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First published online 11 December 2007
doi: 10.1242/jcs.014522
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Research Article |
Strathclyde Institute of Pharmacy and Biomedical Sciences, University of Strathclyde, John Arbuthnott Building, 27 Taylor Street, Glasgow, G4 0NR, UK
* Author for correspondence (e-mail: J.McCarron{at}strath.ac.uk)
Accepted 16 October 2007
| Summary |
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m) to limit ATP production. To investigate how physiological Ca2+ signaling might affect energy production, 
m was examined during Ca2+ oscillations in smooth muscle cells. In single, voltage-clamped smooth muscle cells, inhibition of mitochondrial Ca2+ accumulation inhibited inositol (1,4,5)-trisphosphate [Ins(1,4,5)P3]-evoked Ca2+ release and prolonged the time required for restoration of [Ca2+]c following activation of plasmalemmal Ca2+ currents (ICa). Ca2+ could be released from mitochondria immediately (within 15 seconds) after a [Ca2+]c rise evoked by Ins(1,4,5)P3 or ICa. Despite this evidence of mitochondrial Ca2+ accumulation, no change in 
m was observed during single or repetitive [Ca2+]c oscillations evoked by these conditions. Occasionally, spontaneous, repetitive, persistent Ca2+ oscillations were observed. In these cases, mitochondria displayed stochastic 
m depolarizations, which were independent both of events in neighboring mitochondria and of the timing of the [Ca2+]c oscillations themselves. Such 
m depolarizations could be mimicked by increased exposure to either fluorescence excitation light or the 
m-sensitive dye tetramethylrhodamine ethyl ester (TMRE) and were inhibited by antioxidants (ascorbic acid, catalase, Trolox and TEMPO) or the mitochondrial permeability transition pore (mPTP)-inhibitor cyclosporin A (CsA). Individual mitochondria within smooth muscle cells might depolarize during repetitive Ca2+ oscillations or during oxidative stress but not during the course of single [Ca2+]c transients evoked by Ca2+ influx or store release.
Key words: Smooth muscle, Calcium, Mitochondria, Membrane potential
| Introduction |
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100 nM, using the potential, 
m, generated across the inner mitochondrial membrane by the activity of the electron-transport chain (Becker et al., 1980
Mitochondria, being the site of aerobic ATP production, also affect cellular signaling by modulating the cytosolic ATP:ADP ratio (Nicholls and Ferguson, 2002
). ATP production is itself stimulated by the uptake of Ca2+. The activity of the mitochondrially located citric acid (Krebs)-cycle enzymes pyruvate dehydrogenase, oxoglutarate dehydrogenase and NAD+-isocitrate dehydrogenase (McCormack and Denton, 1980
) as well as that of the F1F0-ATP synthase are stimulated by Ca2+ (Territo et al., 2000
). Conversely, a decrease in 
m, which provides the driving force for the ATP synthase, inhibits ATP production (Leyssens et al., 1996
). Uptake of positively charged Ca2+ ions should depolarize 
m to some extent and so might restrict ATP production. Therefore, Ca2+ signals might limit cellular energy production.
In some cells, mitochondria are located close to sites of initiation of [Ca2+]c signals, such as at voltage-gated Ca2+ channels on the plasmalemma (Barstow et al., 2004
) or at inositol 1,4,5-trisphosphate [Ins(1,4,5)P3] receptors [Ins(1,4,5)P3Rs] on the endoplasmic/sarcoplasmic reticulum (ER/SR) (Csordas and Hajnoczky, 2003
; Hajnoczky et al., 1999
; Rizzuto et al., 1998
). Indeed, mitochondria might be tethered to be within 10 nm of Ins(1,4,5)P3Rs (Csordas et al., 2006
). At these locations, mitochondria are exposed to a local [Ca2+]c that exceeds bulk average values (Rizzuto et al., 1998
), and hence might be expected to both have a greater influence over the [Ca2+]c signal itself (because of their low affinity for Ca2+) and, in turn, be more likely to exhibit a decrease in 
m due to the larger mitochondrial Ca2+ current generated during these local [Ca2+]c transients.
Although transient decreases in 
m have been observed in isolated mitochondria that have been exposed to sudden increases in [Ca2+] (Brustovetsky and Dubinsky, 2000
; Huser et al., 1998
), it is less clear whether or not this occurs during [Ca2+]c signaling in intact cells. Transient, or `flickering', 
m changes have been observed in some (Buckman and Reynolds, 2001
; Drummond et al., 2000
; Duchen et al., 1998
; Haak et al., 2002
; Jacobson and Duchen, 2002
; Kaftan et al., 2000
; O'Reilly et al., 2004
; Petronilli et al., 2001
) but not all (Collins et al., 2001
; Csordas and Hajnoczky, 2003
) intact cell types, although their relationship to [Ca2+]c changes is uncertain. Whether or not transient 
m depolarizations are seen during cellular Ca2+ signals might depend on the cell type, the origin and the characteristics of the Ca2+ signal. For example, inhibition of Ca2+ release from the SR inhibits transient 
m depolarizations in some circumstances (Jacobson and Duchen, 2002
) but not in others (O'Reilly et al., 2004
).
