AJP - Heart Calcium Transients and Cell-Sarcomere
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Am J Physiol Heart Circ Physiol 273: H2481-H2489, 1997;
0363-6135/97 $5.00
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Vol. 273, Issue 5, H2481-H2489, November 1997

Ionic basis of ryanodine's negative chronotropic effect on pacemaker cells isolated from the sinoatrial node

Jin Li, Jihong Qu, and Richard D. Nathan

Department of Physiology, Texas Tech University Health Sciences Center, Lubbock, Texas 79430

    ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
References

Spontaneous electrical activity and indo 1 fluorescence ratios were recorded simultaneously in cultured pacemaker cells isolated from the rabbit sinoatrial node. Ryanodine (10 µM) reduced the amplitude of action potential-induced intracellular Ca2+ (Ca2+i) transients by 19 ± 3%, increased the time constant for their decay by 51 ± 5%, and slowed spontaneous firing by 32 ± 3%. 1,2-Bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid (BAPTA)-acetoxymethyl ester (AM; 25 µM) inhibited the Ca2+i transients and slowed spontaneous firing by 28 ± 4%. Ryanodine did not alter hyperpolarization-activated or time-independent inward current, but it reduced the sum of L- and T-type Ca2+ currents (ICa,L and ICa,T) in both the presence and absence of BAPTA-AM. In contrast, ICa,L was unchanged by ryanodine. Slow inward current tails, presumed to be Na/Ca exchange current (INa/Ca), were abolished by BAPTA or ryanodine. The results suggest that a decrement of ICa,T, due to reduction of the intracellular Ca2+ concentration or a direct effect of ryanodine on T-type Ca2+ channels, contributes to the negative chronotropic effect. Another possibility, based primarily on theory and results in other preparations, is that a reduction of INa/Ca, as a consequence of the smaller action potential-induced Ca2+i transients, contributes to the effect of ryanodine.

L-type calcium current; T-type calcium current; sodium/calcium exchange current; indo 1; 1,2-bis(2-aminophenoxy) ethane-N,N,N',N'-tetraacetic acid; perforated-patch voltage-clamp technique

    INTRODUCTION
Top
Abstract
Introduction
Methods
Results
Discussion
References

RYANODINE, A COMPOUND that reduces by twofold the conductance of Ca2+-release channels in the sarcoplasmic reticulum (SR) (25), slows the final phase of diastolic depolarization and, therefore, pacemaker activity in a number of cardiac preparations: strips of dilated human right atrium (7), subsidiary pacemaker cells of cat right atrium (26), pacemaker cells of cat (18) and guinea pig (24) sinoatrial (SA) nodes, and pacemaker cells isolated from cat right atrium (32) and rabbit SA node (17). The present study was designed to test the hypothesis that ryanodine's negative chronotropic effect on rabbit SA node cells is due to a reduction of inward currents that are modulated by intracellular Ca2+ (Ca2+i). The fluorescent indicator indo 1 was used to monitor Ca2+i, and the perforated-patch configuration of the whole cell patch-clamp technique (15) was employed to record spontaneous electrical activity and ionic currents in single pacemaker cells after 2 or 3 days in culture. Indo 1 allows continuous detection of two emission wavelengths and their ratio, thereby avoiding the switching time required for dual-excitation fluorescent indicators like fura 2. The perforated-patch technique avoids complete dialysis of the cytoplasm by the patch pipette, thereby preventing the loss of compounds that are essential for automaticity (19, 21). 1,2-Bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid (BAPTA)-acetoxymethyl ester (AM), a rapidly acting calcium chelator, was used to test whether reduced intracellular Ca2+ concentration ([Ca2+]i) plays a role in the inhibitory effects of ryanodine. Our results confirm that ryanodine inhibits the release of Ca2+ from the SR of rabbit SA node pacemaker cells and suggest that reductions of inward Na+/Ca2+ exchange current (INa/Ca) and T-type Ca2+ current (ICa,T) account for the negative chronotropic effect of ryanodine.

    METHODS
Top
Abstract
Introduction
Methods
Results
Discussion
References

Cell isolation and culture. Our method for isolating SA node cells from the hearts of male New Zealand White rabbits (1.0-1.5 kg) has been described in detail (19, 21). The cells were plated on glass coverslips (number 0) in 35-mm plastic dishes that contained a culture medium (19, 21) and were stored in an incubator (95% air-5% CO2) at 37°C.

