Abstract
Duchenne muscular dystrophy represents a severe inherited disease of striated muscle. It is caused by a mutation of the dystrophin gene and characterized by a progressive loss of skeletal muscle function. Most patients also develop a dystrophic cardiomyopathy, resulting in dilated hypertrophy and heart failure, but the cellular mechanisms leading to the deterioration of cardiac function remain elusive. In the present study, we tested whether defective excitation-contraction (E-C) coupling contributes to impaired cardiac performance. “E-C coupling gain” was determined in cardiomyocytes from control and dystrophin-deficient mdx mice. To this end, L-type Ca2+ currents (ICaL) were measured with the whole cell patch-clamp technique, whereas Ca2+ transients were simultaneously recorded with confocal imaging of fluo-3. Initial findings indicated subtle changes of E-C coupling in mdx cells despite matched Ca2+ loading of the sarcoplasmic reticulum (SR). However, lowering the extracellular Ca2+ concentration, a maneuver used to unmask latent E-C coupling problems, was surprisingly much better tolerated by mdx myocytes, suggesting a hypersensitive E-C coupling mechanism. Challenging the SR Ca2+ release by slow elevations of the intracellular Ca2+ concentration resulted in Ca2+ oscillations after a much shorter delay in mdx cells. This is consistent with an enhanced Ca2+ sensitivity of the SR Ca2+-release channels [ryanodine receptors (RyRs)]. The hypersensitivity could be normalized by the introduction of reducing agents, indicating that the elevated cellular ROS generation in dystrophy underlies the abnormal RyR sensitivity and hypersensitive E-C coupling. Our data suggest that in dystrophin-deficient cardiomyocytes, E-C coupling is altered due to potentially arrhythmogenic changes in the Ca2+ sensitivity of redox-modified RyRs.
Keywords: ryanodine receptor, calcium signaling, muscular dystrophy
duchenne muscular dystrophy (DMD) belongs to the large group of dystrophinopathies, in which cytoskeletal abnormalities and remodeling may lead to heart failure (18, 36). DMD represents the most severe genetic muscular disorder affecting striated muscle. It results from mutations in the dystrophin gene, which encodes for the cytoskeletal protein dystrophin (8). At the cellular level, dystrophin forms a molecular bridge between the F-actin of the cytoskeleton and the extracellular matrix via the dystroglycan protein complex, thus providing mechanical stability to the myocyte. Lack of dystrophin expression disrupts the dystroglycan complex and is thought to confer instability to the cytoskeleton and plasma membrane with a severe impact on cellular signaling. The disease affects 1 in 3,000 boys with the onset of complications in early childhood. Disease symptoms ultimately lead to premature death, mostly due to respiratory failure. Progressive skeletal muscle wasting in DMD is also accompanied by the development of cardiac abnormalities, such as fibrosis with wall motion malfunctions, left ventricular dysfunction, and ventricular arrhythmias, leading to dilated cardiomyopathy and cardiac failure (11). Since therapy progress at the level of skeletal muscle wasting has significantly improved the life expectancy of DMD patients over the years, dystrophic cardiomyopathy becomes more and more a limiting factor in the (symptomatic) treatment of DMD patients.
An established animal model for studying the disease phenotype of DMD is the mdx mouse, where, in analogy to DMD mutations, a point mutation in the dystrophin gene leads to an untranslatable gene (16, 21). Similar to humans, mdx mice show an age-linked disease onset of cardiomyopathy resulting in cardiac dilation, a progressive decrease in fractional shortening, replacement of the functional myocardium by fibrotic tissue, and, thus, conduction defects (5, 31).
A previous study (41) of the mdx mouse showed substantial changes in Ca2+ signaling with only slightly elevated levels of resting intracellular Ca2+ concentration ([Ca2+]i) in ventricular myocytes. In addition, dystrophic myocytes exhibit an increased susceptibility to mechanical stress-induced Ca2+ influx across the sarcolemma, possibly via microruptures, stretch-activated channels, and other pathways as a consequence of the disrupted dystroglycan complex (9, 20, 41, 45). This allows for excessive Ca2+ influx via voltage-independent pathways during mechanical stress, which is then synergistically amplified by several cellular mechanisms to generate excessive cytosolic and mitochondrial Ca2+ transients and irreversible loss of mitochondrial membrane potential, an early indication of cell death (20). Excessive production of ROS in these cells was identified as a mechanism contributing to this disproportionate Ca2+ signal amplification (20, 42). Since ryanodine receptors (RyRs) become more Ca2+ sensitive after oxidation (30), the simultaneous activation of Ca2+-induced Ca2+ release (CICR) and ROS production in dystrophic myocytes could be the mechanism leading to cellular damage. Functional incapability of precise intracellular Ca2+ regulation might be an early indicator of changes in Ca2+ sensitivity and may have a large impact on excitation-contraction (E-C) coupling and cell survival in the long run.
The goal of the present study was to investigate impairments of E-C coupling in dystrophic cardiomyopathy. In progressive cardiomyopathies, disturbance of the E-C coupling mechanism often contributes to decreased cardiac performance. For example, in several animal models for heart failure, it has been shown that at similar L-type Ca2+ current (ICaL) amplitude, there is a significant reduction in CICR, resulting in smaller Ca2+ transients and decreased myocyte contractility (14, 26, 35). A reduction in the ability of the Ca2+ current to trigger Ca2+ release from the sarcoplasmic reticulum (SR) can indicate a reduced sensitivity of the E-C coupling machinery toward Ca2+. Therefore, we expected alterations of E-C coupling in dystrophy to be similar to those observed in other forms of cardiomyopathy, with a reduced reliability of signal transmission between L-type Ca2+ channels and RyRs. Opposite to these expectations, our data indicated an abnormal ability of dystrophic myocytes to cope with experimental tests designed to challenge E-C coupling mechanisms, which points to a hypersensitivity of E-C coupling rather than to the reduced efficiency of E-C coupling found in other cardiac pathologies. Our results suggest that the hypersensitive E-C coupling results, at least in part, from an increased probability of RyRs to be activated by Ca2+, which may be the consequence of an imbalance in redox regulation in dystrophic myocytes. While such hypersensitivity may initially represent a beneficial mechanism to maintain E-C coupling in the disease, it may also have negative consequences, for example, by increasing the propensity for arrhythmias.