Transient 
m depolarizations have also been attributed to the increased levels of oxidative species generated from a combination of intense excitation light and high concentrations of certain mitochondrial dyes (Szado et al., 2003
), rather than to changes in [Ca2+]c. In yet other studies, neither the intensity of the excitation light nor the concentration of mitochondrial dyes contributed to the generation of transient 
m depolarizations (Buckman and Reynolds, 2001
; O'Reilly et al., 2004
; Vergun et al., 2003
). Evidently, the mechanism(s) underlying the generation of 
m depolarizations and, in particular, whether or not Ca2+ signals arising from either influx or release modulate 
m is unclear.
Cellular Ca2+ signaling imposes an energy burden on the cell (in order to rebalance resting ion concentrations) and paradoxically also impedes the production of ATP by mitochondria if Ca2+ signals result in 
m depolarization. The question of whether or not mitochondrial Ca2+ uptake depolarizes mitochondria was addressed in the present study. To examine how mitochondria affect Ca2+ signals and whether or not changes in 
m occur, 
m was measured during [Ca2+]c transients evoked by Ca2+ influx across the plasmalemma and following Ca2+ release from the SR by localized photolysis of caged Ins(1,4,5)P3, in voltage-clamped single smooth muscle cells. Voltage clamp was used because changes in plasmalemmal potential might compromise the ability to resolve mitochondrial 
m changes (Ward et al., 2000
). The use of caged Ins(1,4,5)P3 should minimize the number of second-messenger systems that are operative, which otherwise might also alter 
m independently of Ca2+ changes. With attenuated light intensity and low concentrations of the 
m indicator tetramethylrhodamine ethyl ester (TMRE), only minimal 
m changes were observed under resting conditions. 
m depolarizations did not occur when [Ca2+]c was increased by Ca2+ influx via voltage-gated Ca2+ channels or by release from Ins(1,4,5)P3Rs, even though mitochondrial Ca2+ uptake took place. However, 
m depolarizations were observed on increasing TMRE concentration or light intensity even though no change in [Ca2+]c took place. These depolarizations were blocked by antioxidants or the mitochondrial permeability transition pore (mPTP)-inhibitor cyclosporin A (CsA). Very occasionally, transient 
m depolarization was seen in cells undergoing sustained, spontaneous [Ca2+]c oscillations. In this case, 
m depolarizations were neither synchronized throughout the mitochondrial complement nor with changes in [Ca2+]c. Therefore, during physiological Ca2+ signaling, mitochondrial Ca2+ uptake modifies the amplitude and duration of Ca2+ signals without significantly altering 
m, unless [Ca2+]c oscillations are repetitive and sustained.
| Results |
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m between the two depolarization events, in order to examine the influence of mitochondrial Ca2+ accumulation upon ICa-evoked [Ca2+]c increases. The proton uncoupler carbonyl cyanide 3-chlorophenylhydrazone (CCCP, 1 µM) and the ATP synthase blocker oligomycin (6 µM) slowed the 50% recovery time (134±13% of the first pulse; n=9, P<0.05 compared with vehicle-treated controls, Fig. 1A), as did mitochondrial depolarization with rotenone (5 µM) plus oligomycin (123±12%; n=8, P<0.05 compared with controls). Oligomycin alone does not alter ICa-evoked [Ca2+]c transients in these cells (McCarron and Muir, 1999
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Mitochondria also regulate Ins(1,4,5)P3-mediated Ca2+ release from the SR. Local photolytic release of Ins(1,4,5)P3 from the caged compound evoked reproducible increases in [Ca2+]c, the second transient was 93±5% of the first Ins(1,4,5)P3-evoked [Ca2+]c peak (amplitude of first 2.86±0.63 F/F0, amplitude of second 2.78±0.91 F/F0, n=9, P>0.05; where F indicates fluorescence counts and F0 indicates baseline values before stimulation). To examine the influence of mitochondrial Ca2+ accumulation upon Ins(1,4,5)P3-evoked [Ca2+]c increases, mitochondrial Ca2+ uptake was again inhibited by pharmacological depolarization of 
m using either CCCP or rotenone 60 seconds prior to the second Ins(1,4,5)P3 release. 
m depolarization substantially reduced the second Ins(1,4,5)P3-evoked [Ca2+]c rise. CCCP (1 µM) plus oligomycin (6 µM) caused a decline in the peak of the second Ins(1,4,5)P3-evoked [Ca2+]c amplitude to 47±9% of that obtained prior to application of these drugs (n=13, P<0.01, Fig. 1B). 
m depolarization with rotenone (5 µM) plus oligomycin (6 µM) also reduced the peak of the second Ins(1,4,5)P3-evoked [Ca2+]c transient to 49±10% of that occurring prior to 
m depolarization (n=11, P<0.01). Inhibition of mitochondrial Ca2+ uptake with Ru360 – a specific inhibitor of the mitochondrial uniporter (Matlib et al., 1998
) – also inhibited Ins(1,4,5)P3-evoked Ca2+ release to 86±8% of control (from 2.01±0.26 F/F0 in control to 1.72±0.16 F/F0 with Ru360; n=3, P<0.05). Again, oligomycin alone did not alter Ins(1,4,5)P3-induced [Ca2+]c transients (McCarron and Muir, 1999
).
