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Circulation Research. 1999;84:1459-1468

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(Circulation Research. 1999;84:1459-1468.)
© 1999 American Heart Association, Inc.


Rapid Communication

Ca2+ Waves During Triggered Propagated Contractions in Intact Trabeculae

Determinants of the Velocity of Propagation

Masahito Miura, Penelope A. Boyden, Henk E. D. J. ter Keurs

From the Department of Medicine (M.M., H.E.D.J.K.), University of Calgary, Calgary, Canada, and Department of Pharmacology (P.A.B.), Columbia College of Physicians and Surgeons, New York, NY.

Correspondence and reprint requests to Henk E.D.J. ter Keurs, MD, PhD, Department of Medicine, Health Science Centre, 3330 Hospital Dr NW, Calgary, Alberta, Canada T2N 4N1. E-mail terkeurs{at}ucalgary.ca


*    Abstract
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*Abstract
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down arrowMaterials and Methods
down arrowResults
down arrowDiscussion
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Abstract—During triggered propagated contractions, Ca2+ waves travel along cardiac trabeculae with a constant velocity (Vprop) ranging from 0.34 to 5.47 mm/s. To explore the determinants of Vprop, we studied (1) the relationship between [Ca2+]i and Vprop and (2) the effect of low concentrations of caffeine on Vprop. Trabeculae were dissected from the right ventricle of rat hearts. [Ca2+]i was measured using electrophoretically injected fura-2 and an image-intensified CCD camera. Force was measured using a silicon strain gauge, and sarcomere length was measured using laser diffraction techniques. After induction of reproducible Ca2+ waves by trains of electrical stimuli (2.5 Hz) at 21.9±0.2°C, the number of stimuli or [Ca2+]o was varied in 9 trabeculae. In 5 trabeculae, the effects of caffeine (0.1 to 1.0 mmol/L) at [Ca2+]o of 2.2±0.3 mmol/L were determined. All images were recorded under stable conditions of wave propagation. The increment in [Ca2+]i during the last electrically stimulated transient ({Delta}CaT) and [Ca2+]i just before onset of the Ca2+ waves (CaD) were used to estimate the Ca2+ loading of the sarcoplasmic reticulum (SR) and the myoplasm, respectively. The ratio ({Delta}CaW/{Delta}CaT) of the [Ca2+]i increment during the waves ({Delta}CaW) to {Delta}CaT was used to estimate the probability of opening of the SR-Ca2+ release channel during wave propagation. As a result of an increase of the number of stimuli or [Ca2+]o, Vprop increased in proportion to (1) {Delta}CaT (r=0.82); (2) CaD (r=0.88); (3) {Delta}CaW (r=0.85); and (4) {Delta}CaW/{Delta}CaT (r=0.74). The addition of caffeine (<=0.3 mmol/L) increased Vprop for any {Delta}CaT and any {Delta}CaW, revealing an increased sensitivity of Vprop to {Delta}CaT and {Delta}CaW. In contrast, caffeine had little effect on the relationship between Vprop and CaD and no effect on that between Vprop and {Delta}CaW/{Delta}CaT. These results suggest that both the cellular Ca2+ loading and open probability of the SR-Ca2+ release channels determine the velocity of propagation of Ca2+ waves.


Key Words: rat cardiac trabeculae • triggered propagated contraction • Ca2+ wave • caffeine


*    Introduction
up arrowTop
up arrowAbstract
*Introduction
down arrowMaterials and Methods
down arrowResults
down arrowDiscussion
down arrowReferences
 
Local aftercontractions starting from damaged regions of muscle propagate along cardiac trabeculae.1 2 The propagated contractions, which can be measured as waves of sarcomere shortening in both rat ventricular1 2 and human atrial trabeculae,3 have been denoted as triggered propagated contractions (TPCs). Recently, regional increases in [Ca2+]i have been observed to travel along rat cardiac trabeculae during TPCs and denoted as Ca2+ waves.4 These Ca2+ waves travel along trabeculae at the same velocities as TPCs, ranging from 0.34 to 5.47 mm/s.

Several studies have suggested that the propagation mechanism of TPCs is consistent with a model of Ca2+-induced Ca2+ release (CICR) from sarcoplasmic reticulum (SR) mediated by Ca2+ diffusion to adjacent SR.1 4 5 6 The velocity of propagation (Vprop) of TPCs varies depending on the [Ca2+]o, the number and frequency of the electrical stimuli,1 2 and the presence or absence of Ca2+ channel agonists and antagonists.7 These observations are consistent with the assumption that Ca2+ loading of the cell (SR Ca2+ content and/or cytosolic Ca2+) is a main determinant of Vprop. Therefore, we propose that the Ca2+ level in the myoplasm and/or SR can determine Vprop via modulation of CICR. Furthermore, computer simulation of CICR and Ca2+ diffusion supports the hypothesis that Vprop of Ca2+ waves (or TPCs) will be altered depending on the combined effects of an increase in (1) the diastolic [Ca2+]i; (2) the rate of rise of the Ca2+ release; and (3) the amount of Ca2+ released by the SR.8

At a low concentration (0.3 mmol/L), caffeine has been shown to increase Vprop and force.7 In addition, 0.5 mmol/L caffeine can increase the amplitude of delayed afterdepolarizations and cause triggered activity.9 10 11 12 Recently, caffeine has been shown to enhance the release of Ca2+ from the SR by activating a cardiac SR-Ca2+ release channel (RyR) incorporated into planar phospholipid bilayers.13 14 15 16 This activation of the channel leads to net shift of Ca2+ from SR to myoplasm, subsequently modulating Ca2+ loading level of the myoplasm and the SR. Thus, we hypothesize that the effect of caffeine on Vprop of TPCs is secondary to drug modulation of CICR due to the changes in Ca2+ levels in the myoplasm and SR.

