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Essential role of diastolic oscillatory potentials in adrenergic control of guinea pig sino-atrial node discharge
Journal of Biomedical Science volume 16, Article number: 101 (2009)
The diastolic oscillatory after-potential Vos and pre-potential ThVos play an essential role in the pacemaker mechanism of sino-atrial node (SAN). The aim of this study was to investigate whether these oscillatory potentials are also involved in adrenergic control of SAN discharge.
Vos and ThVos were visualized by superfusing guinea pig SAN in high [K+]o. The actions of adrenergic agonists on oscillatory potentials were studied by means of a microelectrode technique. Statistical significance was determined by means of Student's paired t-test.
In non-spontaneous SAN, norepinephrine (NE) decreased the resting potential into a voltage range ("oscillatory zone") where increasingly larger ThVos appeared and initiated spontaneous discharge. In slowly discharging SAN, NE gradually increased the rate by increasing the amplitude and slope of earlier-occurring ThVos and of Vos until these oscillations fused with initial diastolic depolarization (DD1). In the presence of NE, sudden fast rhythms were initiated by large Vos that entered a more negative oscillatory zone and initiated a large ThVos. Recovery from NE exposure involved the converse changes. The β-adrenergic agonist isoproterenol had similar actions. Increasing calcium load by decreasing high [K+]o, by fast drive or by recovery in Tyrode solution led to growth of Vos and ThVos which abruptly fused when a fast sudden rhythm was induced. Low [Ca2+]o antagonized the adrenergic actions. Cesium (a blocker of If) induced spontaneous discharge in quiescent SAN through ThVos. In spontaneous SAN, Cs+increased Vos and ThVos, thereby increasing the rate. Cs+ did not hinder the positive chronotropic action of NE. Barium increased the rate, as Cs+ did.
Adrenergic agonists: (i) initiate SAN discharge by decreasing the resting potential and inducing ThVos; (ii) gradually accelerate SAN rate by predominantly increasing size and slope of earlier and more negative ThVos; (iii) can induce sudden fast rhythms through the abrupt fusion of large Vos with large ThVos; (iv) increase Vos and ThVosby increasing cellular calcium; and (v) do not modify the oscillatory potentials by means of the hyperpolarization-activated current If. The results provide evidence for novel mechanisms by which the SAN dominant pacemaker activity is initiated and enhanced by adrenergic agonists.
The mechanisms by which adrenergic agonists increase the rate of the sino-atrial node (SAN) are not agreed upon [1–3]. In part, this is the result of the disagreement about the SAN dominant pacemaker mechanism [see [4, 5]], since adrenergic neuromediators would be expected to change SAN rate by acting on dominant pacemakers.
Adrenergic neuromediators affect several voltage- and time-dependent currents purported to be involved in SAN dominant pacemaker mechanism, including the calcium current ICaL [6–8], the delayed rectifier current IK [1, 9, 10] and the hyperpolarization-activated current If .
In addition, the Na+-Ca2+ exchange current (INa-Ca) contributes to the pacemaker activity in the absence and presence of adrenergic agonists [11, 12]. Stimulation of β-adrenergic receptors increases ICa , the Ca2+ transient [8, 13] and the uptake and release of Ca2+ by the sarcoplasmic reticulum (SR) [3, 12]. A larger Ca2+ release during late diastole increases INa-Ca and therefore the rate of discharge [8, 11, 14].
This complex state of affairs is complicated by the fact that (in addition to diastolic depolarization, DD) two oscillatory potentials (the after-potential Vos and the pre-potential ThVos) are obligatory components of SAN dominant pacemaker mechanism [15–18]. In Tyrode solution, as soon as the maximum diastolic potential (MDP) of SAN dominant pacemakers is reached, the membrane potential turns around into a DD whose slope is similar to that of the preceding final phase 3 repolarization. This U-shaped DD merges smoothly into the slow upstroke of the action potential (AP).