The influence of mitochondrial Ca2+ uptake on [Ca2+]c transients evoked by the Ins(1,4,5)P3-generating agonist carbachol (CCh, 100 µM by pressure ejection) was also examined. In vehicle-treated controls, CCh evoked a large, reproducible transient rise in [Ca2+]c (Fig. 1C). There was no difference in peak [Ca2+]c evoked by two successive applications of CCh, 2 minutes apart (the second peak [Ca2+]c transient was 108±5% of the first, n=3, P>0.05). 
m depolarization with CCCP (1 µM) plus oligomycin (6 µM) 60 seconds prior to the second CCh application decreased the evoked [Ca2+]c transient amplitude to 8±7% of the first (n=3, P<0.01, Fig. 1C). 
m depolarization with rotenone (5 µM) plus oligomycin (6 µM) caused the CCh-evoked [Ca2+]c transient amplitude to decline to 62±9% of that prior to application of the drugs (n=3, P<0.01). On the other hand, Ca2+ release evoked by the RyR agonist caffeine (10 mM) was not significantly altered by 
m depolarization (Fig. 1D, peak Ca2+ was 1.76±0.23 F/F0 prior to, and 1.78±0.24 F/F0 after CCCP plus oligomycin treatment, n=6, P>0.05). This latter result suggests that 
m depolarization had not significantly depleted the SR of Ca2+. Together, these results suggest that, when polarized, mitochondria modulate [Ca2+]c increases arising both from influx of extracellular Ca2+ and from Ca2+ release from intracellular stores via Ins(1,4,5)P3R.
Relationship between [Ca2+]c and 
m
Ca2+ uptake by the mitochondrial uniporter is driven by 
m (Nicholls and Crompton, 1980
) and might itself depolarize 
m (Duchen et al., 1998
; Kaftan et al., 2000
). Accordingly, 
m was measured to determine whether or not depolarization occurred during transient [Ca2+]c rises evoked by either ICa activation or Ins(1,4,5)P3. Changes in [Ca2+]c and 
m were measured simultaneously with Fluo-4 AM (10 µM) and TMRE (10 nM), respectively, in single colonic myocytes. The long wavelength Ca2+ indicator (Fluo-4) was necessary because the requirement for ultra violet (UV)-sensitive caged Ins(1,4,5)P3 precluded the use of ratiometric Ca2+ indicators such as Fura-2, which are excited by UV light. Despite the overlap of the excitation and emission spectra of Fluo-4 and TMRE, independent signals were resolved using selective dichroic mirrors, filters and excitation wavelengths (Fig. 2A) as described in the Materials and Methods. Separation of Fluo-4 and TMRE signals was established by first examining the fluorescence properties of cells loaded separately with each dye (Fig. 2B). Cells loaded with Fluo-4 alone showed barely detectable fluorescence when excited at 560 nm (the wavelength used for excitation of TMRE). Conversely, when cells were loaded with TMRE alone and excited at 475 nm, only a small fluorescence signal was detected, which was less than 5% of that obtained when either TMRE was excited at 560 nm or Fluo-4 at 475 nm (Fig. 2Bii). The separation of the signal from each indicator was confirmed in cells co-loaded with Fluo-4 and TMRE. ICa activation (depolarization to +10 mV from –70 mV for 500 ms) caused a large transient increase in Fluo-4 fluorescence with no change in TMRE fluorescence (Fig. 2D). Subsequent 
m depolarization with CCCP (1 µM) did not alter [Ca2+]c (McCarron and Muir, 1999
), causing a large decrease in TMRE fluorescence with no decrease in Fluo-4 fluorescence (Fig. 2D). The extensive co-localization of TMRE with the mitochondrial stain MitoTracker Green confirmed that TMRE partitioned largely to mitochondria (Fig. 2C).
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m depolarization caused a large decrease in TMRE fluorescence of individual mitochondria (–0.113±0.016
F/F0 20 seconds after CCCP, 1 µM, compared with –0.0025±0.0012
F/F0 in untreated control, n=3, P<0.01, Fig. 3). To examine whether much smaller changes in 
m could be detected than those caused by CCCP (
100 mV), oligomycin (6 µM) was used to inhibit the mitochondrial ATP synthase. Inhibition of the synthase causes a small 
m hyperpolarization (
5-10 mV) due to blockade of proton re-entry into the mitochondrial matrix (Ward et al., 2000
F/F0 20 seconds after oligomycin, n=3, P<0.01 compared to untreated control, –0.0025±0.0012
F/F0, n=3, Fig. 3). These results indicated that both large and small alterations of 
m could be detected in individual mitochondria.