Therefore, in the present study, we investigated (1) the relationship between [Ca2+]i and Vprop of Ca2+ waves to evaluate how Ca2+ levels in myoplasm and SR can affect Vprop and (2) the effect of caffeine on these relationships to evaluate whether Vprop is sensitive to changes in the probability of opening of the SR-Ca2+ release channel (Po) of RyR.


*    Materials and Methods
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up arrowAbstract
up arrowIntroduction
*Materials and Methods
down arrowResults
down arrowDiscussion
down arrowReferences
 
Dissection and Mounting of Rat Ventricular Trabeculae
The experiments in the present study were conducted in accordance with the principles outlined in the most recent Guide to the Care and Use of Experimental Animals by the Canadian Council on Animal Care. Lewis Brown Norway rats (Harlan Sprague-Dawley Inc, Indianapolis, Ind; 250 to 300 g) were anesthetized with diethyl ether. Twelve hearts were excised, and the coronary arteries were immediately perfused via the aorta with a Krebs-Henseleit (K-H) solution modified by adding 15 mmol/L KCl. After arrest of the heart, trabeculae (n=12, length 2.07±0.09 mm, width 207±37 µm, thickness 101±4 µm) were dissected from the right ventricle and mounted horizontally between a force transducer and a micromanipulator in a perfusion bath located on the stage of an inverted microscope (Nikon). Trabeculae were stimulated at 0.5 Hz through parallel platinum electrodes in the bath with 5-ms pulses 50% above threshold and superfused with bicarbonate buffered K-H solution containing (in mmol/L) NaCl 120, KCl 5, MgCl2 1.2, Na2SO4 1.2, NaH2PO4 2.0, NaHCO3 19, glucose 10, and CaCl2, as specified in the Results. The solutions were in equilibrium with 95% O2 and 5% CO2; pH was 7.4.

Fura-2 Loading and Measurement of Fluorescence
[Ca2+]i in the trabeculae was measured as previously described.4 Briefly, fura-2 pentapotassium salt was microinjected electrophoretically into one cell and allowed to spread throughout the trabeculae via gap junctions. After the injection, the trabeculae were stimulated at 1 Hz for 30 to 60 minutes until fura-2 had diffused uniformly throughout the preparation. The epifluorescence of fura-2 from the trabeculae at excitation wavelengths of 340 and 380 nm was measured at 510 nm by a photomultiplier tube (PMT) (PMT-R2693 with a C1053-01 socket, Hamamatsu). The signal from the PMT was stored in a personal computer through an analog-digital converter. Alternatively, the fluorescent image of the trabeculae at excitation wavelengths of 360 and 380 nm was recorded by a CCD camera coupled to a 2-stage image intensifier (IIC; model C330, General Scanning Inc) through a 510- to 560-nm bandpass filter. The images were recorded with a videocassette recorder (VCR) for offline analysis. The force of the muscle was measured using a modified silicon semiconductor strain gauge. Sarcomere length (SL) was measured using laser diffraction techniques.17

Analysis of the Signal From the PMT
[Ca2+]i was determined using the following equation18 (after subtraction of the autofluorescence of the muscle), as previously described4 : [Ca2+]i=Kdxßx(R-Rmin)/(Rmax-R), where Kd is the effective dissociation constant, R is the ratio of the fluorescence at 340-nm excitation to that at 380-nm excitation (340/380), Rmin is R at zero [Ca2+], Rmax is R at a saturating [Ca2+], and ß is the ratio of fluorescence value for Ca2+-free dye to fluorescence value for Ca2+-bound dye at 380-nm excitation. Because we have previously reported a good correlation between in vitro and in vivo calibrations when free Mg2+ was 1 mmol/L in the solutions mimicking the intracellular milieu,19 values for Kd, Rmin, Rmax, and ß were determined using in vitro calibrations. Rmin and Rmax were 0.152 and 4.60, and Kd and ß were 361 nmol/L and 9.18, respectively. This is in agreement with previous data from our laboratory.19

Analysis of an Image From the IIC
Fura-2 fluorescence images recorded at 30 frames per second on the VCR were analyzed as previously described.4 Briefly, fluorescence data of each video frame were digitized with an 8-bit analog-digital converter and stored in a frame buffer memory of 512x480 pixels (Coreco Inc). Therefore, in our optical system, one pixel corresponded to 2.9x2.9 µm in the image plane. For the analysis of the image, a region of interest (ROI) was set horizontally along the long axis of the fluorescence image of trabeculae. The length of the ROI was always 512 pixels (1470 µm) whereas its width was 20 pixels (57.4 µm). To obtain intensity profiles of the fluorescence along the long axis of trabeculae, we calculated an average intensity value from each transverse line of pixels within the ROI. To eliminate high-frequency noise from the intensity profile, we used a low-pass finite impulse response filter (MATLAB) with a cutoff frequency of 5 pixels (14.4 µm). After subtraction of autofluorescence, we calculated the ratio of the fluorescence at 360-nm to that at 380-nm excitation (360/380) at each point on the intensity profiles obtained from the images at 360- and 380-nm excitation light. To correct for the effects of nonuniform illumination of excitation light, we calculated [Ca2+]i at each sampling point after the induction of TPCs using the regression line derived from the relationship between PMT and the IIC ratio determined at the same sampling point. In addition, to avoid noise caused by low-excitation light intensity on the far edges of the profile of fluorescence, we calculated [Ca2+]i only at the regions of the centrally located 250 pixels (719 µm) of the profiles along the trabeculae.