When [K+]o is suitably increased, all APs of SAN display a slow upstroke, a less negative MDP and a U-shaped DD [15–19], as dominant pacemakers do in Tyrode solution. On further increase of high [K+]o, the threshold for the upstroke is missed and the oscillatory potentials Vos and ThVos become unmasked. Vos is obligatorily superimposed on the initial diastolic depolarization (DD1) whereas ThVos appears gradually later when the late DD (DD2) enters a less negative voltage range ("oscillatory zone"). With sufficiently high [K+]o, only a small DD is left and quiescence follows . Quiescence is due to the fact that high [K+]o decreases the oscillatory potentials by decreasing intracellular calcium through an enhanced extrusion of calcium by the Na+-Ca2+ exchange (see 17) and also by decreasing ICa . The converse changes occur when high [K+]o is decreased to normal value.
Our aim was to test the hypothesis that adrenergic agonists increase the SAN rate also by modifying the oscillatory potentials. This hypothesis is based on the fact that, on the one hand, Vos and ThVos are increased by a greater Ca2+ loading [15–19] and, on the other hand, adrenergic agonists increase cellular Ca2+ [6, 13, 21].
The results obtained show that adrenergic agonists initiate spontaneous discharge and increase SAN rate (gradually or suddenly) by modifying in different ways Vos and ThVos as well as the resting potential and DD.
The experiments conform to the principles of national and international ethical guidelines. The experimental protocols were approved by the local Animal Care and Use Committee.
The Methods have been reported in detail [15–18]. In brief outline, eighteen Hartley adult guinea pigs of either sex (weighing 610 ± 59 gr) were euthanized with sodium pentobarbital (60 mg/kg, intraperitoneally). Once the respiration had stopped, the heart was rapidly excised and placed in a Petri dish filled with oxygenated Tyrode solution.
The sino-atrial node was separated from the surrounding red-brown atrial tissue. The SAN was superfused at 37°C with oxygenated (95% O2 and 5% CO2) Tyrode solution of the following composition (mM): NaCl 129, KCl 4, CaCl2 2.7, NaHCO3 20, NaH2PO4 0.45, MgCl2 1.05 and glucose 5.5. Membrane potentials were recorded by means of glass microelectrodes filled with 3 M KCl and coupled to a Dagan probe and to a Dagan model 8500 operational amplifier. Contractile force was recorded by means of a force transducer (Grass Model FTO3C) connected to a Grass Model 7D Polygraph. The traces were displayed on a Tektronix model 5111 storage oscilloscope and recorded on paper on a 3-channel chart recorder (Gould Brush 2400).
To analyze the characteristics of Vos (also referred to in the literature as oscillatory afterpotential or delayed afterdepolarization) and of ThVos (the oscillatory potential leading to the threshold for the upstroke ), [K+]o was increased by mixing the Tyrode solution with a solution containing 40 mM KCl, but otherwise identical with Tyrode solution and gassed with the same mixture. The flow of Tyrode solution was kept constant (Gilson pump, model PP-4-A) and the flow of the K+-rich solution was changed by means of a peristaltic pump (LKB, 12000 Varioperpex). The [K+]o of the final admixture was calculated by means of an equation, as detailed previously [15–18]. The effects of a higher [K+]o were quickly established (<5 min): once a new steady-state was attained, tests were carried out as warranted. The use of the guinea-pig isolated SAN permitted to abolish the electrotonic interference from atrial muscle, since the SAN is made of sinus cells throughout its thickness .
Exposure to suitably high [K+]o made the SAN electrically more homogeneous, since (as a consequence of depolarization) the APs assumed a dominant configuration (smooth transition from U-shaped DD into a slow upstroke and smaller APs). Eventually, high [K+]o permitted the separation of Vos, ThVos and DD [15–18]. That the cells studied in high [K+]o were pacemaker cells is shown by the persistence of their DD during recovery in Tyrode solution. Thus, the cells studied were pacemaker cells with dominant characteristics. Secondary pacemakers have a more negative diastolic potential, abrupt transition between diastolic potential and upstroke, much larger AP, less steep DD and no ThVos, since the more negative diastolic potential is negative to the oscillatory zone [e.g., ].
The abbreviations Vos and ThVos are used for both singular and plural. The early diastolic depolarization is referred to as DD1 and the late diastolic depolarization as DD2. The presence and amplitude of Vos was identified by its peak during DD1. The maximum diastolic potential (MDP) and the resting potential are said to decrease when becoming less negative. When in control the SAN was quiescent in high [K+]o, the characteristics of AP, Vos and ThVos were measured just before stoppage in order to determine their modifications by the subsequent interventions.