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m immediately after either Ins(1,4,5)P3 release or ICa activation (Fig. 4). In the first series of experiments, [Ca2+]c and 
m were monitored simultaneously, and mitochondria were then depolarized rapidly with CCCP (20 µM, applied by pressure ejection from a pipette
50 µm from the cell) at 2, 5 or 15 seconds after localized photolytic release of Ins(1,4,5)P3. Mitochondrial depolarization (as shown by the drop in the averaged TMRE fluorescence of three individual mitochondrial regions, Fig. 4A, red line) evoked a transient increase in [Ca2+]c (Fig. 4A, blue line). The increase in [Ca2+]c presumably arose by mitochondrial Ca2+ release via uniporter reversal upon 
m depolarization. The extent of mitochondrial Ca2+ loading, measured as the time-integrated Fluo-4 fluorescence signal in the 10-second period after CCCP application less that of the control Ins(1,4,5)P3-evoked [Ca2+]c transient (gray shaded area in Fig. 4A), declined with time after Ins(1,4,5)P3 release (Fig. 4B, summarized data from n=3 cells for each data point). Significant mitochondrial Ca2+ release still occurred 15 seconds after Ins(1,4,5)P3 release, even though [Ca2+]c had returned to baseline values
5 seconds after Ins(1,4,5)P3 release. In the next series of experiments, rapid 
m depolarization after ICa activation also evoked a transient [Ca2+]c elevation (Fig. 4C). The extent and duration of this [Ca2+]c rise was less than that evoked after Ins(1,4,5)P3-stimulated [Ca2+]c transients (Fig. 4D), despite similar peak [Ca2+]c levels being evoked by ICa and Ins(1,4,5)P3. These results suggest that mitochondria accumulate Ca2+ following Ins(1,4,5)P3R and voltage-operated Ca2+ channel activation.
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m during [Ca2+]c transients evoked either by Ins(1,4,5)P3 or ICa activation
To evaluate whether or not [Ca2+]c increases altered 
m of individual mitochondria in single colonic myocytes, TMRE fluorescence of individual mitochondria was monitored during increases in [Ca2+]c evoked either by UV flash-photolysis of caged-Ins(1,4,5)P3 or by ICa activation (depolarization to +10 mV for 500 ms). ICa-evoked [Ca2+]c elevation caused little alteration in the TMRE fluorescence of individual mitochondria compared with separate, time-matched control cells in which ICa was not activated (Fig. 5A). However occasionally (5 out of 92 mitochondria examined, n=10), 
m depolarization of individual mitochondria occurred (an example is shown in Fig. 5Ciii). These 
m depolarizations were not correlated with either the timing of ICa activation or the subsequent Ca2+ rise and, consequently, were not considered significant.
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m of individual mitochondria compared with controls (Fig. 5B). At 5 seconds after photolytic release of Ins(1,4,5)P3, a small but statistically insignificant (P=0.0518) decline in the TMRE fluorescence was observed (–0.0063±0.0022
F/F0 compared with –0.0009±0.0006
F/F0 in control, n=10). The significance level did not improve with the inclusion of additional experiments. As with ICa-evoked Ca2+ rises, on occasion in these experiments 
m depolarization of individual mitochondria occurred (7 out of 105 mitochondria in ten cells). These 
m depolarizations were neither correlated with Ins(1,4,5)P3 release nor [Ca2+]c increase. An example (Fig. 5Diii) shows the relative TMRE fluorescence of eight individual mitochondria from one cell in which Ins(1,4,5)P3 was released. In three mitochondria, 
m depolarized, two during Ins(1,4,5)P3-evoked Ca2+ release and one before the Ca2+ transient.

m measurement using quenching concentrations of TMRE
Hitherto in this investigation, TMRE was used at a concentration of 10 nM to prevent dye auto-quenching within the mitochondrial matrix and to enable visualization of the 
m of individual mitochondria. The low concentration might have limited our ability to resolve minor 
m changes across the cell. To examine this possibility, the 
m of the entire mitochondrial complement was studied by loading cells with a concentration of TMRE that exceeds its `quench limit' (150 nM) and monitoring fluorescence throughout the entire cell. At this higher concentration, 
m depolarization increases whole-cell TMRE fluorescence because of a reduction of fluorescence quenching as the dye re-equilibrates out of mitochondria (Duchen et al., 1998
; Ward et al., 2000
) (see Materials and Methods). In these conditions, no change in TMRE fluorescence was observed when [Ca2+]c was elevated either by Ins(1,4,5)P3 release (0.997±0.0014 F/F0, n=8, compared to untreated controls 0.997±0.002 F/F0, n=4, P>0.05, Fig. 6A), a single 500 ms plasmalemma depolarization to +10 mV (1.003±0.004 F/F0, n=6, P>0.05 compared to untreated controls, Fig. 6B), or a 5-second train of depolarizing pulses (–70 to +10 mV, 2 Hz, 1.001±0.002 F/F0, n=4, P>0.05 compared to untreated controls, Fig. 6C). Mitochondrial depolarization with CCCP (1 µM) plus oligomycin (6 µM), by contrast, caused a large increase in TMRE fluorescence (1.204±0.056 F/F0, n=3, P<0.01, Fig. 6D,E). These results again suggest that a transient increase in [Ca2+]c does not significantly depolarize 
m in colonic smooth muscle cells.