Some preliminary data of this study have been presented in abstract form (39).
MATERIALS AND METHODS
Cell isolation.
Adult C57BL10 mice [wild-type (WT) mice] at the age of 6–12 mo and age-matched dystrophin-deficient mdx mice (C57BL/10ScSn-mdx mice) were used in this study. At this age, mdx mice begin to develop a dilated cardiomyopathy but are not in overt heart failure (31). Animals were provided by Dr. M. Rüegg (University of Basel, Basel, Switzerland) and Dr. U. Rüegg (University of Geneva, Geneva, Switzerland) or were purchased from the Jackson Laboratory. Mouse hearts were rapidly excised after cervical dislocation, immersed in cold Ca2+-free saline buffer, and trimmed of excess tissue. Hearts were then cannulated and placed on a Langendorff perfusion apparatus. Enzymatic dissociation of ventricular myocytes was performed as previously described (43). Isolated cells were kept at room temperature until further use. All experiments conformed with the National Institutes of Health Guide for the Care and Use of Laboratory Animals (1996) and were approved by the Institutional Animal Care and Use Committee of the New Jersey Medical School of the University of Medicine and Dentistry of New Jersey and by the State Veterinary Office of Bern, Switzerland.
Electrophysiological experiments.
Membrane currents were measured using whole cell patch-clamp procedures with an Axopatch 200B amplifier (Axon Instruments) controlled by custom-written data-acquisition software developed under LabView (National Instruments). Cells were voltage clamped using low-resistance (1.5–3 MΩ) borosilicate glass micropipettes. The pipette solution contained (in mM) 120 CsAsp, 8 NaCl, 20 tetraethylammonium(TEA)-Cl, 5 MgCl2, 4 KATP, 5 HEPES, and 0.1 K5-fluo-3 at pH 7.2 adjusted with CsOH. For experiments with reduced SR Ca2+ load, Na+ was omitted [to continuously favor Ca2+ extrusion via the Na+/Ca2+ exchanger (NCX)]. The external control solution contained (in mM) 140 NaCl, 5.4 KCl, 5 CsCl, 1.2 CaCl2, 1.1 MgCl2, 5 HEPES, and 10 glucose at pH 7.4 adjusted with NaOH. In some experiments, the external solution contained 1.8, 0.5, or 0.25 CaCl2 instead of 1.2 mM CaCl2.
Starting from a holding potential of −80 mV, the voltage protocol consisted of an initial step to −40 mV for 2 s. When corrected for the tip potential, this would correspond to a real potential of −52 mV, which inactivates voltage-dependent Na+ and T-type Ca2+ currents. This inactivation step was followed by 8 pulses of 50 ms to 0 mV at 1 Hz and then by a 400-ms depolarization to various test voltages. The initial preconditioning pulses were always applied in control solution and served to equalize the SR Ca2+ load before each test step, which was recorded at different extracellular Ca2+ concentrations ([Ca2+]o). Subsequent to the loading pulses, the membrane voltage was kept at −40 mV for 4 s to allow for the complete exchange of extracellular solution by rapid local perfusion (half-life < 0.5 s). The full voltage protocol is shown in Fig. 1A.
Fig. 1.

L-type Ca2+ currents (ICaL), Ca2+ transients, and excitation-contraction (E-C) coupling gain under control conditions [1.2 mM extracellular Ca2+ concentration ([Ca2+]o)]. A: voltage protocol used for the experiments. The eight prepulses were always applied in control solution, whereas for the test step [Ca2+]o was briefly varied according to the experimental challenge. B and C: representative traces for Ca2+ currents (bottom), line-scan images of Ca2+-related changes in fluorescence (ΔF/F0; middle), and normalized cytosolic Ca2+ transients (top) elicited by a 400-ms test pulse to 0 mV in control solution in a wild-type (WT) cell (B) and a mdx cell (C). D: voltage dependence of current activation [current-voltage (I–V) curve, bottom traces] and corresponding Ca2+ transients (Ca2+-V curve, top traces) in WT (black; n = 8–21 cells) and mdx (red; n = 15–30 cells) myocytes. E: E-C coupling gain calculated from the data shown in D in WT (black) and mdx (red) myocytes at different test voltages.
Confocal microscopy.
Changes in [Ca2+]i were simultaneously measured with ionic currents using the fluorescent Ca2+ indicator K5-fluo-3 (100 μM, Biotium) and a laser-scanning confocal microscope (MicroRadiance, Bio-Rad). Fluo-3 was excited with the 488-nm line of an argon ion laser. The emitted light was collected above 500 nm. The acquisition of line-scan images along the cardiomyocytes was triggered by the LabView software 400 ms before the last loading pulse. Line-scan images were recorded for 6 s at a rate of 500 lines/s and captured the last prepulse, the period for solution exchange, and the test step at the end of the voltage protocol.
In experiments with intact ventricular cardiomyocytes (i.e., not dialyzed with a pipette filling solution), intracellular Ca2+ signals were recorded by full-frame image acquisition. Cells were loaded with fluo-3 by exposure to the membrane-permeant ester fluo-3 AM (5 μM, Biotium) for 30 min at room temperature followed by at least 10 min of deesterification. Images were acquired using a laser-scanning confocal microscope (MRC 1000, Bio-Rad). Fluo-3 was excited at 488 nm with a solid-state laser (Sapphire, Coherent), and fluorescence detection was performed at 540 ± 15 nm. Cells were continuously superfused with extracellular solution containing (in mM) 140 NaCl, 5.4 KCl, 1.8 CaCl2, 1.1 MgCl2, 5 HEPES, and 10 glucose at pH 7.4. Different test solutions contained 70 mM NaCl and 70 mM LiCl, or 140 mM LiCl instead of 140 mM NaCl. The osmolality was 310 mosM for all solutions.