Norepinephrine bitartrate (NE), isoproterenol hydrochloride, cesium chloride and barium chloride (Sigma) were added to the Tyrode solution and the final concentration in the bath was calculated by taking into account the flow of high [K+]o solution. The results of the tests performed (n) are expressed as means ± standard error of the mean (SEM). Student's paired t-test was used and a P value < 0.05 was considered significant (indicated in text and figures by an asterisk, *).
Initiation of spontaneous discharge by norepinephrine
In Fig. 1, the SAN was quiescent in high [K+]o (panel a) and NE decreased the resting potential and made ThVos appear (first rightward oblique arrow) that initiated an AP (panel b). The AP was followed by a Vos (leftward oblique arrow). The dash line emphasizes the transition between the peak of Vos and the subsequent DD. ThVos appeared progressively sooner (subsequent rightward oblique arrows) and at more negative potentials. The traces labeled with an empty and a filled star were superimposed in inset 1 and show that NE made ThVos (shaded area) begin early in diastole and at a more negative value (negative shift of the oscillatory zone). By occurring earlier in diastole, ThVos gradually increased the rate. At the same time, Vos size increased (short bars). After the AP labeled by a filled star, ThVos and Vos became fused (see also inset 1).
Subsequent changes are shown at greater time base in panels c-g. Vos increased progressively, as emphasized by the shaded areas (panels c-f). After the peak of Vos, the depolarizing phase (presumably of ThVos) became steeper (dash lines), until in panel g only a U-shaped DD was present. In inset 2, the superimposed c-g traces show that NE shortened the AP (arrow), increased the MDP (from trace c to g), and steepened the slope of Vos as well as of ThVos. As shown in panel h (recorded simultaneously with panel g), much larger APs discharged at 150 min-1.
During the recovery from NE exposure (inset 3), the converse changes occurred. As shown by the shaded areas in the enlarged top trace (rightward oblique arrow), the slowing of discharge initially was due to a gradually less steep slope during later diastole. Eventually, ThVos missed the threshold for the upstroke (asterisk), as emphasized by its superimposition on the previous AP (indicated by the horizontal arrow). This indeed shows that the peak of Vos was followed by the depolarizing slope of ThVos.
The traces labeled with dot, circle, rhombus and square show that, during the recovery from NE exposure, the amplitude of Vos gradually decreased (shaded areas), the early ThVos decreased in amplitude and the subsequent ThVos attained the threshold gradually later. The superimposed traces (displaced vertically for clarity) emphasize the decrease in Vos and ThVos amplitude, the gradual slowing being due to the later appearance of ThVos during DD2. In the bottom trace, the last AP was followed by ThVos, which increased in amplitude, failed to attain the threshold and progressively declined to the resting potential ("diamond pattern").
Thus, ThVos was responsible solely for the initiation of spontaneous discharge and predominantly for the gradual increase in rate. The earlier, larger and more negative ThVos eventually fused with the larger Vos into the U-shaped DD.
In 12.3 ± 1.0 mM [K+]o, SAN was quiescent in n = 10 and slowly driven in n = 3 at an average 9 beats min-1. Norepinephrine (415 ± 77 nM) decreased the resting or diastolic potential by 2.7 ± 0.28* mV by the time it consistently induced ThVos, thereby initiating spontaneous discharge. As shown in Fig. 1, inset 4 (means and SEM), NE increased the rate from 2.08 to 164 ± 15* min-1, the action potential amplitude (APa) 11%*, diastolic depolarization amplitude (DDa) 43%, Vos amplitude (Vosa) 112%*, Vos depolarizing slope (Vosds) 55%*, ThVos depolarizing slope (ThVosds) 219%* and force 1800%*.
Increase in spontaneous rate of discharge by norepinephrine
Since the SAN is generally active, [K+]o, was increased to a level that permitted at the same time spontaneous discharge and the visualization of both Vos and ThVos. In this way, it was possible to verify how NE progressively modified the oscillatory potentials while increasing the rate.