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m fluctuations in cells during repetitive [Ca2+]c oscillations
Very occasionally (<1%), cells exhibited spontaneous, repetitive [Ca2+]c oscillations of variable frequency and amplitude (Fig. 7). 
m depolarization, and often subsequent repolarization of individual mitochondria, was observed in these cells. The 
m depolarization apparently occurred regardless of the 
m of neighboring mitochondria. Fig. 7Aii and iv show enlarged regions of cells in which single mitochondria depolarized and repolarized independently of neighboring mitochondria, although the distance between the organelles could be as little as 5 µm. Regions in which fluorescence decreased from one frame to another are marked with a blue arrow; those in which fluorescence increased with a white arrow. This observation suggests that, rather than acting as an interconnected electrical network, these 
m depolarizations were independent of similar events in neighboring mitochondria. The 
m depolarizations also do not appear to be linked to the occurrence of individual [Ca2+]c oscillations (shown in Fig. 7Ai,iii). Fig. 7B shows examples of TMRE fluorescence from individual mitochondria alongside the corresponding [Ca2+]c changes. 
m depolarizations appeared to be equally as likely when [Ca2+]c was at resting or peak values, suggesting that these depolarizations did not occur as a direct consequence of the flux of positively charged Ca2+ ions into mitochondria.
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m depolarizations differed in each cell, as can be seen in Movies 1 and 2 in the supplementary material showing TMRE fluorescence during spontaneous [Ca2+]c oscillations. In Movie 1, the cell shows two mitochondria within the field of view that depolarized, one of which repolarized within the course of the experiment (10 minutes). Many more mitochondria appeared to depolarize and repolarize in the cell shown in Movie 2, with frequency increasing as the experiment progressed.
Cells displaying spontaneous Ca2+ oscillations were rare (<1%), precluding the study of the mechanisms underlying 
m depolarization. Interestingly, mimicking the spontaneous Ca2+ oscillations by repetitively applying either Ins(1,4,5)P3 (by photolysis) or CCh did not produce 
m depolarization (not shown, repeated application of Ins(1,4,5)P3 at a holding plasma membrane potential, Vm, of –70 mV: n=7; repeated application of Ins(1,4,5)P3 at a Vm of –20 mV: n=4; repeated application of CCh at a Vm of –70 mV: n=4; sequential application of Ins(1,4,5)P3, CCh and ICa activation by depolarization of Vm to +10 mV for 500 ms: n=3). However, flickering 
m depolarizations could be evoked by increasing either the intensity of excitation light or the concentration of TMRE used, or both. When used at a concentration of 150 nM, transient decreases in the TMRE fluorescence (
m depolarizations) of individual mitochondria were observed, without any changes in [Ca2+]c. (Although 
m depolarization increases whole-cell fluorescence when the concentration of TMRE is above the quench limit, individual mitochondria will still display a decrease in fluorescence intensity upon 
m depolarization because of dye re-equilibration, see Materials and Methods.) As the TMRE concentration was decreased from 150 nM to 10 nM, the number of 
m depolarizations decreased from 1.009±0.092 (150 nM TMRE) to 0.074±0.004 (10 nM TMRE) per mitochondrion per 10-minute imaging period (1 frame s–1, n=5, P<0.01, Fig. 8A). Thus, 0.74% of mitochondria displayed 
m depolarizations per minute when loaded with 10 nM TMRE, whereas some 10% depolarized per minute when loaded with 150 nM TMRE. The occurrence of 
m depolarizations also increased with increasing illumination light intensity when examined at lower TMRE concentrations (10 or 50 nM, Fig. 8A). These transient 
m depolarizations were attenuated by a mixture of antioxidants containing ascorbic acid (1 mM), catalase (250 units/ml), (R)-Trolox methyl ether (Trolox, 1 mM) and 2,2,6,6-tetramethylpiperidin-1-yloxy (TEMPO, 500 µM). In these experiments 
m depolarizations decreased from 1.061±0.091 (control) to 0.280±0.035 in the presence of antioxidants (depolarizations per mitochondrion per 10-minute imaging period, n=5, P<0.01, Fig. 8B). The mPTP inhibitor CsA (2 µM) also decreased 
m depolarization frequency from 1.061±0.091 to 0.427±0.028 (n=4, P<0.01, Fig. 8B). These 
m depolarizations might arise from an oxidant-mediated transient opening of the mPTP (Huser et al., 1998
; Jacobson and Duchen, 2002
).