Measurement of intracellular Ca2+. Cultured SA node cells were incubated with 25 µM indo 1-AM for 10-15 min at room temperature and then washed with Tyrode solution for at least 15 min. This concentration and loading period were adopted to optimize the signal-to-noise ratio for indo 1 fluorescence without excessive buffering of Ca2+i. A Photon Technology International (PTI, South Brunswick, NJ) filter-based detection system was used to record indo 1 fluorescence simultaneously at 405 and 485 nm during epifluorescence illumination at 365 nm. Fluorescence was measured as photons per second, and PTI's FELIX software was used to acquire the fluorescence ratio (F405/F485) and electrophysiological data simultaneously. Fluorescence was measured from a rectangular area roughly the size of the cell under study. The background fluorescence, recorded from a cell-free field of the same size, was subtracted from each of the two signals before the fluorescence ratio was calculated. To minimize photobleaching of indo 1, we exposed the cells to 365-nm light only during the recording period.

Electrophysiological recordings. A model 3900A patch-clamp amplifier (Dagan, Minneapolis, MN) and ruptured-patch or perforated-patch whole cell recordings (19, 21) were used to record ionic currents or spontaneous electrical activity in isolated pacemaker cells after 2 or 3 days in vitro. Cells were superfused with Tyrode solution containing (in mM) 130 NaCl, 5.4 KCl, 1.8 CaCl2, 0.6 MgCl2, 0.6 NaH2PO4, 18 NaHCO3, and 5.5 dextrose, pH adjusted to 7.4 with the addition of 95% O2 or 95% air and 5% CO2. The pipette solution for perforated-patch recordings with nystatin contained impermeant divalent cations to minimize the Donnan potential [in mM: 75 K2SO4, 55 KCl, 7 MgCl2, 10 dextrose, and 10 N-2-hydroxyethylpiperazine-N'-2-ethanesulfonic acid (HEPES)] and was titrated to pH 7.2 with KOH. To isolate Ca2+ currents, the modified Tyrode solution contained the following blockers (in mM): 0.01-0.03 tetrodotoxin, 2 CsCl, 4 4-aminopyridine, and 2 BaCl2, and the pipette solution contained Cs+ instead of K+. Because amphotericin B can achieve a lower access resistance than nystatin, current tail measurements and some Ca2+ current measurements employed amphotericin B in a pipette solution that contained (in mM) 5 NaCl, 125 CsCl, 5 MgATP, 10 dextrose, 10 ethylene glycol-bis(beta -aminoethyl ether)-N,N,N',N'-tetraacetic acid (EGTA), and 10 HEPES and was titrated to pH 7.2 with CsOH. This solution also could be used for ruptured-patch recordings in the same cell. In some experiments, the ruptured-patch technique was used to promote rundown of L-type Ca2+ current (ICa,L) so as to isolate ICa,T. In those measurements, MgATP and HEPES were omitted and the pipette solution contained (in mM) 140 CsCl, 10 NaCl, and 10 dextrose and was titrated to pH 7.2 with CsOH. The calculated corrections for liquid-junction potentials between the modified Tyrode and nystatin or amphotericin B pipette solutions were -2.9 and -5.2 mV, respectively (19, 21). Because these potentials were unchanged by the addition of ryanodine or BAPTA, we did not make such corrections. A stock solution of nystatin [50 mg/ml in dimethyl sulfoxide (DMSO)] or amphotericin B (30 mg/ml in DMSO) was diluted in the appropriate pipette solution and ultrasonicated. The tip of the pipette was filled with antibiotic-free solution and the rest of the pipette with nystatin (300 µg/ml)- or amphotericin B (400 µg/ml)-containing solution. Pipettes were made on a model P80/PC puller (Sutter Instrument, Novato, CA); their resistances ranged from 1 to 5 MOmega . After a pipette-membrane seal had formed (resistance, 10-20 GOmega ), we waited 10-15 min for patch perforation before making the electrophysiological measurements. Series resistance compensation was maximized to minimize the time constant for decay of the capacitive transient.