In Fig. 2A, in control (panel a), the SAN was discharging at 30.7 beats min-1 and the AP was followed by a Vos (leftward oblique arrow), whose peak is indicated by the short bar. In turn, Vos was followed by a sub-threshold ThVos (rightward oblique arrow). The depolarizing phase of the subsequent ThVos was faster and larger, and attained the threshold for the upstroke (end of shaded area). NE increased Vos amplitude (upward shift of Vos peak, marked by short bars), caused ThVos to appear much earlier during DD2 (rightward oblique arrows in panels b, c and d), and increased the slope of ThVos depolarizing phase (dash lines, panels b-d).
As a consequence of the larger Vos and of the earlier onset and steeper slope of ThVos (small shaded area in panel c), the threshold for the upstroke was attained much sooner. In panels e-g, the inflection was no longer clearly visible as Vos and ThVos were fused into the U-shaped DD. The rate increased to 166 min-1 (panel g, 440% of control).
In inset 1, the superimposed traces show that NE increased the rate (leftward oblique arrow) by gradually increasing the slope and amplitude of earlier ThVos (dots) and of Vos (rectangle). During partial recovery (panel h), slowing of the rate was due to the first ThVos missing the threshold and to the decrease toward control value of depolarizing slope of the second ThVos (dash line). The depolarizing phase of Vos was also slower, as shown by the superimposition of the trace labeled with empty star in panel g on the recovery trace in panel h.
In n = 14, the SAN was spontaneously active in 15.1 ± 1.8 mM [K+]o. As shown in inset 2, NE (469 ± 55 nM) changed the rate by 124%*, APa 15%*, DDa 30%, Vosa 54%*, Vosds 64%*, ThVosds 120%* and force 974%*. Thus, NE increases the rate of spontaneously discharging SAN by shifting the diastolic potential in a positive direction, and by increasing the amplitude and slope of already present Vos and ThVos. Also, NE increased the amplitude and decreased the duration of AP (-13.3%*), and increased force, as it does in Tyrode solution.
Sudden initiation of fast discharge by adrenergic activation
In vivo, sympathetic nerve stimulation induces a gradual increase in the rate of SAN and (in complete atrio-ventricular block) of the idioventricular rhythm originating in Purkinje fibers. However, adrenergic activation may also induce a sudden marked acceleration of the idioventricular rhythm .
Adrenergic agonists could suddenly induce a fast rhythm also in SAN superfused in vitro and therefore allow the study of the underlying mechanisms. In Fig. 3, the non-spontaneous SAN was driven in high [K+]o at 6 min-1 and the AP was followed by a Vos, but no ThVos were present (panel a). In panel b, adding the β-adrenergic agonist isoproterenol decreased the diastolic potential and increased the amplitude of Vos (short bars). The third driven AP initiated a sudden rhythm at 240 min-1. The drive was stopped and the fast rhythm continued as long as isoproterenol was superfused. During recovery in high [K+]o (panel d), the brief slowing and sudden stoppage was due to the late DD1 slope becoming slower and suddenly missing the threshold. Damped oscillations followed.
In Fig. 3e, in control, the driven AP was followed by Vos whose peak barely reached the resting potential. The drive was stopped and isoproterenol administration decreased the resting membrane by ~7 mV. ThVos appeared (arrow) which elicited an AP that initiated a sudden fast rhythm (254 min-1 in panel g). In panel h, during the recovery from isoproterenol exposure, the driven AP was again followed by large damped oscillations.
In inset 1, n = 6, in 12.6 ± 1.4 mM [K+]o, the SAN was not spontaneously active and was either driven at 6 min-1 or left quiescent. Isoproterenol (114 ± 53 nM) decreased the resting or diastolic potential by 4.4 ± 0.9* mV and increased the spontaneous rate from zero to 127 ± 40* min-1, APa 22%*, DDa 59%*, Vosa 78%*, Vosds 209%* and force 313%*. The effects were similar to those induced by NE, thus indicating that they are related to stimulation of β receptors.
In n = 9, in 10.8 ± 0.5 mM [K+]o, the SAN was quiescent. NE or isoproterenol (mean value 520 ± 0.13 nM) induced a sudden fast rhythm (214 ± 14* min-1) either with the first AP or after a few accelerating APs. In n = 22, in 13.3 ± 1.5 mM [K+]o, the SAN was either quiescent or spontaneously active (mean rate 17 beats min-1). NE or isoproterenol (mean value 459 ± 170 nM) induced or increased ThVos that resulted in a gradual acceleration to 105 ± 9* min-1. In 6/22, the gradual increase led to a sudden acceleration to 190 ± 17 min-1 (* with respect to the gradually increased rhythm).
