temperature.
Ca2+ measurement in intracellular stores
The isolated acinar cells were incubated with 2.5 μM Mag‐fura 2 AM and 0.01% pluronic F‐127 for 10–15 min at 37°C, then washed twice and used within 4 h. Before the establishment of the patch–clamp whole‐cell recording configuration, there was intense fluorescence throughout the cell (Figure 1Aa). It is reasonable to assume that at this stage the fluorescent probe is present both inside organelles and in the cytoplasm. In order to wash out the cytoplasmic probe content, a patch pipette was sealed to the cell membrane and the membrane area covered by the pipette disrupted by suction to establish the whole‐cell recording configuration (Hamill et al., 1981). The overall fluorescence intensity was markedly reduced by this procedure and, as seen in Figure 1Ab, 15 min after starting the wash out into the pipette, the two nuclei (in this particular cell) had a very low concentration of the probe.
Fluorescence images were captured using the set‐up previously described (Mogami et al., 1997). Alternate excitation wavelengths of 340 and 380 nm from a Xenon light source were used. Three regions of interest were selected: the apical pole, the basal pole including the nucleus and the basal pole excluding the nucleus. The ratio (340/380) of fluorescence intensities in these regions was used to calculate [Ca2+] in the stores. The Mag‐fura 2 fluorescence ratio was calibrated using exposure to 10 μM ionomycin and 15 mM Ca2+ or 10 mM EGTA, assuming a dissociation constant for Ca2+–Mag‐fura 2 at room temperature of 53 μM. Since Mag‐fura 2 is also Mg2+‐sensitive (although with a much lower affinity than for Ca2+), we attempted to assess to what extent Mg2+ had an influence on our measurements by lowering [Mg2+] in the pipette solution to 0.113 mM. In three experiments of this type, the ACh (10 μM)‐evoked reduction in [Ca2+]Lu and the subsequent reuptake were very similar to those obtained in the presence of the standard 1.13 mM MgCl2 solution, indicating that the influence of Mg2+ on the fluorescence ratio is relatively minor. We also carried out five experiments with the Ca2+‐selective probe fura 2‐FF. The procedures for loading the cells with the probe (2.5 μM fura 2‐FF‐AM and 0.01% pluronic F‐127, 10–15 min at 37°C) and washing it out from the cytoplasm were similar to what has been described above for Mag‐fura 2. The excitation wavelengths were 340 and 380 nm and the fluorescence was recorded at 510 nm. Calibration was carried out as described above for Mag‐fura 2, assuming a dissociation constant of 35 μM for Ca‐fura 2‐FF (Hajnoczky and Thomas, 1997). With regard to the precision of [Ca2+]Lu measurements, the reader is referred to the discussion of this point by Hofer and Schulz (1996).
An initial analysis (Figure 2) indicated that [Ca2+]Lu changes in response to ACh application and removal were very similar in the three selected regions of interest. Since the basal non‐nuclear region is totally dominated by ER (Kern, 1993; Gorelick and Jamieson, 1994), this suggests that with our experimental protocol we are essentially measuring [Ca2+]Lu in the ER. The quantitative part of our analysis was based exclusively on measurements from the basal region of the cells excluding the nuclei. It cannot be excluded that the kinetics of Ca2+ release and uptake are influenced by the Ca2+ buffer component contributed by Mag‐fura 2 or fura 2‐FF; however, our estimates indicate that the additional buffering due to the presence of these dyes is probably only a small proportion of the overall buffering.
Cytosolic Ca2+ measurements
Calibration of [Ca2+]i was carried out using fura 2 applied through the patch pipette. The Rmin value was obtained with a pipette solution containing 10 mM BAPTA whereas Rmax was obtained when the cell was incubated with 15 mM CaCl2 in the presence of 10 μM ionomycin using a Kd for Ca2+–fura 2 of 150 nM.
Patch–clamp whole‐cell current recording
Standard patch–clamp whole‐cell current recording was used (Hamill et al., 1981; Osipchuk et al., 1990; Thorn and Petersen, 1992). The electrophysiological recording of Ca2+‐sensitive Cl− and non‐selective cation currents is a very sensitive measure of [Ca2+]i changes (Osipchuk et al., 1990; Thorn et al., 1993, 1996). We usually recorded the Ca2+‐sensitive currents when the membrane potential was clamped at −30 mV. Under our experimental conditions, the equilibrium potentials for both the Ca2+‐sensitive cation current and the Cl− current were close to 0.
This work was supported by a Medical Research Council Programme Grant (G 8801575).
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