Solutions. The cell isolation solutions and culture medium have been described (19, 21). The indo 1-AM loading solution was made by adding 25 µg indo 1-AM (Texas Fluorescence Laboratory, Austin, TX), 25 µl DMSO, 45 µl fetal calf serum (GIBCO, Grand Island, NY), and 2.2 µl of 25% (wt/wt) Pluronic F-127 (Sigma Chemical, St. Louis, MO) in DMSO to 1 ml of a HEPES-buffered balanced salt solution (19, 21) that contained 1.8 mM CaCl2. The final concentration of indo 1-AM was 25 µM. Drug-containing solutions were prepared by appropriate dilution of the stock solutions except for caffeine, which was added as a powder directly to the Tyrode solution. BAPTA was loaded into the cells by adding 25 µM BAPTA-AM (Texas Fluorescence Lab) to the Tyrode solution. In each experiment, the isolated pacemaker cells were superfused with Tyrode solution at a rate of 1 ml/min. A control system (model TC-1, Cell Micro Controls, Virginia Beach, VA) was employed to maintain the temperature within ±0.5°C of 34 or 35°C.

Data analysis. Beat rates were calculated from the total period for 10 consecutive action potentials, and pCLAMP 6 software (Axon Instruments, Foster City, CA) was used to measure the characteristics of at least 3 action potentials; then these were averaged. Slopes of the initial and final phases of diastolic depolarization (DD1 and DD2, respectively) were obtained from linear fits (Fig. 1C), and the "takeoff" potential (TP) was approximated by the intersection of linear fits of the action potential upstroke and DD2. Hyperpolarization-activated inward current (If) was measured as the difference between the inward current at the end of 300-ms voltage steps, a duration that approximates diastole, and the instantaneous or "background" inward current (Ibg) at the onset of the step. Ca2+ currents were measured as the difference between the peak of the transient inward current and the current at the end of 300-ms voltage steps, which was assumed to be leakage current. Currents were normalized by cell input capacitance (C), where C = Q/Delta V, Q is the charge (measured as the area subtended by the capacitive current), and the change in voltage (Delta V) is 10 mV. A Chebyshev-Simplex method (pCLAMP 6) was employed to fit the decay of Ca2+i transients by a single exponential and to fit slow inward current tails by a sum of two exponentials. The tail's peak was determined from the exponential fit. Analog data were digitized at 12-bit resolution by a Labmaster DMA board (Axon Instruments) that was controlled by pCLAMP software and then stored on the hard disk of a computer for later analysis. Data are presented as means ± SE. A paired Student's t-test was used for statistical analyses, and differences between means with P < 0.05 were considered significant.


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Fig. 1.   Simultaneous recordings of electrical activity and action potential-induced intracellular Ca2+ (Ca2+i) transients before and after addition of ryanodine. A: action potentials (Vm, top) and indo 1 fluorescence ratio (F405/F485, bottom) under control conditions. B: action potentials (top) and fluorescence ratio (bottom) 10 min after addition of 10 µM ryanodine (same cell as in A). C: superimposed electrical activity before (solid trace) and after (dashed trace) addition of ryanodine. Note reduced slope of final phase of diastolic depolarization (DD2), but not in initial phase (DD1), and depolarization of "takeoff" potential (arrows) after exposure to ryanodine.

    RESULTS
Top
Abstract
Introduction
Methods
Results
Discussion
References

Effect of ryanodine on spontaneous electrical activity and Ca2+i transients. During simultaneous recordings of electrical activity and the indo 1 fluorescence ratio, the addition of 10 µM ryanodine slowed the firing rate and reduced the amplitude of action potential-induced Ca2+i transients. For example, in one pacemaker cell, the beat rate (BR) decreased from 86 to 67 beats/min, the peak-to-peak amplitude of F405/F485 decreased from 0.6 to 0.5, and the time constant for its decay increased from 126 to 176 ms after 10 min (Fig. 1, A and B). The slower firing rate might be explained by the slower DD2, which decreased from 35.1 to 19.5 mV/s (dashed curve, Fig. 1C), and by depolarization of the TP from -51 to -42 mV (arrows, Fig. 1C). The effects of 10 µM ryanodine on the electrical activity of 15 cultured pacemaker cells are summarized in Table 1. Reductions of BR (30 ± 3%), maximum upstroke velocity (dV/dtmax; 12 ± 3%), DD2 (37 ± 3%), and TP (11 ± 2%) were all significant (P < 0.01). Results obtained in 10 freshly isolated pacemaker cells (not shown) were not significantly different. The fact that DD2, but not DD1, was reduced by ryanodine is consistent with the microelectrode recordings of Rubenstein and Lipsius (18, 26) in cat SA node and subsidiary pacemaker tissue and of Rigg and Terrar (24) in guinea pig SA node tissue. However, in those studies, a significant depolarization of the maximum diastolic potential (MDP) and changes in the action potential overshoot (OS) were also seen. In the present study, ryanodine simultaneously reduced the peak-to-peak amplitude of action potential-induced Ca2+i transients by 19 ± 3% (P < 0.01) and increased their time constant for decay by 51 ± 5% (P < 0.01). Some slowing of BR and reduction of the Ca2+i transient could be seen after just 2 min of exposure to ryanodine, and a maximal effect was reached in <8 min. Thus the results described below were obtained after 8-10 min of exposure.