To calculate Vprop, we identified the peak of a Ca2+ transient during the Ca2+ wave at each pixel along trabeculae and plotted the time of the maximum against the position of the peak. Vprop was calculated from the slope of the fitted line to the plot, when regression analysis showed a linear relationship (r>=0.9), as described previously.4

Experimental Protocol
To induce a Ca2+ wave (or TPC), bath temperature was lowered to 20°C to 23°C, and trains of electrical stimuli at 2.5 Hz were applied for 10 seconds at [Ca2+]o of 0.3 mmol/L. SL was set to 2.10 µm for all muscles. [Ca2+]o was then increased in steps of 0.2 mmol/L until a TPC appeared.1 2 The measurement of [Ca2+]i started when Vprop of Ca2+ waves (or TPCs) triggered by serial trains of stimuli varied by <10%. We regarded such Ca2+ waves as reproducible; reproducible conditions lasted at least 30 minutes. In the present study, we induced reproducible Ca2+ waves in 12 trabeculae. To change Ca2+ loading of the muscle, we varied [Ca2+]o and/or duration of the train of electrical stimuli in 9 trabeculae. The measurement of [Ca2+]i was started again when Ca2+ waves (or TPCs) reached a new steady state. Thus, we eventually analyzed 23 reproducible Ca2+ waves ([Ca2+]o 2.2±0.3 mmol/L, temperature 21.9±0.2°C).

The effect of caffeine on Ca2+ waves was studied using 7 reproducible Ca2+ waves elicited in 5 trabeculae (length 2.19±0.19 mm, width 228±57 µm, thickness 101±4 µm, [Ca2+]o 2.4±0.3 mmol/L, temperature 21.6±0.3°C, 10-second electrical stimulation at 2.5 Hz). When the Ca2+ waves were reproducible, trabeculae were superfused with K-H solution containing varied concentrations (0.1 to 1.0 mmol/L) of caffeine (Sigma). After the superfusion with caffeine, force development induced by trains of electrical stimuli was monitored and reached a new steady-state level within 5 minutes; measurement of [Ca2+]i was then begun. All measurements made in the presence of caffeine were completed within 30 minutes, and trabeculae were then superfused with caffeine-free K-H solution. After washout, we confirmed that the Ca2+ waves were still reproducible.

Data Analysis
To assess Ca2+ loading of myoplasm and SR, we calculated the following parameters (see Figure 1Down). First, we estimated the SR Ca2+ loading from the increment in [Ca2+]i during the last stimulated twitch of the trains ({Delta}CaT), ie, the difference between a peak of a Ca2+ transient during the twitch and the minimal [Ca2+]i preceding the last twitch. Second, we measured the diastolic [Ca2+]i (CaD) just before a Ca2+ wave, ie, the minimal [Ca2+]i observed between the last twitch and a subsequent TPC. Third, the amount of Ca2+ released during the wave was estimated from the increment in [Ca2+]i during a Ca2+ wave ({Delta}CaW), ie, the difference between the peak of a Ca2+ wave (Caw) and CaD. Using these parameters, we calculated {Delta}CaW/{Delta}CaT, the amount of Ca2+ released during the wave normalized for the SR Ca2+ content. We assumed that this parameter reflects the released fraction of Ca2+ inside SR and corresponds to the probability of Ca2+ release from SR during the wave (see Discussion). When obtained with use of the PMT (Figure 1Down), we will refer to these parameters as global changes in [Ca2+]i (g{Delta}CaT, gCaD, and g{Delta}CaW). When obtained from images recorded by the IIC, we first calculated these parameters at each pixel position along trabeculae and then averaged the values obtained at each pixel position. In that case, we will refer to the averaged values as regional changes in [Ca2+]i (r{Delta}CaT, rCaD, and r{Delta}CaW). Moreover, we measured developed force during the last twitch (FT) and that during a TPC (FTPC).



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Figure 1. Effect of changes in the duration of electrical stimuli on global changes in [Ca2+]i. Upper panels are changes in [Ca2+]i calculated from the fluorescence signals recorded by the PMT, and the lower panels are 2 force recordings (normalized for cross-sectional area of the muscle) at the 340- and 380-nm excitation wavelength during the last 2 electrically stimulated twitches and a subsequent TPC. The arrows indicate an increase in [Ca2+]i (upper panel) and an aftercontraction (lower panel) during which a TPC was observed. S indicates moment of electrical stimulation (temperature 23.1°C, [Ca2+]o 3.0 mmol/L, experiment 970110). A, Electrical stimulation at 2.5 Hz for 5 seconds. g{Delta}CaT indicates an increment in [Ca2+]i during the last stimulated twitch; gCaD, a diastolic [Ca2+]i just before a Ca2+ wave; g{Delta}CaW, an increment in [Ca2+]i during a Ca2+ wave; and gCaW, a peak of [Ca2+]i during a Ca2+ wave. B, Electrical stimulation at 2.5 Hz for 15 seconds. g{Delta}CaT increased from 508 to 604 nmol/L, gCaD increased from 213 to 256 nmol/L, and g{Delta}CaW increased from 90 to 204 nmol/L (upper panel). FT increased from 28.6 to 30.2 mN/mm2 and FTPC increased from 10.1 to 13.8 mN/mm2 (lower panel).