Role of Vos and ThVos in sudden fast rhythms on decreasing high [K+]o
High [K+]o was decreased (to increase [Ca2+]i) in order to investigate whether and how Vos and ThVos induce a sudden fast rhythm, as adrenergic agonists do.
In Fig. 4A, [K+]o was decreased while the SAN was driven at 6 min-1. The resting potential became more negative and Vos (whose peak is marked by short bars) gradually increased until the peak of Vos actually overshot the resting potential. Small ThVos appeared, but it was the last driven AP that initiated a sudden fast rhythm (146 min-1). During recovery, when the threshold was missed, diastolic oscillations were unmasked (not shown).
In Fig. 4B (same SAN), again [K+]o was decreased while driving the SAN at 6 min-1 As in Fig. 4A, the APs were followed by Vos which gradually increased in size (see traces labeled by a dot and a rhombus without and within inset 1). However, this time larger ThVos (downward arrows) elicited an AP that initiated a sudden fast rhythm ahead of the next driven AP (horizontal arrow). As shown in inset 2, during the recovery in higher [K+]o, the U-shaped DD began to miss the threshold (circle), thereby unmasking large diastolic oscillations. The oscillations appear to include ThVos, since they undershot DD, a hyperpolarization typical of ThVos but not of Vos [17, 18]. Thus, on lowering [K+]o, Vos increased progressively and a fast rhythm could follow either a driven or a ThVos-induced AP, as in the case of adrenergic agonists.
In Fig. 4C, in the same SAN, driven APs (rightward oblique arrows) initiated trains of fast rhythm. The termination of the fast rhythm unmasked large damped oscillations. After the first two trains, drive was stopped and during the subsequent longer DD2, increasingly larger ThVos appeared (downward oblique arrows), which also initiated trains of fast rhythm. The termination of these trains was followed by damped oscillations, which showed large hyperpolarizing phases, typical of ThVos. Thus, the growth of both Vos and ThVos might be involved in the induction of sudden fast rhythms by APs elicited by drive or by ThVos.
When [K+]o was decreased from a higher value to 11.2 ± 0.4 mM, the SAN was either quiescent (n = 9) or driven at 6 min-1 (n = 11). ThVos initiated a fast rhythm in all the quiescent preparations and in 3 of the driven preparations. In the remainder, the fast rhythm was initiated by driven APs. The rate the sudden rhythm was 130 ± 3.7* min-1. When the fast rhythm subsided, large oscillations were unmasked.
Role of Vos and ThVos in the fast discharge in Tyrode solution
As for the mechanism leading to the sudden attainment of the threshold after the first action potential of the run, Vos could have directly attained the threshold by growing to a value positive to the resting potential (Fig. 4A and 4B). Alternatively, Vos could have entered the oscillatory zone and initiated a supra-threshold ThVos.
The contribution of both Vos and ThVos to fast rhythms is illustrated in Fig. 5 during recovery from high [K+]o to Tyrode solution. In high [K+]o sub-threshold stimuli at 6 min-1 were followed by sub-threshold ThVos (leftward oblique arrows). As shown in inset 1 at higher gain, ThVos consisted of damped depolarizing and hyperpolarizing phases. When Tyrode solution was superfused, the resting potential became more negative and a stimulus-driven ThVos (rightward oblique arrow) attained the threshold, thereby initiating an AP. The AP was followed by DD, but not by recognizable Vos or ThVos. The two larger APs at the end of Fig. 5A attained a more negative MDP and were followed by large Vos (short bars). After these APs were recorded, drive was discontinued.