                              
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Table 1.   Effect of ryanodine on electrophysiological characteristics of cultured rabbit sinoatrial node cells

Blockade of SR Ca2+ release by ryanodine. To confirm that the actions of ryanodine were due, in part, to its effects on the SR, we used caffeine to release Ca2+ from the SR and then tested whether ryanodine could block this release. Because caffeine enhances ICa,L in rabbit SA node tissue (27), it was necessary to block this current before the addition of caffeine to eliminate its contribution to the Ca2+i transient. Exposure of pacemaker cells to Ni2+, which inhibits both ICa,L and ICa,T in this preparation (21), rapidly blocked the action potential-induced Ca2+i transients, and Ca2+i fell below the diastolic level (Fig. 2A). Addition of 10 mM caffeine produced a transient increase in Ca2+i, but a second addition had no effect. This indicates that 10 mM caffeine depleted the Ca2+ stores. With Ni2+ and caffeine washout, there was complete recovery of the Ca2+i transients. Pretreatment of another pacemaker cell with 10 µM ryanodine prevented the caffeine-induced Ca2+i transient, and pacemaker activity became arrhythmic with Ni2+ and caffeine washout (Fig. 2B). Similar results were obtained in another 11 pacemaker cells.


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Fig. 2.   Ryanodine blockade of caffeine-induced release of Ca2+ from sarcoplasmic reticulum (SR). A: blockade of action potential-induced Ca2+i transients by 5 mM Ni2+ followed by caffeine (10 mM)-induced release of SR Ca2+. A second addition of caffeine failed to elicit Ca2+ release. B: pretreatment of another cell with 10 µM ryanodine abolished transient response to caffeine. Note that recordings were interrupted for 1-2 min after addition and washout of Ni2+.

Effect of ryanodine on hyperpolarization-activated and background inward currents. Because the slowing of spontaneous firing induced by ryanodine coincided with a slower DD2 (Fig. 1C), we tested the hypothesis that exposure to ryanodine leads to a decrement of If and Ibg, inward currents that might contribute to this phase of the pacemaker potential. To activate these currents, we applied 300-ms voltage steps from a holding potential of -50 mV to potentials between -50 and -100 mV. The records before and 10 min after exposure to 10 µM ryanodine show that ryanodine did not alter If or Ibg (Fig. 3A). In fact, no effect was seen after 2, 5, 10, or 15 min of exposure to ryanodine. In eight pacemaker cells, the current-voltage (I-V) relationships for If and Ibg before and 10 min after addition of ryanodine were not significantly different (Fig. 3B).


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Fig. 3.   Effect of ryanodine on hyperpolarization-activated (If) and background (Ibg) inward currents. A: hyperpolarizing voltage steps (300-ms duration) from a holding potential (HP) of -50 mV to potentials between -50 and -100 mV; control (top) and 10 min after addition of 10 µM ryanodine (bottom). B: mean current-voltage (I-V) relationships for If and Ibg (n = 8) before and after addition of 10 µM ryanodine.

Effect of ryanodine on T- and L-type Ca2+ currents. Because the slowing of spontaneous firing induced by ryanodine coincided with a slower DD2 and depolarization of the TP (Fig. 1C), we tested the hypothesis that exposure to ryanodine leads to a decrement of ICa,T and ICa,L, inward currents likely to contribute to these two phases of the electrical activity (8, 13). As demonstrated previously in SA node pacemaker cells, ICa,L and ICa,T can be separated by the holding potential (8, 13). Both currents could be elicited from a holding potential of -80 mV, whereas only ICa,L could be activated from a holding potential of -40 mV. In the present study, total Ca2+ current (ICa = ICa,L + ICa,T) was reduced after just 2 min of exposure to 10 µM ryanodine; however, as recorded in ventricular myocytes (1, 20, 23) and freshly isolated rod-shaped rabbit SA node cells (28), the amplitude of ICa,L was not changed significantly. Longer exposures (up to 15 min) also did not alter ICa,L significantly, ruling out "rundown" of ICa,L as the cause of the decline of ICa. Figure 4A illustrates the effects of ryanodine on ICa and ICa,L (traces labeled R) in a representative pacemaker cell. Figure 4B shows the mean I-V relationships for eight pacemaker cells before and 10 min after addition of 10 µM ryanodine. The perforated-patch technique (with nystatin) was employed to minimize rundown of ICa,L. Ryanodine reduced ICa significantly at -30, -20, and -10 mV (P < 0.05). In contrast, it had no significant effect on ICa,L at any potential. Significant changes in ICa were observed at -30, -20, -10, 0, and 10 mV (P < 0.05) in another 10 cells when the patch pipette contained amphotericin B to reduce the series resistance (data not shown). The absence of an effect of ryanodine on the amplitude of ICa,L suggests that the attenuation of ICa is due to a reduction of ICa,T. This could explain the reductions of both DD2 and TP, because ICa,T is activated at those potentials (8, 13).