Statistics
All averaged values were expressed as mean±SEM. Single-factor ANOVA, unless stated otherwise, was used to detect significant differences (P<0.05).


*    Results
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up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
*Results
down arrowDiscussion
down arrowReferences
 
Figures 1Up and 2Down show clearly that Ca2+ waves are accelerated by Ca2+ loading.4 To change Ca2+ loading of the muscle, we increased [Ca2+]o or the duration of the train of electrical stimuli after the induction of reproducible Ca2+ waves. Figure 1Up shows global [Ca2+]i and force development during the last 2 electrically stimulated twitches of a train at 2.5-Hz stimulation. With a longer period of stimulation, all parameters of global [Ca2+]i (g{Delta}CaT, gCaD, and g{Delta}CaW) increased by 19%, 20%, and 127%, respectively, and parameters of force (FT and FTPC) increased by 6% and 37%, respectively. In Figure 2Down, regional changes in [Ca2+]i during comparable TPCs were determined directly after the recordings in Figure 1Up. With a longer period of stimulation, Vprop of the Ca2+ wave increased from 2.92 to 4.40 mm/s. The parameters of regional [Ca2+]i (r{Delta}CaT, rCaD, and r{Delta}CaW) also increased in proportion to each other (Figure 3Down).



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Figure 2. Effect of changes in the duration of electrical stimuli on regional changes in [Ca2+]i. The regional [Ca2+]i calculated from the images by the IIC during the last electrically stimulated twitch and a TPC a few minutes after the recording of the PMT shown in Figure 1Up. Abscissa represents time; ordinate, [Ca2+]i; and z-axis, the position along the long axis of the trabecula. s indicates moment of electrical stimulation (experiment 970110). A, Electrical stimulation for 5 seconds. After the end of the clearly uniform stimulated Ca2+ transient, a small Ca2+ transient was observed to move as a wave from position A (*) toward position B at the calculated Vprop of 2.92 mm/s. B, Electrical stimulation for 15 seconds. Vprop increased to 4.40 mm/s. In addition, r{Delta}CaT increased from 555 to 615 nmol/L, rCaD increased from 165 to 245 nmol/L, and r{Delta}CaW increased from 157 to 245 nmol/L.



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Figure 3. Relationships between Vprop and the regional changes in [Ca2+]i under control conditions (n=23). Vprop was tightly and linearly correlated with r{Delta}CaT (A), rCaD (B), r{Delta}CaW (C), and r{Delta}CaW/r{Delta}CaT (D). Note that all Ca2+ parameters correlate strongly and linearly, indicating that the Ca2+ loading of the muscle caused a proportional increase of rCaD, r{Delta}CaW, and r{Delta}CaT. In addition, r{Delta}CaW/r{Delta}CaT increased in proportion with the Ca2+ loading of the muscle (for further explanation, see text).

Ca2+ loading of the muscle increased the amplitude of TPCs and accelerated their propagation. As a result, TPCs already did occur in between the twitches during the stimulus train (Figure 1Up), which might cause nonuniformity of the Ca2+ release process during the (last) twitch that preceded the TPC, which was analyzed here. The nonuniformity of Ca2+ transients after the last stimulus along the analyzed region appeared to be small. The maximal difference in peak amplitude of r{Delta}CaT was <40 nmol/L whereas rCaD differed <20 nmol/L between both ends of the ROI (data not shown). Hence, we believed that activation of the ROI was sufficiently uniform to permit evaluation of the factors that dictate the rate of propagation of the Ca2+ waves occurring after the twitch.

Data obtained from 23 reproducible Ca2+ waves from 12 trabeculae showed that Vprop correlated strongly with r{Delta}CaT (Figure 3AUp), rCaD (Figure 3BUp), and r{Delta}CaW (Figure 3CUp) as well as r{Delta}CaW/r{Delta}CaT (Figure 3DUp). In 15 Ca2+ waves from 8 trabeculae, Vprop also correlated linearly with FT (r=0.70) and FTPC (r=0.67) (data not shown), as we have described previously.7 The increase of cytosolic Ca2+ correlated with r{Delta}CaT (Figure 3Up) and FT (not shown). FT is proportional to the amplitude of rapid cooling contractures (H. Banijamali, H.E.D.J. ter Keurs, unpublished observations, 1994) so that one may conclude that Ca2+ loading in our experiments led to proportional increases in cytosolic Ca2+ and in the SR Ca2+ content (reflected by r{Delta}CaT) of the muscle.