In Fig. 5B, ThVos appeared which reached the threshold an initiated the first AP (star). During the following diastole, the larger and faster depolarizing phase of ThVos (arrow) elicited an AP that initiated a sudden fast rhythm (125 min-1). The beginning of the fast rhythm is shown at a greater time base in inset 2. As indicated by the horizontal arrow, the peak of Vos was still negative to the resting potential and could not possibly have attained the threshold. Instead, with a short delay, Vos was followed by a depolarizing event that attained the threshold in the potential range of the previous ThVos. The trace marked by the line beginning and ending with a dot in Fig. 5B is shown at a greater time base in inset 3. As Vos became larger (dots and shaded areas), the delay in the ensuing depolarizing phase became gradually shorter and eventually disappeared. The gradual fusion of Vos with the apparent depolarizing phase of ThVos led to the U-shaped DD (last trace in Fig. 5B). This suggests that the larger Vos entered the oscillatory zone and fused with ThVos so that the threshold was quickly attained.
The relationship between ThVos and voltage (oscillatory zone) is illustrated in inset 4, where sub-threshold stimuli were applied. The first stimulus caused a ThVos with an oscillation above and below the resting potential (vertical upward arrow in inset 4). The second stimulus increased the depolarizing phase of ThVos, which reached the threshold for the upstroke. During the following diastole, the first stimulus (leftward oblique arrow) did not induce a ThVos, but the subsequent stimuli fell on a gradually less negative DD and elicited gradually larger ThVos. The fifth stimulus enhanced the depolarizing phase of ThVos so that it attained the threshold.
As the drive continued, the stimuli during the early DD failed to elicit ThVos, but the oscillatory zone shifted to more negative values, as indicated by the fact that some ThVos initiated prior to the stimuli at potentials negative to the resting values (dots). Indeed, after the stoppage of the stimuli, spontaneous ThVos (still negative to the resting potential) initiated APs (not shown). These results suggest that the fast SAN discharge involves the growth of both Vos and ThVos and that the entry of Vos into the oscillatory zone is associated with a negative shift of faster and earlier ThVos.
The findings illustrated in Fig. 6 directly demonstrate the gradual growth and fusion of Vos and ThVos as well as the negative shift of the oscillatory zone. The SAN was spontaneously active (30 min-1) in high [K+]o and, during the recovery in Tyrode solution, the discharge at first increased gradually and then suddenly (Fig. 6A at normal and B at higher gain). As shown at a greater time base in Fig. 6C, the gradual acceleration was associated with a progressive growth of both Vos (dots) and of the sub-threshold ThVos(circles). In addition, the gradually increasing ThVos began at more negative potentials (negative shift of the oscillatory zone).
The gradually larger Vos and ThVos eventually fused. At the star, ThVos had barely missed the threshold and undershot DD (cf. DD at the beginning of trace 6C). During the following diastole (triangle) the depolarizing phase of ThVos attained the threshold. The superimposed traces in inset 1 show that indeed it was ThVos (and not Vos) that reached the threshold, thereby initiating fast discharge. As Vos kept on increasing (see dots in Fig. 6B), the depolarizing phase of ThVos became faster (see last three APs in Fig. 6C), leading to a slight increase in rate of the sudden fast rhythm. Thus, the sudden fast rhythm is different from a gradually increasing discharge in that the fusion of large Vos and ThVos leads to a quick attainment of the threshold for the upstroke.
In n = 15, in 16.0 ± 1.7 mM [K+]o, the SAN was either quiescent or spontaneously active (average rate 34.3 ± 9 min-1). During the recovery in Tyrode solution, in quiescent preparations, ThVos consistently initiated the spontaneous discharge. The spontaneous discharge increased gradually to 163 ± 6.5* min-1 by the time the MDP became more negative by 20.1 ± 1.9 mV. The gradual acceleration was caused by the increase in size and slopes of both Vos and ThVos, the latter occurring progressively sooner during diastole until Vos and ThVos gradually fused.
In n = 22, in 14.8 ± 1.6 mM [K+]o, the SAN was quiescent and during the recovery in Tyrode solution, when the resting potential had repolarized by 4.1 ± 0.4 mV, ThVos appeared and consistently initiated APs. A sudden fast rhythm initiated either after the very first AP or after a number of slower beats. The rate of the sudden rhythm was 140 ± 8.4* min-1 and it increased to 166 ± 6.2 min-1 (* with respect to 140 min-1) by the time the MDP had become more negative by 11.6 ± 1.3 mV.