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Fig. 4.   Effect of ryanodine on Ca2+ currents (ICa). A: ICa elicited by depolarizing voltage steps to potentials indicated from HP of -80 mV (left) and -40 mV [L-type Ca2+ current (ICa,L), right], before (C) and 10 min after (R) addition of 10 µM ryanodine. B: mean I-V relationships for 8 cells in absence and presence of 10 µM ryanodine (after 10 min). For ICa (top, HP = -80 mV), mean values at -30, -20, and -10 mV are significantly different. For ICa,L (bottom, HP = -40 mV), no changes are significantly different.

Further evidence that ryanodine reduces ICa,T is presented in Fig. 5. Because we could not find a concentration of Ni2+, Cd2+, or La3+ that would block ICa,L completely without also reducing ICa,T and because the dihydropyridines are not selective at diastolic potentials (4), we promoted rundown of ICa,L by using the ruptured-patch technique and omitting ATP and HEPES from the pipette solution (see METHODS for details). After ICa,L had run down almost completely (Fig. 5A), exposing the pacemaker cells to 10 µM ryanodine led to a small reduction of ICa (Fig. 5B) that could be attributed almost exclusively to ICa,T. The mean I-V relationships of five cells exposed to such rundown conditions are shown in Fig. 5C. The differences at -30, -20, -10, 0, and 10 mV were all significant (P < 0.05).


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Fig. 5.   Effect of ryanodine on T-type Ca2+ current. A: ICa,L elicited from an HP of -40 mV after rundown. B: total Ca2+ current elicited by depolarizing voltage steps from an HP of -80 mV to potentials indicated before (left) and 10 min after addition of 10 µM ryanodine (right). C: mean I-V relationships for ICa (HP = -80) in absence and presence of 10 µM ryanodine (n = 5). Changes at -30, -20, -10, 0, and 10 mV are all significant (P < 0.05).

Effect of BAPTA-AM on spontaneous electrical activity and Ca2+i transients. To test the hypothesis that a reduction of the amplitude of Ca2+i transients was responsible for ryanodine's slowing of DD2 and BR and depolarization of the TP, we exposed 14 pacemaker cells to BAPTA-AM, a rapidly acting Ca2+ chelator. During simultaneous recordings of electrical activity and the indo 1 fluorescence ratio, action potential-induced Ca2+i transients were eliminated 3-5 min after the addition of 25 µM BAPTA-AM, whereas the spontaneous electrical activity continued (Fig. 6). BAPTA, like ryanodine, had no effect on DD1, yet it slowed the DD2 and BR, reduced the dV/dtmax, and depolarized the TP (P < 0.01; Table 2). However, unlike ryanodine, BAPTA prolonged the duration of the action potential measured at -20 mV (Dur; P < 0.05) and depolarized the MDP (P < 0.01). These results suggest that the effects of ryanodine on DD2, BR, dV/dtmax, and TP might arise, in part, from the reduction of [Ca2+]i that accompanies ryanodine's inhibition of SR Ca2+ release. The additional effects of BAPTA on the Dur and MDP might be explained by the likelihood that BAPTA can reduce [Ca2+] in the cytoplasm to a greater degree than can ryanodine (see DISCUSSION).


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Fig. 6.   Simultaneous recordings of electrical activity and action potential-induced Ca2+i transients before and after addition of 1,2-bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid (BAPTA)-acetoxymethyl ester (AM). A: Vm (top) and F405/F485 (bottom) under control conditions. B: Vm and F405/F485 10 min after addition of 25 µM BAPTA-AM (same cell as in A). Note that action potential-induced Ca2+i transients were blocked completely.