It was striking that r{Delta}CaW/r{Delta}CaT under drug-free conditions increased linearly with both r{Delta}CaT and rCaD (Figure 3Up). The increase of this ratio suggests that an increase of the Ca2+ loading of the muscle increases the probability of opening of the SR-Ca2+ channels during the wave. Ca2+ wave propagation accelerated with an increase in the latter parameter (r{Delta}CaW/r{Delta}CaT; Figure 3DUp). Regional measurements showed that acceleration of the Ca2+ wave was not the cause of the larger amplitude of the transient owing to faster wave propagation, as would be observed in the recordings with the PMT, which collected the fluorescence from a larger region in the muscle.4

To modify the kinetics of net Ca2+ transport from the myoplasm to the SR, 5 trabeculae were superfused with caffeine (0.1 to 1.0 mmol/L) after the induction of a reproducible Ca2+ wave. Figure 4Down shows an example of the global [Ca2+]i and the force development during the last 2 stimulated twitches in a train and a subsequent TPC in the absence and in the presence of caffeine. The addition of 0.3 mmol/L caffeine decreased the amplitude of g{Delta}CaT by 47% while gCaD and g{Delta}CaW increased by 51% and 91%, respectively. FT also decreased (27%) whereas FTPC increased (113%). In the presence of 1.0 mmol/L caffeine, we could neither detect an increase in [Ca2+]i nor an aftercontraction following the train of electrical stimuli. g{Delta}CaT and FT decreased by 77% and 55%, respectively. The diastolic diffraction pattern was uniform and stationary whereas twitch force during the train stayed constant. These observations suggested that random spontaneous sarcomere contractions occurred only rarely in the presence of 1 mmol/L caffeine.



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Figure 4. Effects of caffeine on global changes in [Ca2+]i in a typical trabecula. Upper panels show global changes in [Ca2+]i calculated from the PMT signals, and lower panels show force recordings during the last 2 electrically stimulated twitches in a train and a subsequent TPC in one trabecula using a similar protocol as in Figure 1Up. S indicates moment of electrical stimulation (temperature 21.9°C, [Ca2+]o 2.0 mmol/L, experiment 970214). A, In the absence of caffeine. The arrows indicate an increase in [Ca2+]i (upper panel) and an aftercontraction (lower panel) during which a TPC was observed. g{Delta}CaT, gCaD, and g{Delta}CaW were 697, 163, and 53 nmol/L, respectively (upper panel). FT and FTPC were 28.3 and 1.6 mN/mm2, respectively (lower panel). B, In the presence of 0.3 mmol/L caffeine. The arrows indicate an increase in [Ca2+]i (upper panel) and an aftercontraction (lower panel) during which a TPC was observed. g{Delta}CaT decreased to 369 nmol/L whereas gCaD and g{Delta}CaW increased to 246 and 101 nmol/L, respectively (upper panel). FT decreased to 17.3 mN/mm2 whereas FTPC increased to 3.4 mN/mm2 (lower panel). C, In the presence of 1.0 mmol/L caffeine. We could neither detect an increase in [Ca2+]i nor an aftercontraction subsequent to the train of electrical stimuli. g{Delta}CaT and FT decreased to 158 nmol/L and 11.8 mN/mm2, respectively.

Figure 5Down shows the last stimulated Ca2+ transient(s) and a cytosolic Ca2+ wave during the TPC in the absence (Figure 5ADown) and in the presence of 0.3 mmol/L caffeine (Figure 5BDown). The addition of 0.3 mmol/L caffeine increased the calculated Vprop from 1.86 to 6.39 mm/s. r{Delta}CaT decreased by 43%, but both rCaD and r{Delta}CaW increased by 40% and 115%, respectively.



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Figure 5. Effects of caffeine on regional changes in [Ca2+]i in the trabecula of Figure 4Up. The regional [Ca2+]i calculated from the images by the IIC during the last electrically stimulated twitch and a TPC a few minutes after the recording of the PMT shown in Figure 4Up. In these 3-dimensional representations, the axes are the same as those in Figure 2Up. After the end of the clearly uniform stimulated Ca2+ transient, a small Ca2+ transient appeared to move from A (*) toward B (for explanation, see text). s indicates moment of electrical stimulation (experiment 970214). A, Before the addition of caffeine. The calculated Vprop was 1.85 mm/s. B, After the addition of 0.3 mmol/L caffeine. Vprop increased to 6.39 mm/s. rCaD increased from 161 to 226 nmol/L, and r{Delta}CaW increased from 66 to 142 nmol/L whereas r{Delta}CaT decreased from 616 to 351 nmol/L.

Figure 6Down shows the effects of caffeine on global and regional changes in [Ca2+]i and Vprop. The twitch Ca2+ transient declines to {approx}25% of the control value whereas diastolic Ca2+ increased monotonically even at 1 mmol/L caffeine. This observation would be expected if caffeine eliminates contribution of the SR to the twitch, leaving only Ca2+ transport across the sarcolemma to supply and remove Ca2+. Ca2+ waves and aftercontractions increased and accelerated with caffeine up to 0.3 mmol/L, but they always disappeared after the addition of 1.0 mmol/L caffeine (n=3). Thus, we measured g{Delta}CaT, gCaD, and g{Delta}CaW at caffeine concentrations of 0, 0.1, 0.3, and 0.5 mmol/L (n=7, 3, 7, and 4, respectively) and measured g{Delta}CaT at 1.0 mmol/L caffeine (n=3). At these concentrations, g{Delta}CaT decreased and gCaD increased; g{Delta}CaW increased at 0.1 mmol/L caffeine but then decreased at 0.5 mmol/L caffeine. Measurement of regional [Ca2+]i changes in 2 of 7 muscles tested at 0.3 mmol/L caffeine and in all 4 muscles tested at 0.5 mmol/L caffeine became inaccurate, because Vprop became too fast to be calculated from video frames obtained at 30 per second. Thus, we calculated r{Delta}CaT, rCaD, r{Delta}CaW, and Vprop in control, 0.1 mmol/L, and 0.3 mmol/L caffeine (n=7, 3, and 5, respectively). At these concentrations, r{Delta}CaT decreased significantly whereas Vprop increased in the presence of caffeine; r{Delta}CaW increased at 0.1 mmol/L caffeine.