In n = 30, in 16.8 ± 1.2 mM [K+]o, the SAN was active (either spontaneously active or driven at 6 min-1) with an average rate for all tests 19.8 ± 3.7 min-1. During the recovery in Tyrode solution, when the diastolic potential had become more negative by 4.2 ± 0.4 mV, a spontaneous or a driven AP initiated a sudden fast rhythm at 147 ± 7.3* min-1, which gradually increased to 177 ± 4.3 min-1 (* with respect to 147 min-1) by the time the MDP had become more negative by 12.5 ± 1.6 mV.
Thus, during the recovery in Tyrode solution (normal [K+]o), ThVos consistently initiated and gradually accelerated SAN discharge. The sudden discharge was due to the summation of large Vos and early ThVos during DD1.
Induction of slow and fast rhythms by overdrive
If adrenergic agents act by increasing [Ca2+]i, overdriving the SAN should act similarly, since a faster rate increases the intracellular Ca2+ . On this basis, shorter or slower overdrives would be expected to induce a smaller acceleration than longer or faster overdrives. In addition, the greater Ca2+ load with faster overdrive might induce fast rhythms.
In Fig. 7A, in high [K+]o, the spontaneous rate was 21.4 min-1. Overdrive at 60 min-1 progressively increased the size of the depolarizing phase of ThVos (cf. shaded areas at beginning and toward end of overdrive), until spontaneous APs preceded the electrical stimuli. On stoppage of drive, larger Vos and more rapid depolarization of ThVos increased the rate of discharge to 85.7 min-1. At that rate, the peak of Vos was followed by ThVos. In inset 1, the superimposed a traces show that the subsiding of overdrive excitation was due to ThVos missing the threshold. The superimposed b traces show that the ThVos missing the threshold oscillated above and below the control DD, as ThVos usually do.
In Fig. 7B, the spontaneous rate was 5.9 min-1. At the end of the 120 min-1 overdrive, after two APs, a sudden fast rhythm began at the rate of 150 min-1. The sudden fast rhythm was due to the fusion of the large Vos and ThVos. In inset 2, the superimposed a traces show that the subsiding of the fast rhythm was due to the large ThVos missing the threshold. The superimposed b traces show that ThVos that missed the threshold undershot the control DD. The results support the notion that fast sudden rhythms are brought about by the fusion of larger Vos and ThVos in early diastole due to a larger calcium load.
In n = 19, in 13.3 ± 0.9 mM [K+]o, all preparations but one were quiescent and a slow or short overdrive (average rate 44 min-1 for 43 s) did not induce discharge in 8 tests and caused overdrive excitation in 11 tests at the rate of 23.6 ± 6.7* min-1. In no instance, overdrive caused sudden a fast rhythm. In the same preparations, the control rate was 14.3 ± 5.1 min-1 and an overdrive at 95 ± 8 min-1 for 53 ± 7 s, increased the rate to 118 ± 13* min-1. In 8/19 of these tests, overdrive induced a sudden fast rhythm at the rate of 154 ± 18 min-1 either immediately or after a gradual acceleration. Therefore, at the same [K+]o, doubling the driving rate (+113%) consistently induced a much faster overdrive excitation and in 58% of the tests induced a sudden fast rhythm.
Low [Ca2+]o and the effects of adrenergic agonists on oscillatory potentials
If adrenergic agonists increase Vos and ThVos by increasing cellular calcium, then low [Ca2+]o would be expected to antagonize the adrenergic effects on the oscillatory potentials and on the rate increase.
In Fig. 8A, in high [K+]o, the upstroke of the AP was attained with a marked delay and was followed by sub-threshold responses at 28 min-1 (panel a). NE increased the amplitude and slope of Vos (short bars) and of ThVos (dash lines) and it induced APs with faster upstrokes and larger magnitude (panels c-e). In panel e, the superimposition of control diastolic trace (square) on that recorded during NE exposure (star) emphasizes the changes induced by NE on Vos and ThVos. The rate of discharge was faster (303% of control) and the twitch larger.