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| Discussion |
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300 nM (Bezprozvanny et al., 1991
Mitochondrial Ca2+ uptake should depolarize 
m to restrict the ability of mitochondria to produce ATP. Ca2+ signaling could, in theory at least, limit the primary mechanism for ATP production. It is therefore important to resolve whether or not 
m depolarization occurs following increases in [Ca2+]c. The present study found no detectable alterations in 
m during large, transient [Ca2+]c rises evoked by Ca2+ influx across the plasmalemma in single colonic myocytes (Figs 5 and 6). The limit of resolution in the present study was
5 mV. Therefore, 
m depolarization during Ca2+ uptake was smaller than this value.
Isolated mitochondria exposed to bolus additions of Ca2+ undergo transient 
m depolarizations (Brustovetsky and Dubinsky, 2000
; Huser et al., 1998
). However, whether or not the local [Ca2+]c experienced by mitochondria in situ, in intact cells, is sufficient to cause 
m depolarizations comparable to those that occur in isolated mitochondria is unresolved. 
m depolarization has been observed in response to the [Ca2+]c rise produced by trains of plasmalemmal depolarization in single toad gastric myocytes (Drummond et al., 2000
). No alterations in 
m were observed in the present study to trains of depolarization (Fig. 6C). Mitochondria might be arranged differently in the two cell types and positioned further from voltage-gated Ca2+ channels in colonic myocytes than in gastric myocytes, and hence exposed to lower local [Ca2+]c. Alternatively, the inclusion of mitochondrial substrates (pyruvate and malate) in the pipette filling solution in the present study, which are required to maintain the driving force for 
m production, might have contributed to the differences in the two studies. Indeed, partial metabolic limitation of the electron-transport chain resulted in a greater 
m depolarization during Ca2+ entry evoked by tetanic stimuli in motor neuron terminals (Talbot et al., 2007
).
The present study also found no significant alteration in 
m during [Ca2+]c transients evoked by Ca2+ release from internal stores via Ins(1,4,5)P3Rs (Figs 5 and 6). Other studies have, like ours, failed to measure any significant 
m depolarization in response to transient [Ca2+]c increases produced by Ins(1,4,5)P3-generating agonists, e.g. in HeLa or RBL-2H3 cells (Collins et al., 2001
; Csordas and Hajnoczky, 2003
). Although Ca2+ uptake by mitochondria must lead to 
m depolarization, its magnitude is small and unresolved because either the input resistance of the inner mitochondrial membrane was too low for a significant 
m to occur with the current carried by Ca2+ or because a compensatory efflux of positively charged species (i.e. protons) offsets the depolarization evoked by Ca2+ influx.
Mitochondrial ion fluxes and energy metabolism have recently been modeled in electrically paced cardiac myocytes (Nguyen et al., 2007
). This model shows that a rapid rise in mitochondrial [Ca2+], during cytosolic [Ca2+] transients, is accompanied by increases in mitochondrial [ATP], [NAD+], [Pi] and [Na+] and decreases in mitochondrial [ADP], [NADH] and 
m. The magnitude of the drop in 
m is
8 mV with a time constant of recovery of <0.1 seconds (Nguyen et al., 2007
). A transient 
m depolarization of
8 mV is around the limit of resolution in the present study and is unlikely to be detected. Mitochondrial energy metabolism was also modeled in hypothetical microdomains of high [Ca2+]c (up to
20 µM) in cardiac dyadic space. Here, 
m was predicted to transiently depolarize to
0 mV due to mitochondrial Ca2+ uptake. Recovery was complete within 0.3 seconds (Nguyen et al., 2007
). It is unlikely, therefore, in the current study, that [Ca2+]c in microdomains near mitochondria reached these concentrations (20 µM), or 
m depolarization would have been observed.
Very occasionally, spontaneous [Ca2+]c oscillations were observed in colonic myocytes. Because these spontaneous Ca2+ oscillations were rare (occurring in only 3 out of 314 cells), they would appear to be an unusual form of Ca2+ signaling in this cell type. In cells showing spontaneous Ca2+ oscillations, depolarization of the 
m of individual mitochondria occurred (Fig. 7). The 
m depolarizations were randomly distributed throughout the cell, did not affect the 
m of neighboring mitochondria and appeared independent of the timing of individual [Ca2+]c oscillations.
Random depolarization of 
m was also observed with increasing intensity of excitation light or increased TMRE concentration (see also Collins et al., 2002
; Duchen et al., 1998
; Huser and Blatter, 1999
; Huser et al., 1998
; Jacobson and Duchen, 2002
) (Fig. 8). The 
m depolarizations were decreased in frequency by antioxidants (Jacobson and Duchen, 2002
). Hence, these 
m depolarizations seem likely to have arisen from light- or dye-induced oxidant production. Oxidants activate the mPTP, which might depolarize 
m (Duchen, 2000
). Indeed, 
m depolarization was blocked by the mPTP inhibitor CsA in the present study (Fig. 8B).