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Figure 6. Effects of caffeine on global ({circ}) and regional (•) changes in [Ca2+]i and Vprop. gCaD (P<0.05 [B]) and Vprop (P<0.01 [D]) increased significantly in the presence of caffeine whereas g{Delta}CaT and r{Delta}CaT decreased (P<0.0001 [A]). g{Delta}CaW (P<0.005 [C]) and r{Delta}CaW (P<0.05) increased at 0.1 mmol/L caffeine but then decreased in the presence of 0.5 mmol/L caffeine.

FT also decreased to 72.8±3.3% (P<0.005) and 62.0±3.5% (P<0.0005) of control FT in the presence of 0.1 and 0.3 mmol/L caffeine whereas FTPC increased to 147±11.2% (P<0.05) and 201±21.5% (P<0.01) of control FTPC, respectively (unpaired t test with unequal variation). The data obtained in each muscle in the presence of the drug were compared, for this analysis, with the data from the same muscle in the drug-free state ([Ca2+]o 2.1±0.2, temperature 21.8±0.2).

The data in Figure 6Up suggest that caffeine decreases {Delta}CaT while it increases {Delta}CaW at 0.1 mmol/L. This would be consistent with the effect of caffeine to cause an increase of the probability of opening of the SR-Ca2+ channels, increasing Ca2+ leak from the SR.13 14 15 16 17 The expectation that {Delta}CaW/{Delta}CaT reflects the probability of opening of the SR-Ca2+ channels is indeed met by observation of the effect of caffeine. Figure 7ADown shows that caffeine (0.1 to 0.5 mmol/L) increased both global and regional {Delta}CaW/{Delta}CaT significantly. Changes in force development (FTPC/FT) in the same muscles in the presence of caffeine increased significantly with increased caffeine concentration (Figure 7BDown).



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Figure 7. Effects of caffeine on global ({circ}) and regional (•) {Delta}CaW/{Delta}CaT (A) and FTPC/FT (B). The global and regional {Delta}CaW/{Delta}CaT and FTPC/FT increased significantly (P<0.005) in the presence of caffeine.

Figure 8Down shows the effects of caffeine on the relationship between Vprop and regional changes in [Ca2+]i of 8 Ca2+ waves from 5 trabeculae. For reference, control data (Figure 3Up) in the absence of caffeine are reproduced as open circles ({circ}). In the presence of caffeine, there remains a reasonable relationship between Vprop and r{Delta}CaT (Figure 8ADown) and r{Delta}CaW (Figure 8CDown). However, if we assume that r{Delta}CaT reflects the SR Ca2+ content in both drug-free and drug-containing solutions, then we are struck by the observation that the small r{Delta}CaT in caffeine are associated with waves with higher Vprop (leftward shift only). This suggests to us that caffeine renders Vprop of Ca2+ waves more sensitive to SR Ca2+ content. It appears that in the presence of caffeine, Ca2+ waves (r{Delta}CaW) similar in size to control waves propagate faster (parallel shift upward only), again suggesting that the higher Vprop reflects an increased sensitivity to the SR Ca2+ content.



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Figure 8. Effects of caffeine on the relationships between Vprop and regional changes in [Ca2+]i. In the presence of caffeine (0.1 and 0.3 mmol/L), the relationships between Vprop and r{Delta}CaT (r=0.71 [A]) and r{Delta}CaW (r=0.81 [C]) moved leftward and upward whereas the relationships between Vprop and rCaD (r=0.93 [B]) and r{Delta}CaW/r{Delta}CaT (r=0.74 [D]) showed little change. {circ} indicates in the absence of caffeine; •, in the presence of 0.1 mmol/L caffeine, and {blacksquare}, in the presence of 0.3 mmol/L caffeine.

In contrast, caffeine has little effect on the relationships between Vprop and rCaD (Figure 8BUp) or r{Delta}CaW/r{Delta}CaT (Figure 8DUp) seen in control, although an increase of Vprop correlated with increased r{Delta}CaW/r{Delta}CaT in the presence of caffeine. The relationship between Vprop and FTPC/FT is not altered by caffeine (data not shown). Clearly, Figure 8DUp shows that the rate of propagation increases in proportion to the increase in fractional Ca2+ release during a wave (reflected by r{Delta}CaW/r{Delta}CaT). Thus, caffeine increases fractional Ca2+ release (increased r{Delta}CaW/r{Delta}CaT) with a commensurate increase of Vprop.

As stated, we assumed that the probability of opening of the SR-Ca2+ channels would be reflected by the amount of Ca2+ released from the SR relative to the SR Ca2+ content ({Delta}CaW/{Delta}CaT). The observation that both the cellular Ca2+ loading (as reflected by r{Delta}CaT, rCaD, and rCaW) and caffeine13 14 15 16 increased r{Delta}CaW/r{Delta}CaT (Figure 9Down) is consistent with this prediction. In control drug-free conditions, increases in r{Delta}CaT, rCaD, and rCaW resulted in a concomitant increase in r{Delta}CaW/r{Delta}CaT. Caffeine increased r{Delta}CaW/r{Delta}CaT {approx}2-fold (Figure 9BDown and 9CDown). Intriguingly, caffeine shifted the relationship between r{Delta}CaW/r{Delta}CaT and r{Delta}CaT more dramatically to the left (Figure 9ADown), suggesting a stronger dependence of {Delta}CaW/{Delta}CaT on the SR Ca2+ content than on CaD.