Thapsigargin and ryanodine were from Alamone Laboratories, Mn-cpx3 was from Calbiochem, and mercaptopropionyl-glycine (MPG) was from Sigma-Aldrich. All experiments were performed at room temperature (22°C).
Data analysis.
Electrophysiological data were analyzed using IgorPro software (Wavemetrics). Current inactivation was fitted with a double-exponential function. Confocal images were initially analyzed using Image SXM [free software based on NIH Image (3)] and further processed by IgorPro. Fluorescence changes (ΔF/F0) during Ca2+ transients in line-scan images were fitted with a sigmoidal function to determine peak amplitude and rise time.
Significance was tested by Student's t-test. Values of P < 0.05 were considered significant. Pooled data are given as means ± SE, with n representing the number of cells tested. In the figures and table, significance is indicated by *P < 0.05 and **P < 0.01.
RESULTS
ICaL, cytosolic Ca2+ transients, and E-C coupling gain in WT and dystrophic cardiomyocytes.
During cardiac E-C coupling, depolarization-induced Ca2+ influx through L-type Ca2+ channels triggers Ca2+ release from the SR via CICR, which subsequently initiates the contraction of cardiac muscle cells.
Figure 1 shows the voltage protocol (A), representative traces of ICaL, and corresponding cytosolic Ca2+ signals at peak activation [maximal current amplitude at 0 mV (Imax)] in WT (B) and mdx (C) myocytes. At similar trigger Imax, SR Ca2+ release reached comparable amplitudes in both WT (n = 20) and mdx myocytes (n = 16; see also Table 1). The voltage of test steps ranged from −25 to +50 mV. The current-voltage relationship and the associated voltage dependence of cytosolic Ca2+ transients under control conditions are shown in Fig. 1D.
Table 1.
Comparison of ICaL and corresponding intracellular Ca2+ transients and E-C coupling gain in WT and mdx cardiomyocytes at different [Ca2+]o and membrane voltages
| WT Cardiomyocytes |
mdx Cardiomyocytes |
|||||||
|---|---|---|---|---|---|---|---|---|
| ICaL, pA/pF | ΔF/F0 | Gain, (ΔF/F0)/ICaL | n | ICaL, pA/pF | ΔF/F0 | Gain, (ΔF/F0)/ICaL | n | |
| 1.2 mM [Ca2+]o | ||||||||
| 0-mV test voltage | −5.36±0.09 | 3.36±0.24 | 0.69±0.07 | 20 | −5.81±0.37 | 3.83±0.21 | 0.67±0.04 | 16 |
| −25-mV test voltage | −0.40±0.06† | 0.98±0.12 | 3.58±0.39 | 21 | −0.83±0.12† | 1.39±0.17 | 2.66±0.38 | 28 |
| 0.5 mM [Ca2+]o | ||||||||
| 0-mV test voltage | −2.97±0.30 | 2.61±0.54 | 0.91±0.20 | 12 | −3.12±0.39 | 3.65±0.32 | 1.04±0.08 | 23 |
| −25-mV test voltage | −0.39±0.07 | 0.46±0.13 | 1.98±0.34 | 15 | −0.53±0.09 | 0.79±0.12 | 3.04±0.63 | 25 |
| 0.25 mM [Ca2+]o | ||||||||
| 0-mV test voltage | −1.94±0.37 | 1.20±0.59* | 0.48±0.18* | 5 | −2.93±0.49 | 2.90±0.37* | 1.04±0.11* | 6 |
| −25-mV test voltage | −0.37±0.07 | 0.27±0.06† | 1.20±0.33* | 7 | −0.47±0.15 | 0.83±0.11† | 3.20±0.60* | 9 |
Values are means ± SE; n, no. of cells. ICaL, maximum current; ΔF/F0, Ca2+ transients; [Ca2+]o, extracellular Ca2+ concentration. Significant differences between datasets of wild-type (WT) and mdx cardiomyocytes are indicated as
P < 0.05 and
P < 0.01. See the text for statistics for other comparisons.
Analysis of the E-C coupling gain provides an estimate of the coupling fidelity between L-type Ca2+ channels and RyRs. It is determined by normalizing the amplitude of the cytosolic Ca2+ transient to the corresponding amplitude of ICaL at each given voltage. When performing this E-C coupling analysis, gain was comparable in dystrophic and WT myocytes, particularly at positive test voltages, as expected from the similarity in Ca2+ current amplitudes and Ca2+ transients (Fig. 1E). At negative membrane voltages, the E-C coupling gain was always largest, possibly due to higher coupling fidelity between the L-type Ca2+ channel and RyR and less redundant Ca2+ current (1). However, under control conditions, the gain was only insignificantly reduced in mdx cells at −25 mV (3.58 ± 0.39, n = 21, and 2.66 ± 0.38, n = 28, at −25 mV in WT and mdx cells, respectively).
Thus, in contrast to observations in several other cardiac pathologies, such as hypertrophy and heart failure (4, 14, 28), the efficiency of E-C coupling in dystrophic myocytes did not seem to be affected under control conditions.
ICaL, cytosolic Ca2+ transients, and E-C coupling gain at threshold conditions.