No significant transient 
m depolarizations were observed during or after either ICa- or Ins(1,4,5)P3-evoked increases in [Ca2+]c because, in these experiments, the TMRE concentration used was low (10 nM), excitation light was attenuated with a neutral density filter and the duration of the imaging period was limited to 30 seconds. Each of these measures should limit oxidant production. The 
m depolarizations that did occur during spontaneous [Ca2+]c oscillations were not linked temporally to the [Ca2+]c changes. It might be that these 
m depolarizations arise from a gradual accumulation of [Ca2+]m, perhaps resulting in activation of the mPTP directly by Ca2+ or indirectly via a Ca2+-dependant increase in oxidant production (Brookes et al., 2004
). The rare appearance of spontaneous Ca2+ oscillations precluded further examination of these possibilities.
The localized, individual nature of 
m depolarizations that occurred in cells with Ca2+ oscillations, or during light- and dye-induced 
m depolarizations, suggests that mitochondria do not form an interconnected electrical network in smooth muscle. Had mitochondria done so, depolarization of 
m at one site should have depolarized 
m at distant sites. Mitochondria might exist as an interconnected network in some (Diaz et al., 2000
; Rizzuto et al., 1998
; Szado et al., 2003
) but not in other (Buckman and Reynolds, 2001
; Collins et al., 2001
; Jacobson and Duchen, 2002
; Montero et al., 2002
; O'Reilly et al., 2004
) cell types. In the present study, mitochondria appear to be individual units of approximately 1-5 µm in length. Mitochondrial modulation of Ca2+ signaling might primarily be a localized, subcellular effect.
The present findings demonstrate that mitochondria contribute to the decline in [Ca2+]c after ICa activation and promote Ca2+ release via Ins(1,4,5)P3Rs on the SR. During these [Ca2+]c increases, 
m – the driving force for ATP production – was not significantly altered; hence, one mitochondrial function – that of ATP production – is not negatively affected by another, i.e. Ca2+ uptake and modulation of [Ca2+]c. Some alteration in 
m could occur with prolonged repetitive Ca2+ signaling, presumably as a consequence of a gradual, cumulative mitochondrial Ca2+ overloading or oxidant production. Mitochondrial Ca2+ uptake provides a fine-tuning of Ca2+ signaling. For example, a slight alteration of Ins(1,4,5)P3R activity by mitochondrial Ca2+ accumulation could modulate the threshold for global [Ca2+]c wave initiation. Mitochondria accomplish this activity without compromising their ability to produce ATP.
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500 g) as described previously (McCarron and Muir, 1999
Electrophysiology
Membrane currents were measured using conventional tight-seal whole-cell recording. The extracellular solution contained (mM): Na glutamate 80, NaCl 40, tetraethylammonium chloride (TEA) 20, MgCl2 1.1, CaCl2 3, HEPES 10, glucose 30 (pH 7.4 with NaOH) plus TMRE (10 nM) unless otherwise indicated. The pipette solution contained (mM): Cs2SO4 85, CsCl 20, MgCl2 1, HEPES 30, MgATP 3, sodium pyruvate 2.5, malic acid 2.5, NaH2PO4 1, creatine phosphate 5 and NaGTP 0.5, with caged inositol trisphosphate [Ins(1,4,5)P3] trisodium salt 0.025 added for experiments involving photolytic release of Ins(1,4,5)P3. The high concentration of HEPES was to ensure adequate control of pH during 
m depolarization; sodium pyruvate and malic acid to maintain mitochondrial activity; and phosphocreatine and ATP to maintain [ATP] during the experiments. Whole-cell currents were measured using an Axopatch 200B (Molecular Devices, Sunnyvale, CA, USA), low-pass filtered at 500 Hz (8-pole bessel filter; Frequency Devices, Haverhill, MA, USA), digitally sampled at 1.5 kHz using a digidata interface and pClamp (version 8; Molecular Devices), and stored for analysis.
Imaging
Cells were co-loaded with the Ca2+-sensitive dye Fluo-4 AM (10 µM) and the 
m-sensitive dye TMRE (10 nM unless stated otherwise) for 30 minutes in the presence of wortmannin (10 µM; to prevent contraction). Qualitatively identical results were obtained in the absence of wortmannin. TMRE is a lipophilic, cationic fluorescent dye that accumulates within mitochondria according to their 
m in a Nernstian fashion (Duchen et al., 1998
; Scaduto and Grotyohann, 1999
). 
m depolarization causes a decrease in mitochondrial [TMRE] regardless of the concentration of the indicator used; however, TMRE fluorescence of the whole cell may increase or decrease on 
m depolarization, depending on the concentration of TMRE used (Ward et al., 2000
). This is because, above a certain concentration (e.g.