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Figure 9. Relationships between r{Delta}CaW/r{Delta}CaT and regional changes in [Ca2+]i in the absence of caffeine ({circ}) and after the addition of 0.1 mmol/L (•) and 0.3 mmol/L caffeine ({blacksquare}). After the addition of caffeine (0.1 and 0.3 mmol/L), the relationships between Vprop and r{Delta}CaT (A), rCaD (B), and r{Delta}CaW (C) moved upward.


*    Discussion
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
up arrowResults
*Discussion
down arrowReferences
 
To our knowledge, this is the first study to characterize the determinants of Ca2+ wave propagation by direct measurement of the spatial and temporal properties of Ca2+ changes in a cardiac multicellular preparation during TPCs. Figure 10Down summarizes our observations suggesting that (1) both increased cytosolic Ca2+ (CaD) and SR Ca2+ loading ({Delta}CaT) influence Vprop through the modulation of Po of RyR ({Delta}CaW/{Delta}CaT) by facilitating CICR, (2) the diastolic [Ca2+]i level (CaD) may determine Vprop by facilitating diffusion of Ca2+ ions, and (3) at constant cytosolic [Ca2+] and SR Ca2+ loading, caffeine accelerates Vprop by directly increasing the Po of RyR ({Delta}CaW/{Delta}CaT).



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Figure 10. The proposed scheme of events that lead to an acceleration of traveling of Ca2+ waves (and TPCs). Ca2+ loading of the cell increases the SR Ca2+ content and cytosolic Ca2+ level. Both parameters increase the Po of RyR. In addition, the increase of the diastolic [Ca2+]i will increase occupancy of Ca2+ ligands in the cell and increase the effective diffusion coefficient. These effects would decrease the time needed to release Ca2+ from adjacent SR and thus increase the velocity of propagation of the Ca2+ waves. The effect of caffeine can be explained by its direct action on the Po of the RyR (see text for further explanation).

Effect of SR Ca2+ Content, Cytosolic Ca2+, and Diastolic Ca2+ on Vprop
It is obvious that CaD only reflects the cytosolic Ca2+ in between the contractions and depends on extrusion of Ca2+ from the cytosol. Most of the Ca2+ ({approx}80%) during the twitch in rat cardiac muscle is provided by Ca2+ release from SR20 21 22 23 24 and leads to the [Ca2+]i rise, {Delta}CaT. Our assumption that {Delta}CaT correlated with the SR Ca2+ content was further supported by the observation that the amplitude of the twitch is proportional to that of rapid cooling contractures (data not shown). So, {Delta}CaT eliciting the twitch could be taken to reflect the SR Ca2+ content. This interpretation requires caution, because the last twitch of the train nearly always followed a Ca2+ wave, which may have caused nonuniformity of Ca2+ release during this twitch.25 However, regional measurements of {Delta}CaT showed that this effect was minimal in the range of Ca2+ loading, which we have used. We have assumed that Ca2+ ions during a Ca2+ wave are also released from the SR,25 26 since it has been shown that TPCs are abolished by agents that interfere with SR Ca2+ loading or release, such as ryanodine and caffeine7 (Figure 6Up). Thus, we assumed that {Delta}CaT reflects the SR Ca2+ content available for release, and that {Delta}CaW reflects the amount of Ca2+ released from the SR during the Ca2+ wave. It follows that the released fraction of the SR Ca2+ content during the wave ({Delta}CaW/{Delta}CaT) reflects the probability of opening of SR-Ca2+ release channel.

It has been reported that the Po of cardiac RyR incorporated into planar phospholipid bilayers can be modulated by intraluminal SR Ca2+16 27 28 29 30 as well as by cytosolic Ca2+.31 32 These studies have shown that elevation of [Ca2+] on either the luminal or cytosolic side increases Po of RyR. The relationships between r{Delta}CaW/r{Delta}CaT and r{Delta}CaT on the one hand (Figure 9AUp) and rCaD on the other hand (Figure 9BUp and 9CUp) suggest that under drug-free conditions, SR Ca2+ content and cytosolic Ca2+ during a Ca2+ wave indeed determine the released fraction of Ca2+ from inside the SR, possibly by modulating the probability of opening of the SR-Ca2+ channels. If so, our observations are consistent with the features of RyR measured using phospholipid bilayers.16 27 28 29 30 31 32

It follows from the tight correlations between Vprop and r{Delta}CaT, rCaD, r{Delta}CaW, and r{Delta}CaW/r{Delta}CaT described in Figure 3Up that Vprop is facilitated under conditions of a higher SR Ca2+ content, a higher diastolic [Ca2+]i, and a larger amount of Ca2+ released from SR and possibly Po. These findings were predicted by computer simulation of Ca2+ waves using a model of CICR and Ca2+ diffusion.8 These observations are conceptually summarized in Figure 10Up, assuming that Ca2+ waves (or TPCs) travel along trabeculae, owing to the combination of CICR and Ca2+ diffusion.1 4 5 6 The simplest explanation of the observations is that SR Ca2+ content and cytosolic Ca2+ increase Po of RyR. The latter effect would increase fractional Ca2+ release from the SR during a Ca2+ wave (r{Delta}CaW/r{Delta}CaT), thus decreasing the time needed to release Ca2+ from adjacent release sites during propagation of the Ca2+ wave. We cannot prove from these data that the SR Ca2+ content influences Po, as has been suggested by lipid bilayer studies,16 27 28 29 30 but our data are certainly consistent with this hypothesis.