                              
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Table 2.   Effect of BAPTA-AM on electrophysiological characteristics of cultured rabbit sinoatrial node cells

Effect of ryanodine on Ca2+ currents in BAPTA-AM-loaded cells. To determine whether the reduction of ICa was due to changes in [Ca2+]i or to ryanodine itself, we first reduced [Ca2+]i with BAPTA and then added ryanodine. After the pacemaker cells had been exposed to 25 µM BAPTA-AM for 10 min, the amplitudes of ICa and ICa,L were unchanged (Fig. 7). This was confirmed by the mean I-V relationships for five pacemaker cells that were not significantly different at any potential (Fig. 8A). Despite the fact that there was no significant effect on the amplitudes of ICa and ICa,L, BAPTA did slow inactivation of the two currents (Fig. 7), as would be expected for a reduction of Ca2+-induced inactivation (22). With BAPTA-AM still present, 10 µM ryanodine reduced ICa after only 2 min, whereas ICa,L was not changed, just as we had seen in the absence of BAPTA (Fig. 7). After the pacemaker cells had been exposed to ryanodine for 10 min, the reduction of ICa was significant at -30, -20, and -10 mV (P < 0.05); however, there was no significant effect on ICa,L (Fig. 8B). These results suggest that ryanodine's reduction of ICa might be due to a direct effect of ryanodine on T-type Ca2+ channels, independent of changes in [Ca2+]i.


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Fig. 7.   Effect of ryanodine on Ca2+ currents in presence of BAPTA. Ca2+ currents were elicited by depolarizing voltage steps from HP of -80 mV (ICa) and -40 mV (ICa,L) under control conditions (left), 8 min after addition of 25 µM BAPTA-AM (middle), and 10 min after addition of 10 µM ryanodine (right).


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Fig. 8.   A: mean I-V relationships for ICa (HP = -80 mV) and ICa,L (HP = -40 mV) in absence (Control) or presence of 25 µM BAPTA-AM (n = 5). Mean values for control and BAPTA are not significantly different at any potential. B: mean I-V relationships for ICa and ICa,L in presence of 25 µM BAPTA-AM and in absence (BAPTA) or presence of 10 µM ryanodine (n = 5). Mean values for ICa at -30, -20, and -10 mV are significantly different (P < 0.05). Perforated patches were obtained with amphotericin B.

Effects of BAPTA and ryanodine on slow inward current tails. This set of experiments was designed to test the hypothesis that ryanodine also reduces inward INa/Ca in SA node pacemaker cells. By decreasing the amplitude of Ca2+i transients, ryanodine would be expected to diminish the extrusion of Ca2+ via the Na+/Ca2+ exchanger and thereby reduce the net influx of Na+, i.e., INa/Ca. After repolarization of the membrane potential after a 5-ms test pulse to +20 mV, a slow decay of inward current could be seen (Fig. 9). The amplitude of this slow inward current tail seemed to depend on the amplitude of ICa,L elicited during the test pulse, and the tail could be eliminated if ICa,L was completely inactivated (at a holding potential of 0 mV). Although this slow decay could be interpreted as an ICa,T tail (4), this is highly unlikely, because ICa,T would have been completely inactivated at the employed holding potentials of -40, -20, and 0 mV (8, 13). Addition of 25 µM BAPTA-AM blocked the tails completely in seven SA node pacemaker cells; moreover, BAPTA slowed inactivation but did not alter the amplitude of ICa,L (Fig. 9A). In nine pacemaker cells, exposure to 10 µM ryanodine also blocked the slow tails and slowed the inactivation of ICa,L (Fig. 9B). When the holding potential was -40 mV, ryanodine reduced the peak of the tail from -173 ± 22 to -59 ± 13 pA (P < 0.01) and decreased the time constant of its decay from 13 ± 3 to 7 ± 1 ms (P < 0.05).


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Fig. 9.   Effect of BAPTA or ryanodine on slow inward current tails. A: current tails elicited by a 5-ms test pulse to +20 mV, followed by repolarization to -80 µV, before (Control) or 10 min after addition of 25 µM BAPTA-AM; prepulses to -40, -20, and 0 mV were 1 s in duration. B: current tails obtained with same protocol as in A before (Control) or 10 min after addition of 10 µM ryanodine.