100 nM in the cells used in this study), TMRE self-quenches within mitochondria to reduce the fluorescence emanating from the indicator. In these circumstances, 
m depolarization will decrease the mitochondrial [TMRE] to decrease or cause no change in the fluorescence of individual mitochondria, but whole-cell TMRE fluorescence will transiently increase. Dye that was previously quenched (non-fluorescent) within mitochondria moves to the cytosol to increase fluorescence there before re-equilibrating across the plasmalemma (Ward et al., 2000
). In this `quenched' mode, TMRE cannot be used quantitatively to monitor 
m of individual mitochondria. At a concentration below
100 nM, TMRE fluorescence does not self-quench within mitochondria and decreases with 
m depolarization. The 
m of individual mitochondria can be resolved with TMRE concentrations below the quench limit (e.g. 10 nM). In this study, a sub-quenching concentration of TMRE (10 nM) was used to monitor the 
m of individual mitochondria and a quenching concentration of TMRE (150 nM) to monitor the 
m of the entire mitochondrial complement of the cell.
Two-dimensional images of [Ca2+]c and 
m were obtained using a wide-field digital imaging system. Single cells were excited at 475 nm and 560 nm (Polychrome IV monochromator, TILL Photonics, Martinsried, Germany), and light was passed via a fiber-optic guide through a dual 483/553 nm bandpass filter (bandpass 15 and 20 nm, respectively), a field stop diaphragm, through an ND4 neutral density filter (unless otherwise stated) and reflected off a custom-made dual long-pass dichroic mirror (transmissive in the ranges 505-540 nm and 577-640 nm, and reflective from 490 to below 300 nm; Chroma, Rockingham, VT, USA) and then through an oil immersion objective (x40 UV 1.3 NA; Nikon UK, Surrey, UK). Emitted light was guided through a dual bandpass 518/594 nm barrier filter (bandpass 25 and 18 nm, respectively) to an intensified, cooled, frame transfer CCD camera (Pentamax Gen IV; Roper Scientific, Trenton, NJ, USA) controlled by MetaFluor software (Universal Imaging, Downingtown, PA, USA). Full-frame images (150x150 pixels), with a pixel size of 563 nm at the cell, were acquired sequentially with an exposure period of 100 ms for Fluo-4 and then 50 ms for TMRE (resultant acquisition rate for the pair was 5 Hz). In some experiments, TMRE fluorescence alone was recorded at a frequency of 100 Hz (10 ms exposure) with the camera under the control of WinView32 operating in high-speed mode. No difference in the frequency of 
m depolarizations was noted between 5 and 100 Hz sampling frequency.
Localized flash photolysis
The output of a xenon flashlamp (Rapp Optoelecktronic, Hamburg, Germany), used to uncage Ins(1,4,5)P3, was passed through a UG-5 filter to select UV light, focused and merged into the excitation light path via a fiber-optic bundle and long pass dichroic mirror at the lens part of the epi-illumination attachment of the microscope. The diameter of the fiber optic together with the lens magnification determined the area (spot size
10 µm diameter) of Ins(1,4,5)P3 photolysis.
Data analysis
Images were analyzed using MetaMorph 6.2 (Universal Imaging). [Ca2+]c measurements were made from the Fluo-4 fluorescence changes in the entire cell. Fluorescence signals were expressed as ratios (F/F0) or change of ratios (
F/F0) of fluorescence counts (F) relative to baseline values before stimulation (F0). Peak Fluo-4 F/F0 and the time required for Fluo-4 F/F0 to decline to 50% of the peak value were calculated before and after treatment with either CCCP (1 µM) plus oligomycin (6 µM) or rotenone (5 µM) plus oligomycin (6 µM). CCCP dissipates transmembrane proton gradients, oligomycin prevents ATP consumption by inhibiting the mitochondrial ATP synthase and rotenone is a complex I inhibitor that will also depolarize 
m. The use of CCCP and rotenone with oligomycin will depolarize mitochondria without ATP depletion (Budd and Nicholls, 1996
); 0.2% dimethyl sulfoxide (DMSO) served as the vehicle control. TMRE fluorescence was measured over regions of interest drawn around individual mitochondria or the whole cell as described in the text. Each of these fluorescence signals from mitochondria and whole cells were normalized to starting baseline values (taken as 1) and the gradual decline in the signals due to dye photobleaching was corrected for by subtracting a linear extrapolation of bleaching from each region (thus making the baseline fluorescence values 0). To create summarized results and allow statistical analysis, a rolling `box-car' average (5 seconds) of corrected TMRE
F/F0 was created and sampled every 2.5 seconds for most experiments (30-second data-collection period). With longer data-collection periods during the examination of oxidant-induced 
m depolarization (60-600 seconds), the rolling average was increased to a 20-second window, sampled every 10 seconds. Results are express