At physiological [Ca2+]o, the E-C coupling machinery is optimized to produce reliable E-C coupling in cardiomyocytes and may therefore be able to compensate for subtle problems resulting from a disease. To detect changes in the functionality of the involved key proteins, the system may be tested under conditions that challenge the efficiency of the E-C coupling mechanism. Lowering the [Ca2+]o has previously been successfully used as an experimental tool to unmask subtle impairments of E-C coupling in a diseased heart (28). Therefore, we repeated the experiments shown in Fig. 1 at lower [Ca2+]o, and the data are shown in Fig. 2.
Fig. 2.

ICaL, Ca2+ transients, and E-C coupling gain challenged by low (0.5 mM) [Ca2+]o. Please note that the prepulses to load the sarcoplasmic reticulum (SR) were done in control solution (1.2 mM [Ca2+]o). A: voltage dependence of current (top lines) and corresponding Ca2+ transients (bottom lines) in WT (black) and mdx (red) cells. B: voltage dependence of the E-C coupling gain from the data shown in A in WT (black; n = 4–17 cells) and mdx (red; n = 9–25 cells) myocytes. C: statistical comparison of the E-C coupling gain in 1.2 and 0.5 mM Ca2+ in WT (black; n = 15 cells) and mdx (red; n = 25 cells) cells.
First, ICaL and intracellular Ca2+ transients were simultaneously measured during test steps at 0.5 mM [Ca2+]o. Please note that the SR Ca2+-loading procedure (as in Fig. 1A) was performed before each test pulse by applying the prepulses in control solution containing 1.2 mM [Ca2+]o to assure a SR Ca2+ load equal to that under control conditions.
As expected upon reduction of [Ca2+]o, Ca2+ current was reduced in both WT and dystrophic myocytes. The Ca2+ transients were also smaller. However, contrary to our expectations, mdx myocytes were much less sensitive to reductions of [Ca2+]o than WT cells. The E-C coupling gain was calculated for each current-transient pair, and the averages are shown in Fig. 2B as a function of the test voltage. The phenomenon was most pronounced at negative test potentials but was consistently seen at all voltages tested. Whereas in WT cells the E-C coupling gain at −25 mV decreased by 45% in low [Ca2+]o (to 1.98 ± 0.34, n = 15), it increased by 14% in mdx cells (to 3.04 ± 0.63, n = 25; Fig. 2, B and C and Table 1). In other words, in mdx cardiomyocytes, the SR Ca2+ release was less impaired by reductions of [Ca2+]o, and thus the trigger signal for CICR, than in WT cells. Averaged amplitudes of ICaL and Ca2+ transients at two different test voltages (0 and −25 mV) are shown in Table 1. Current-voltage relationship and the associated voltage dependence of cytosolic Ca2+ transients are shown in Fig. 2A.
Because of this surprising finding, we challenged the E-C coupling mechanism even more by further lowering [Ca2+]o to near critical levels for functional coupling (to 0.25 mM). Figure 3 shows representative Ca2+ current traces, line scans of Ca2+-dependent changes in fluorescence, and line profiles of cytosolic Ca2+ transients at test voltages of 0 mV (A and B) and −25 mV (C and D) for WT and mdx myocytes. Table 1 shows averaged amplitudes of ICaL and Ca2+ transients obtained in this group of experiments. At both test potentials, the amplitude of the Ca2+ transient was significantly larger in mdx cells than in WT cells in 0.25 mM [Ca2+]o at similar trigger ICaL.
Fig. 3.

ICaL, Ca2+ transients, and E-C coupling gain in 0.25 mM [Ca2+]o elicited with the same voltage protocol as shown in Fig. 1. A–D: representative traces of Ca2+ currents (bottom), line-scan images (middle), and normalized cytosolic Ca2+ transients (top) elicited by test pulses to 0 mV (A and B) and −25 mV (C and D) in WT (A and C) and mdx (B and D) myocytes. Insets in C and D show enlarged Ca2+ signals at −25 mV. E: statistical comparison of the E-C coupling gain in 1.2 mM (from Fig. 2) and 0.25 mM Ca2+ at −25 mV for WT (black; n = 7 cells) and mdx (red; n = 9 cells) cells. *P < 0.05.
The differences in CICR between WT and mdx cells are emphasized when the values at 0.25 mM [Ca2+]o are compared with the corresponding controls at 1.2 mM [Ca2+]o. Figure 3E shows the E-C coupling gain in WT and mdx myocytes at −25 mV in 0.25 mM [Ca2+]o. Whereas in WT cells the gain decreased by 66% (n = 7) in 0.25 mM [Ca2+]o, it increased by 20% (n = 9) in mdx myocytes compared with control [Ca2+]o.
Thus, in contrast to WT cells, lowering of [Ca2+]o unmasked an unusual resistance to reductions in triggering ICaL in mdx myocytes and resulted in an abnormal increase in the E-C coupling gain. Again, this reflects a behavior that is opposite to the results from previous studies of altered E-C coupling in cardiac diseases, such as heart failure (4, 14, 28). This observation could, for example, be explained by a hypersensitivity of E-C coupling and RyRs toward Ca2+ triggers in mdx cardiomyocytes.
Initial support for this possibility comes from the analysis of the dependence of half-maximal SR Ca2+ release on [Ca2+]o. We determined Ca2+ transient amplitudes during test steps to −25 mV in 1.8, 1.2, 0.5, and 0.25 mM [Ca2+]o. The half-maximal Ca2+ release was observed at 0.69 mM [Ca2+]o in WT, whereas it was shifted to lower Ca2+ concentrations (to 0.41 mM) in mdx myocytes.
RyR Ca2+ sensitivity.