Effects of lower concentrations of ryanodine. To identify the contribution of each process, a reduction of ICa,T and blockade of SR Ca2+ release, to the negative chronotropic effect of ryanodine, we used lower concentrations of ryanodine and looked for a dose-dependent difference in its effects. Unfortunately, we could not find such a difference. At concentrations of 5 and 2 µM (6 and 9 cells, respectively), ryanodine continued to slow pacemaker activity, reduce ICa,T, partially block inward current tails, and block caffeine-induced Ca2+i transients. At a concentration of 1 µM, ryanodine's effects on ICa,T and SR Ca2+ release still could not be separated. Ryanodine reduced ICa,T in three of four cells, and it blocked caffeine-induced Ca2+i transients in four of four cells. We considered 1 µM ryanodine to be the "threshold" dose, because this concentration slowed pacemaker activity in only two of five cells.

    DISCUSSION
Top
Abstract
Introduction
Methods
Results
Discussion
References

Previously, we showed that ryanodine reduces the amplitude of action potential-induced Ca2+i transients and slows the firing of cultured SA node pacemaker cells (17). The latter effect could be due to changes in any of the currents that contribute to pacemaker activity. However, the present study was designed to test the hypothesis that ryanodine's negative chronotropic effect is due to a reduction of inward currents that contribute to pacemaker activity and can be modulated by Ca2+i. Such currents include the following: 1) If, which may (12) or may not (31) depend on [Ca2+]i; 2) time-independent Ibg or "sustained" inward currents carried by Na+ (10, 14); 3) INa/Ca, which depends on both the Na+ and Ca2+ electrochemical gradients (11, 32); and 4) ICa,T and ICa,L, which also depend on the Ca2+ gradient (5, 8, 13).

With the use of 10 µM ryanodine, a concentration sufficient to block SR Ca2+ release (Fig. 2), we found no significant effect on either If or Ibg (Fig. 3). In contrast, 10 µM ryanodine did reduce If significantly in freshly isolated rod-shaped rabbit SA node cells (28). We have no explanation for this discrepancy. In our cultured SA node pacemaker cells, 10 µM ryanodine reduced ICa significantly at -30, -20, and -10 mV (Fig. 4B). Even though they were not statistically significant, reductions of ICa were also seen at -50 and -40 mV (Fig. 4A), potentials at which ICa,T is activated (8, 13) and the takeoff potential is seen (Fig. 1C, Table 1). In rabbit SA node cells, the role of ICa,T is to accelerate DD2 and maintain the action potential threshold at more negative potentials (5, 13). For example, blockade of ICa,T by 40 µM Ni2+ prolonged DD2 without changing DD1 (13), just as we have seen in our own experiments with ryanodine (Fig. 1C). Nevertheless, other mechanisms might also play a role, because ryanodine reduced but did not block ICa,T (Fig. 4). With the use of two different recording procedures, the perforated-patch technique (with nystatin in 8 cells and amphotericin B in 10 cells) and the ruptured-patch technique (to promote rundown of ICa,L in 5 cells), we observed a consistent decline in the amplitude of ICa after addition of ryanodine. This decline cannot be explained by rundown of ICa,L, because ICa,L was recorded about the same time as ICa and was unaffected by ryanodine (Figs. 4, A and B). Given that ICa = ICa,L ICa,T, these results suggest that ryanodine slows pacemaker activity, in part, by reducing ICa,T. The rundown experiment (Fig. 5) provides additional support for this hypothesis, because, in the virtual absence of ICa,L, ICa was reduced significantly by ryanodine.