An increase in diastolic Ca2+ decreases the buffering capacity for Ca2+33 34 35 36 because of the increased Ca2+ binding to ligand proteins, as shown in Figure 10Up. With reduced buffering capacity for Ca2+, Ca2+ will diffuse faster,37 and Ca2+ release in adjacent SR will be "induced" earlier.

Effect of Caffeine
Caffeine has been reported to enhance the sensitivity of the myofilaments to Ca2+38 and inhibit net Ca2+ uptake by the SR.39 40 Recently, it has been concluded from studies using cardiac RyR incorporated into planar lipid bilayers that caffeine can increase the sensitivity of RyR to Ca2+15 and increase Po of RyR.13 14 16 28 The increase in Po of RyR can enhance the release of Ca2+ from SR and result in an increase in [Ca2+]i. On the other hand, the increase in Po reduces SR Ca2+ content and eventually depletes the SR of Ca2+, depending on the concentration of caffeine. The observation that caffeine produced an increase in CaD and a decrease in {Delta}CaT (or FT) (Figure 6AUp and 6BUp) is consistent with this concept. With caffeine at 1.0 mmol/L, Ca2+ waves (and TPCs) disappeared, probably as a result of Ca2+ depletion of the SR. We assume that the decrease in {Delta}CaT (and FT) in the presence of caffeine is due to a net decrease in SR Ca2+ content available for release but not due to the preceding spontaneous Ca2+ transient (and aftercontraction) for the following reasons. First, g{Delta}CaT in the presence of 1.0 mmol/L caffeine was significantly smaller than that of 0.1 to 0.3 mmol/L caffeine (Figure 6AUp), although spontaneous Ca2+ transient (and aftercontractions) had already disappeared at 1.0 mmol/L caffeine. Second, in the presence of 0.1 and 0.3 mmol/L caffeine, the developed force triggered by the last stimulus of a train changed by <10% of that triggered by the first one of the train, which was not preceded by aftercontractions. Therefore, our observations are consistent with the effect of caffeine on RyR observed within lipid bilayers.13 14 15 16 29

In the presence of caffeine, the relationships between Vprop and rCaD (Figure 8BUp) and r{Delta}CaW/r{Delta}CaT (Figure 8DUp) were almost similar to control. This means that caffeine has little effect on the mechanisms that link rCaD and r{Delta}CaW/r{Delta}CaT to Vprop. In contrast, the relationships between Vprop and r{Delta}CaT (Figure 8AUp) and r{Delta}CaW (Figure 8CUp) suggest that caffeine makes Vprop much more sensitive to the SR Ca2+ content. This means that caffeine has a substantial effect on the pathway(s) that couple(s) r{Delta}CaT or r{Delta}CaW to Vprop. As suggested in Figure 10Up, caffeine increases Po of RyR similar to SR Ca2+ content and cytosolic Ca2+. The latter effect of caffeine would increase fractional Ca2+ release from the SR during a Ca2+ wave (r{Delta}CaW/r{Delta}CaT), as shown in Figures 7Up and 9Up, and would decrease the time needed to release Ca2+ from adjacent release sites during propagation of the Ca2+ wave. Hence, for any level of SR Ca2+ loading, Vprop would increase, owing to caffeine (Figure 8AUp). Vprop would also increase, even if the amplitude of the Ca2+ propagating transient would be constant, as is shown by Figure 8CUp.

Limitations of the Study
It is well known that the unitary SR Ca2+ release event in both cardiac cells and muscle consists of Ca2+ sparks.41 Ca2+ sparks have been described to underlie propagating Ca2+ waves41 42 at low levels of cellular loading (Cao {approx}50% of the EC50). Such Ca2+ waves travel a distance of only a few sarcomeres.41 42 Although it is tempting to assume that the microscopic waves observed in that study could consist of an avalanche of propagating Ca2+ sparks, our methods do not permit statements to this effect for the following reasons. First, we used fura-2, which does not exhibit a high enough photon efficiency to permit visualization of sparks. Second, the use of conventional microscopy precludes evaluation of events, which occur at a submicron scale. Hence, the fundamental question whether Ca2+ release by RyR (Ca2+ sparks) together with diffusion of Ca2+ from terminal cisterna to terminal cisterna (2 µm) causes Ca2+ waves as observed in the present study has to await exploration using probes such as confocal microscopy. This approach is important because theoretical modeling of propagation of Ca2+ waves has put the challenging constraint on the model that Ca2+ release from the SR has to occur in a fraction of a millisecond8 to permit Vprop to reach values of several millimeters per second. Even though it has been shown that opening of RyR exhibits rapid kinetics,43 the capacity of the channel to Ca2+ release on a submillisecond timescale remains to be proven.


*    Acknowledgments
 
This work was supported by grants from the Alberta Heart and Stroke Foundation and a NATO Collaborative Research Grant. Dr ter Keurs is a Medical Scientist of the Alberta Heritage Foundation for Medical Research (AHFMR). Dr Miura holds a postdoctoral research fellowship from Merck Frosst Canada Inc.

Received March 9, 1999; accepted April 19, 1999.


*    References
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
up arrowResults
up arrowDiscussion
*References
 
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Right arrow Articles by Keurs, H. E. D. J. t.
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