To investigate whether mdx myocytes indeed exhibit higher sensitivity toward changes in [Ca2+]i, we provoked moderate and slow Ca2+ influx into cardiomyocytes via the activation of NCX in its Ca2+ influx (reverse) mode. Lowering the Na+ concentration in the extracellular medium by substitution with Li+ forced the NCX into the Ca2+ influx mode. Figure 4, A and B, shows representative intracellular Ca2+ signals in WT and mdx cells in response to a stepwise reduction of external Na+ to 70 or 0 mM. Ca2+ influx via NCX triggered substantial and reversible Ca2+ oscillations (Fig. 4, A and B). Whereas at 70 mM extracellular Na+ the frequency of oscillations was still comparable in the two types of myocytes (0.27 ± 0.05 Hz, n = 19, and 0.29 ± 0.02 Hz, n = 9, in WT and mdx cells, respectively), it was significantly higher upon complete removal of Na+ in mdx myocytes (0.39 ± 0.04 Hz, n = 19, and 0.68 ± 0.08 Hz, n = 8; Fig. 4C). Equally important, Ca2+ oscillations at reduced Na+ occurred significantly earlier in mdx cells (after 23.1 ± 4.1 vs. 8.87 ± 1.69 s in 70 mM Na+ and 13.0 ± 2.1 vs. 5.1 ± 0.4 s in 0 mM Na+ in WT and mdx cells, respectively; Fig. 4D). While the higher frequency of Ca2+ oscillations can have several reasons, the shorter delay is a hallmark of increased RyR Ca2+ sensitivity (19).
Fig. 4.

Ca2+ oscillations in WT and mdx cells. A and B: representative cytosolic Ca2+ signals in a WT cardiomyocyte (A) and a mdx (B) cardiomyocyte upon rapid reduction to 70 mM Na+ or complete removal of Na+ from the external solution (0 mM Na+). C and D: averaged frequency of oscillations (C) and time delay to their initiation (D) in WT (solid bars; n = 19) and mdx (shaded bars; n = 8) cardiomyocytes. *P < 0.05; **P < 0.01.
To verify that the above observations are linked to a putatively increased Ca2+ sensitivity of RyRs in mdx myocytes, but not to changes in NCX activity itself, we estimated the influx of Ca2+ via NCX while eliminating SR function. The latter was achieved by the incubation of cells with thapsigargin (1 μM) and ryanodine (10 μM). Figure 5A shows a representative trace of slow changes in [Ca2+]i elicited by the rapid removal of external Na+ in a WT cardiomyocyte. Figure 5B shows the results of similar experiments in all WT (n = 11) and mdx (n = 5) cells studied with this protocol. There were no significant differences detected in the NCX-elicited Ca2+ influx in WT and mdx cells. Ca2+ influx via NCX in 70 mM Na+ raised cytosolic Ca2+ levels by 0.37 ± 0.05 and 0.33 ± 0.18 ΔF/F0 in WT and mdx cells, respectively. The increase was larger upon complete removal of Na+ but was not significantly different in the two groups. Cytosolic [Ca2+]i rose by 1.65 ± 0.28 and 1.13 ± 0.71 ΔF/F0 in WT and mdx myocytes. Taken together, these findings indicate an increased Ca2+ sensitivity of RyRs in mdx cells that may result in the dystrophy-related changes of E-C coupling.
Fig. 5.

Activity of the Na+/Ca2+ exchanger (NCX) in WT and mdx myocytes. A: Ca2+ influx into a WT cardiomyocyte upon rapid reduction to 70 mM Na+ or complete removal of Na+ from the external solution (0 mM Na+) with eliminated SR function (1 μM thapsigargin and 10 μM ryanodine). B: averaged intracellular Ca2+ responses to a stepwise reduction or removal of external Na+ in WT (solid bars; n = 11) and mdx (shaded bars; n = 5) cells.
Estimations of SR Ca2+ load.
When E-C coupling gain values are analyzed and compared among various experimental series or preparations, several confounding factors need to be considered. Importantly, the E-C coupling gain depends on the SR Ca2+ content (34). It has been shown that an elevated SR Ca2+ concentration ([Ca2+]SR) increases the open probability of RyR channels at any given cytosolic Ca2+ level (17). Moreover, the increase is nonlinear and much more pronounced at high [Ca2+]SR. This was the reason that we carried out most of our experiments at low SR Ca2+ loads to reduce interference resulting from small alterations of SR Ca2+ load. This is of particular relevance for the present experiments, because the SR Ca2+ content has been reported to be elevated in mdx cardiomyocytes (41). To minimize alterations of our gain estimates that could result from differences in SR Ca2+ load, we applied a voltage-clamp Ca2+ preloading protocol throughout the experiments (see Fig. 1A). Furthermore, to keep the SR Ca2+ content in the lower range, where the dependence of Ca2+ release on SR Ca2+ load is much less steep (34), we generally omitted Na+ from the pipette solution. This maneuver favors Ca2+ extrusion via NCX and reduced the SR Ca2+ load by ∼30%.
We compared SR Ca2+ content (and SR Ca2+ release) in WT and mdx cells under experimental conditions of low intracellular Na+ concentration ([Na+]i) using several complementary approaches: analysis of caffeine-induced intracellular Ca2+ transients and NCX currents and analysis of the inactivation kinetics of ICaL (Fig. 6). Figure 6A shows representative intracellular Ca2+ transients elicited by 10 mM caffeine in WT and mdx myocytes in patch-clamped cells at −40 mV. Figure 6B shows the averaged amplitudes of Ca2+ transients as estimated from caffeine-induced Ca2+ transients (2.88 ± 0.32 ΔF/F0 in WT cells and 3.49 ± 0.33 ΔF/F0 in mdx myocytes, respectively, n = 10 and 13). In the presence of 8 mM [Na+]i, SR Ca2+ content increased to 4.61 ± 0.68 ΔF/F0 in WT cells and 4.72 ± 0.38 ΔF/F0 in mdx cells, respectively (n = 8 in both groups; not shown). Thus, SR Ca2+ content was not significantly different between WT and mdx cells at either [Na+]i (P = 0.89 and P = 0.21 at 8 and 0 mM, respectively).