Studies of ventricular myocytes (1, 20, 23) and SA node pacemaker cells (28) suggest that ryanodine, at concentrations between 1 and 10 µM, does not act directly on L-type Ca2+ channels; instead, its effects are mediated by changes in [Ca2+]i. In fact, privileged cross signaling between ryanodine receptors and L-type Ca2+ channels has been suggested to occur in adult rat ventricular myocytes (3, 29). Previously, we showed that ICa,L inactivation is dependent on [Ca2+]i in SA node pacemaker cells (22), and those observations are supported by the present results in which BAPTA slowed the inactivation of ICa,L (Figs. 7 and 9A). However, little slowing of ICa,L inactivation was observed after the addition of ryanodine (Fig. 4A), suggesting that its reduction of [Ca2+]i was small. This was confirmed by the modest decrease (19%) in the amplitude of action potential-induced Ca2+i transients after the addition of ryanodine (Fig. 1B). A similar discrepancy can be seen when one compares the effects of ryanodine and BAPTA on the MDP and Dur of the action potential in Tables 1 and 2. Ryanodine (10 µM) had no significant effect, whereas BAPTA depolarized the MDP and increased the Dur significantly. Interestingly, in freshly isolated rod-shaped rabbit SA node cells, 1 µM ryanodine not only slowed pacemaker activity but also increased the OS and Dur significantly; however, it had no effect on the MDP (28). In contrast, 1 or 2 µM ryanodine depolarized the MDP and changed the OS significantly in cat subsidiary (26) and guinea pig SA node (24) pacemaker cells. Such differences might be explained by the relative changes in [Ca2+]i produced by ryanodine or by the relative abundance of SR in cat, guinea pig, and rabbit pacemaker cells. In the present study, it is possible that ryanodine had a direct effect on ICa,T, independent of the changes in [Ca2+]i, considering that ryanodine reduced ICa regardless of whether BAPTA was present (Figs. 7 and 8B) or not (Fig. 4B). Although BAPTA blocked the Ca2+i transients (Fig. 6) and slowed the inactivation of ICa,L (Figs. 7 and 9), it had no effect on the amplitude of either ICa or ICa,L (Figs. 7 and 8A). Therefore, it is possible that BAPTA failed to reach the T-type Ca2+ channels. Thus we cannot rule out the possibility that ryanodine's reduction of ICa,T was due to its attenuation of the Ca2+i transients (Fig. 1B). In fact, a reduction of [Ca2+]i has been shown to decrease ICa,T in canine ventricular and Purkinje cells (30).

In our cultured SA node pacemaker cells, we observed a relatively slow inward current tail that consistently followed depolarizing voltage steps that activated ICa,L (see Controls, Fig. 9). Similar current tails, recorded in atrial myocytes and pacemaker cells, have been attributed to the Na+/Ca2+ exchanger (2, 6, 9, 32). BAPTA's blockade of such tails (Fig. 9A) is consistent with previous results, in which cat latent pacemaker cells were dialyzed with EGTA (32), and supports the hypothesis that this current depends on [Ca2+]i. In agreement with some but not all previous studies of rabbit atrial myocytes (6, 9) and cat latent pacemaker cells (32), ryanodine inhibited slow inward current tails in our rabbit SA node pacemaker cells (Fig. 9B). Additional results in cat latent pacemaker cells (32) demonstrated that INa/Ca can contribute significantly to the generation of diastolic depolarization, particularly DD2. Nevertheless, the role of INa/Ca in rabbit SA node pacemaker activity remains to be clarified. Although ryanodine (10 µM) had just a small effect on the amplitude of action potential-induced Ca2+i transients that were measured by indo 1 in the cytoplasm (Fig. 1), the slow inward current tails were abolished by the same concentration of ryanodine (Fig. 9B). This suggests that the whole cell spatially averaged [Ca2+]i, measured by indo 1, is an unreliable indicator of the Ca2+ that is released from the SR and is most effective in activating Na+/Ca2+ exchange (16).

In summary, ryanodine's negative chronotropic effect is derived, in part, from a reduction of ICa,T. This reduction can be explained by the attenuation of action potential-induced Ca2+i transients or by a direct effect of ryanodine on T-type Ca2+ channels. Although it is not known whether INa/Ca contributes to the diastolic depolarization of rabbit SA node cells, it is known to contribute to DD2 in cat latent pacemaker cells (32), and it generates inward current tails (2, 6, 9, 32) much like those we recorded (Fig. 9). Thus, on the basis primarily of theory and results in other preparations, it is possible that, after inhibition of SR Ca2+ release by ryanodine, the smaller action potential-induced Ca2+i transients could have reduced INa/Ca and, therefore, the beat rate.

    ACKNOWLEDGEMENTS

We thank Theresa Redington for preparation of the SA node pacemaker cells, Robert Powell for assistance in preparing the figures, Chris Bell for assistance in the fluorescence measurements, and Drs. John Fowler, Sandor Györke, and Alan Neely for helpful comments on the manuscript.

    FOOTNOTES

This work was supported in part by National Heart, Lung, and Blood Institute Grant HL-48836 and by the Texas Advanced Research Program Grant 010674-048.

This work was in partial fulfillment of the requirements for a PhD in physiology at Texas Tech University Health Sciences Center (J. Li).

Address reprint requests to R. D. Nathan.

Received 25 October 1996; accepted in final form 8 July 1997.

    REFERENCES
Top
Abstract
Introduction
Methods
Results
Discussion
References

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AJP Heart Circ Physiol 273(5):H2481-H2489
0363-6135/97 $5.00 Copyright © 1997 the American Physiological Society



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