Fig. 6.

Estimation of luminal SR Ca2+ content. A: caffeine-induced cytosolic Ca2+ transients in a WT myocyte (black) and a mdx myocyte (red). Confocal line-scan images and average fluorescence signals are shown. B: averaged amplitudes of caffeine-induced Ca2+ transients in both types of cells. C: NCX current (top) and integrated NCX current (bottom) activated by caffeine-induced Ca2+ transients in a WT myocyte (left) and a mdx myocyte (right). D: averaged integrated NCX currents in WT (n = 6) and mdx (n = 8) myocytes. E: representative traces of ICaL during a test step from −40 mV to maximal current at 0 mV under control conditions in WT (black line) and mdx (red line) cells. F: fast (τ1) and slow (τ2) time constants of current inactivation at 0 mV at different [Ca2+]o in WT (black) and mdx (red) cells. At 1.2 mM [Ca2+]o, τ1 and τ2 were 14.5 ± 1.1 and 78.9 ± 6.1 ms (n = 42) in WT cells and 18.8 ± 2.0 and 87.7 ± 5.5 ms (n = 57) in mdx cells, respectively.
Integrated NCX currents activated by caffeine-induced Ca2+ transients are more reliable estimates of SR Ca2+ content because they do not depend on the particular time course of the caffeine-induced Ca2+ release. These estimates were even more similar in both types of myocytes than those derived from fluorescence transients (Fig. 6, C and D). Figure 6C shows representative traces of NCX current in WT and mdx myocytes (top left and top right traces, respectively) and the corresponding current integrals (bottom left and bottom right traces). The averaged data of integrated NCX currents are shown in Fig. 6D. They were 0.41 ± 0.09 pC/pF (n = 6) in WT cells and 0.43 ± 0.07 pC/pF (n = 8) in mdx cells.
Yet another, although more indirect, way to estimate luminal Ca2+ content and SR Ca2+ release is to compare the inactivation kinetics of ICaL. In cardiac myocytes, a massive release of Ca2+ from the SR prominently contributes to the inactivation of Ca2+ currents via a Ca2+-dependent mechanism (33). Membrane currents were measured during a voltage step from −40 to 0 mV. As before, the test depolarization was preceded by a series of preconditioning pulses to optimize SR Ca2+ load. Figure 6E shows representative traces of Imax in a WT cardiomyocyte and a mdx cardiomyocyte under control conditions (1.2 mM [Ca2+]o). The fast and slow time constants of current inactivation were not significantly different in WT and mdx cells studied at various [Ca2+]o (Fig. 6F).
Taken together, these results indicates that there were no significant differences in SR Ca2+ content between WT and mdx cells under our experimental conditions. Therefore, luminal Ca2+ is unlikely to explain the observed enhanced Ca2+ sensitivity of RyRs and hypersensitive E-C coupling in mdx myocytes.
E-C coupling gain in the presence of ROS scavengers.
There is increasing evidence of oxidative stress in the dystrophic heart, which is caused by an imbalance in the production of ROS and the cell's innate capability to inactivate them (20, 42). Permanent exposure of the cells to increased levels of ROS may severely damage several components of the cell, resulting in cell death. In a recent study (20), we found abnormally elevated ROS levels in dystrophic cardiomyocytes both at rest and after mechanical stress.
The RyR contains a number of free cysteine residues, which are prone to redox modifications. In the case of oxidation of the cytosolic environment, free and neighbored thiol groups may form disulfide bonds, thereby altering the secondary structure of the RyR and increasing its sensitivity to Ca2+ activation (10). We speculated that the increased intracellular levels of ROS observed previously may be responsible for the abnormal Ca2+ sensitivity of RyRs and consequently lead to unusually reliable E-C coupling in dystrophic myocytes. Therefore, we tested whether a reduction of cytosolic ROS levels would normalize E-C coupling in dystrophic myocytes. For these experiments, we used two approaches: 1) the addition of a synthetic compound (Mn-cpx3) that acts as a natural SOD mimetic, which helps to maintain a reducing environment within the cell; and 2) the addition of a general antioxidant (MPG), which directly interacts with the oxidized protein and reduces it.
Preincubation of mdx cells with either 10 μM Mn-cpx3 or 800 μM MPG for 30 min normalized SR Ca2+ release during E-C coupling under conditions of reduced [Ca2+]o and eliminated the hypersensitivity of E-C coupling. Figure 7 shows the averaged E-C coupling gain in dystrophic cardiomyocytes preconditioned with Mn-cpx3 and MPG, respectively, and studied in 0.5 and 0.25 mM [Ca2+]o. For better comparison, these data are shown together with some that are replotted from Figs. 2C and 3E. The E-C coupling gain of mdx myocytes pretreated with Mn-cpx3 or MPG was no longer significantly different from that in WT cells. Thus, reduction of intracellular levels of ROS and oxidative stress eliminated the hypersensitivity of RyRs toward Ca2+ and restored normal E-C coupling gain in dystrophic myocytes. Since RyRs are redox sensitive even at normal cytosolic redox potentials (10), treatment of WT myocytes with MPG also led to a reduction of E-C coupling gain, as expected.
Fig. 7.

Reduction of oxidative stress prevents the hypersensitivity of E-C coupling gain in mdx cardiomyocytes. E-C coupling gain data for WT and mdx are replotted from Figs. 2C and 3E for better comparison. Preincubation of mdx cells with 800 μM mercaptopropionyl-glycine (MPG; 30 min, n = 3) or with 10 μM Mn-cpx3 (30 min, n = 7) reduced the E-C coupling gain to levels similar to those in WT cells kept in control conditions (dashed lines). WT myocytes pretreated with 800 μM MPG also led to the expected reduction of the E-C coupling gain. *P < 0.05 and **P < 0.01.
DISCUSSION
Patients suffering from muscular dystrophy develop early cardiomyopathy with reduced cardiac force. Therefore, we expected that the contractility of dystrophic cardiomyocytes would be diminished. In particular, we anticipated that E-C coupling would be impaired. Surprisingly, our study revealed an extremely reliable E-C coupling mechanism in dystrophic cardiomyocytes, which is even more resistant to experimental challenges than in WT cells. This unique feature has not been previously observed in studies of other cardiac pathologies and may be due to an increased sensitivity of RyRs to Ca2+ resulting from redox modification of the channel proteins.
E-C coupling in dystrophic cardiomyocytes.
E-C coupling comprises the early steps that link electrical excitation of the cardiac muscle to mechanical contraction. The quality of the E-C coupling mechanism can be assessed by the E-C coupling gain, which is a measure for the effectiveness of a cardiomyocyte to amplify the Ca2+ influx via L-type Ca2+ channels by triggered Ca2+ release from the SR. Amplification of the cardiac Ca2+ signal is well controlled and not only depends on Ca2+ influx via L-type Ca2+ channels but also on the complex regulation of RyRs and accessory proteins as well as on SR Ca2+ content, ultrastructural features, and the metabolic state of the cell. Therefore, the amplification mechanisms are likely to be affected in various diseases. So far, only a few studies have specifically investigated this phenomenon by focusing on the actual E-C coupling mechanism. They found that the E-C coupling gain is significantly decreased in several animal models of heart failure or dilated cardiomyopathies (for examples, see Refs. 4, 12, 14, 26, 28, and 35). The reduction in E-C coupling gain could be, at least partially, responsible for the decreased cardiac contractility in these pathologies (but see Ref. 38).
In our present study, there was no obvious deficiency found when E-C coupling was analyzed under control conditions. Since E-C coupling presumably incorporates a high degree of reliability, this mechanism may have a large margin of safety, and small shifts in its sensitivity may not lead to obvious signaling disturbances. Thus, we needed experimental conditions to unmask even subtle alterations of E-C coupling. Our method to discover such changes was to challenge E-C coupling by reducing [Ca2+]o. This procedure has already proven useful in a previous study by McCall et al. (28), who showed that reducing the trigger signal for CICR by lowering [Ca2+]o can be used to reveal slight E-C coupling problems in heart failure. Whereas this test was well tolerated by control cells, in their study it lead to a pronounced and disproportionate decrease in contractile function in myocytes from failing hearts at similar trigger Ca2+ currents.
In our experiments, we used this method to reduce the safety margin for functional E-C coupling, so that the system does not operate above saturation any longer. With this approach, changes in the coupling between ICaL and RyR Ca2+ release are easier to uncover. When compared with the study on heart failure mentioned above (28), the dystrophic cardiomyocytes examined here behaved in the exact opposite way. Acutely lowering [Ca2+]o reduced Ca2+ release from the SR to a lesser extent in mdx cardiomyocytes than in WT cardiomyocytes. This resulted in an increase of E-C coupling gain, not only relative to that in WT cells but also compared with the gain at control [Ca2+]o. At this point, it is important to mention again that all experiments have been performed at matching SR Ca2+ load. Using our voltage protocol, conditioning pulses were always applied in control [Ca2+]o, and only the test step that directly followed the loading pulses was applied in different reduced [Ca2+]o.
The discovery of Ca2+ hypersensitivity at reduced [Ca2+]o does not mean that this hypersensitivity is not present under normal conditions. It may just be masked by the already redundant activation of RyRs during E-C coupling and is therefore best identified at smaller trigger ICaL (1). Thus, the physiological or pathophysiological relevance of the hypersensitivity is not limited to depolarizations to −25 and 0 mV but present for the entire range of membrane potentials that are covered during the cardiac action potential (see Fig. 2B). Therefore, our data indicate a hypersensitive E-C coupling mechanism in dystrophic cardiomyocytes, which are more resistant to this specific experimental challenge.
Altered Ca2+ sensitivity in dystrophic cardiomyocytes.
Increased E-C coupling gain actually means that Ca2+ is more easily released from the SR at similar trigger ICaL. Since the properties of ICaL in mdx myocytes showed no difference compared with WT myocytes, the critical changes of E-C coupling seemed to have occurred on the intracellular level, downstream of ICaL. Most likely, a change in RyR Ca2+ sensitivity has occurred. Several mechanisms are known to modify the actual or apparent Ca2+ sensitivity of RyRs. They include, but are not limited to, ultrastructural changes in the dyadic junction, changes in luminal Ca2+ concentration or [Ca2+]i, oxidative stress, and/or nitrosative stress.
At the level of the microarchitecture, it is conceivable that loss of the cytoskeletal protein dystrophin causes disarrangements in the dyadic cleft and disruption of the coupling between the L-type Ca2+ channel and RyR. However, one would expect that such structural changes lead to a reduction in the apparent Ca2+ sensitivity of the RyR and to a decrease in the E-C coupling gain. Such loss of function has been reported for a cardiac myocyte hypertrophy model (13). Pressure overload of the cardiomyocytes resulted in the disruption of the cytoskeleton, a significant decrease in E-C coupling efficiency, and a reduction in cardiac output. In contrast, a significant gain in the sensitivity of E-C coupling was observed in dystrophic cardiomyocytes.
An increase in [Ca2+]SR can also have profound consequences on RyR function and intracellular Ca2+ signaling (23), leading to elevated RyR Ca2+ sensitivity and even to spontaneous SR Ca2+-release events like Ca2+ waves (22). Potential alterations in the expression and function of several major SR-related proteins, such as RyRs, SR Ca2+ pumps, and calsequestrin, in mdx myocytes might modify SR Ca2+ refilling, Ca2+ leak, and, finally, SR Ca2+ content (27, 32, 41). Loss of dystrophin reduces the mechanical stability of the myocyte and may favor the formation of microruptures and activation of other Ca2+ influx pathways, thus leading to uncontrolled Ca2+ entry into the cells. The resulting slight elevation of resting [Ca2+]i found in mdx cardiomyocytes could, in principle, also add to a putative SR Ca2+ overload (20, 41).
Our data also show that slow increases in cytosolic Ca2+ via NCX operating in its Ca2+ influx mode trigger Ca2+ oscillations significantly earlier in mdx cells than in WT cells. This rapid response might be an indicator for higher diastolic [Ca2+]i, increased SR Ca2+ content, or abnormally high sensitivity of RyRs toward changes in [Ca2+]i. However, minimally raised diastolic Ca2+ levels are unlikely to account for the observed differences in E-C coupling in patch-clamped cells, where diastolic [Ca2+]i is also determined by the pipette solution and, thus, is similar in both WT and mdx myocytes. In addition, our voltage protocols were specifically designed to guarantee equal SR Ca2+ load before each test step. The repetitive application of preconditioning pulses in control [Ca2+]o ensured similar SR loading conditions throughout all experiments and for the test step at various [Ca2+]o. The latter was confirmed by estimates of SR Ca2+ content. A comparison of the caffeine-sensitive Ca2+ content of the SR revealed no significant differences, nor were there any differences in NCX activity in WT and dystrophic myocytes. Taken together, these observations suggest that the hypersensitivity of E-C coupling in mdx myocytes is unlikely to result from changes in [Ca2+]i and luminal [Ca2+]SR but rather is related to changes of RyR function.
Oxidative and nitrosative stress are known to have marked consequences on the activity of the macromolecular RyR complex. In particular, ROS/reactive nitrogen species have been described as potent modulators of RyR gating properties and Ca2+ sensitivity resulting in RyR hyperactivity and increased SR Ca2+ leak without the need of elevated SR Ca2+ load (2, 7, 15, 44). We and others (20, 42) have recently reported an increased basal ROS production in the dystrophic heart. In addition, we (20) have previously shown that ROS generated by NAD(P)H oxidase and mitochondria are causally involved in the excessive Ca2+ signaling response to mechanical stress observed in mdx cardiomyocytes. Recently, it was found that oxidative stress during overt heart failure can lead to RyR oxidation and elevated Ca2+ sensitivity, thus contributing to the elevated SR Ca2+ leak (37). Abnormal levels of ROS in dystrophic cardiomyocytes might therefore contribute to the enhanced Ca2+ sensitivity of RyRs and to the increased E-C coupling gain when the cardiomyopathy has not yet evolved into heart failure. Our experiments using reducing agents support the latter possibility. We (20) have previously shown that a number of different ROS reducing substances (MnTBAP, Mn-cpx3, tiron, and apocynin) effectively normalized the stress sensitivity of dystrophic cardiomyocytes. In the present study, we used Mn-cpx3, which acts as a SOD mimetic, and MPG, which directly reduces the proteins. Reducing the cytosolic ROS concentration and oxidative stress by these means eliminated the hypersensitive E-C coupling in mdx cells. Although through different mechanisms, both tested substances more or less led to the normalization of E-C coupling gain in dystrophic myocytes, suggesting that protein oxidation may indeed be involved. As expected, treatment of WT myocytes with the reducing agent MPG led to some reduction in E-C coupling gain, since the RyR open probability is also sensitive to changes in cytosolic redox potentials, even in normal animals (10).
Under normal and healthy conditions, RyR hypersensitivity by itself may not lead to any dramatic changes in E-C coupling. However, if we extrapolate our findings to conditions of mechanical stress and undue Ca2+ accumulation (due to microruptures and other voltage-independent Ca2+ influx pathways), as it is suspected for dystrophic myocytes, one can imagine that excess cytosolic Ca2+ may easily activate hypersensitive RyRs and initiate spontaneous, arrhythmogenic Ca2+ release from the SR–and even more so during β-adrenergic stimulation (29). Related to this notion, it is believed that in the presence of RyR hypersensitivity the combination of two (or more) proarrhythmogenic mechanisms dramatically increases the susceptibility for arrhythmias (40). In an animal model harboring a gain of function mutation in the cardiac RyR, such a “double-hit” scenario has been observed directly (6).
Similarly, hypersensitivity of RyRs caused by several recently discovered RyR mutations is known to have profound arrhythmogenic potential. In these patients, catecholaminergic polymorphic ventricular tachycardias (CPVTs) can be triggered by physical or emotional stress and cause sudden cardiac arrest (24). Thus, we speculate that the frequent CPVTs observed in dystrophic patients may also be linked to RyR hypersensitivity, at least in part (25). The fact that RyR Ca2+ hypersensitivity and E-C coupling gain can be normalized in dystrophic cells by antioxidants may open new perspectives for the therapeutical treatment of DMD patients.
Conclusions.
The key result of our study is the discovery of a RyR hypersensitivity for Ca2+ due to redox modifications in dystrophic cardiomyopathy, which is not only responsible for excessive stress responses but also changes the signal transduction linking L-type Ca2+ channels to RyRs during E-C coupling.
GRANTS
This work was supported by the Swiss Foundation for Research on Muscle Diseases (to E. Niggli and N. Shirokova), Swiss National Science Foundation Grant 31-109693.05 (to E. Niggli), the Muscle Dystrophy Association (to N. Shirokova), National Institute of Arthritis and Musculoskeletal and Skin Diseases Grant AR-053933 (to N. Shirokova), the American Heart Association (to N. Shirokova), and the Sigrist Foundation (to N. Shirokova and E. Niggli).
DISCLOSURES
No conflicts of interest are declared by the author(s).
ACKNOWLEDGMENTS
The authors thank Dr. John Reeves and Dr. Martha Nowycky for helpful comments on the manuscript. Technical help was provided by Daniel Luethi.
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