In Fig. 8B, during NE exposure, lower [Ca2+]o (-63.7%) gradually decreased Vos (short bars) and the slope of ThVos (dash lines) (panels f-h). At the rhombus, ThVos missed the threshold, as emphasized by the superimposition of the following AP (arrow) in panel g. As shown by the NE trace (star) superimposed on the low [Ca2+]o trace (panel h), lower [Ca2+]o decreased the magnitude and slope of the oscillatory potentials. The rate was decreased by 30% with respect to NE value and contractions were hardly visible. When [Ca2+]o was restored to its normal value, the effects of NE on rate and force were restored (panel i). The recovery in high [K+]o is shown in panel j.
In n = 3, in 13.3 ± 0.9 mM [K+]o, NE or isoproterenol (mean value 496 ± 272 nM) consistently increased the rate (225%), APa (26%), Vosds (194%), Vosa (83%), DDa (50%) and force (907%). In the presence of adrenergic agonists, lower [Ca2+]o (1.3 ± 0.4 mM) consistently decreased the rate (-39%), APa (-19%), Vosds (-28%), Vosa (-30%), DDa (-33%) and force (-47%). In a fourth experiment, low [Ca2+]o induced quiescence  and adding NE failed to induce spontaneous activity. In one experiment, during the exposure to isoproterenol, increasing [Ca2+]o markedly increased rate, DDs and force. Therefore, decreasing [Ca2+]o counteracted the increased calcium load by adrenergic agonists, thereby reducing their effects on oscillatory potentials and rate. Increasing [Ca2+]o had the converse effects.
Cesium effects on dominant and subsidiary SAN pacemakers
Since the oscillatory potentials are integral part of the dominant pacemaker mechanism, the effects of Cs+ (a blocker of If) on the oscillatory potentials were investigated to verify whether If participates in their mechanisms.
In Fig. 9A, in a spontaneously active SAN (14 beats min-1) in high [K+]o, the action potential was preceded by ThVos and was followed by Vos, as indicated by the respective arrows. Cs+ did not suppress either the oscillatory potentials or discharge. Instead, Cs+ increased the rate by means of larger and earlier ThVos and larger Vos, as emphasized by the superimposed traces labeled by rhombus and a square without and within inset 1. The more negative ThVos are consistent with a negative shift of the oscillatory zone.
In inset 2, the progressive changes in Vos and ThVos are shown at greater time base, ThVos reaching the threshold by the last dot, as its depolarizing phase became larger and faster. The gradually increasing peak and under-swing of the subsequent diastolic oscillations in inset 2 suggests that Vos and the depolarizing phase of ThVos were fused (greater peak), the under-swing being caused by the larger hyperpolarizing phase of ThVos. Eventually, Vos and ThVos fused in the U-shaped DD (last A panel), the rate being 130 beats min-1 (828%).
The converse changes occurred during recovery from Cs+ exposure (Fig. 9B). When the first fused diastolic oscillation (upward oblique arrow) missed the threshold, a large ThVos was present (downward oblique arrow), although only a subsequent one initiated an AP (trace a). Later on, Vos was smaller and clearly separated from the subsequent smaller ThVos (trace b). The complete separation between Vos and ThVos is shown in trace c, where DD is interposed between the two oscillatory potentials. The depolarizing and hyperpolarizing slopes of ThVos gradually became slower and the oscillatory zone returned to less negative values.
In n = 5, (Fig. 9, inset 3), in SAN quiescent in 13.3 ± 0.4 mM [K+]o, 1.5 ± 0.2 mM Cs+ induced spontaneous discharge at 29* min-1 and induced the following changes: APa -0.002%, Vosa 53%, Vosds 73%*, ThVosds 132%* and force 20% (APd -2.9%, DDa 23%, not shown).
In n = 14, in SAN active in 13.6 ± 0.8 mM [K+]o, 1.7 ± 0.1 mM Cs+ induced the following changes: rate 97%*, APa -0.002%, APd 0.006%, Vosds 116%, Vosa 8.6%, ThVosds 330%*, DDa -0.01% and force 48%. Therefore, Cs+ did not abolish Vos, ThVos or DD, indicating that If does not play a role in the mechanisms underlying these events. This agrees with findings that in SAN Cs+ blocks If, but not spontaneous discharge in Tyrode solution [19, 25] or in high [K+]o .
The more negative DD of SAN subsidiary pacemakers appears to be due to the activation of If  and therefore Cs+ would be expected to have on subsidiary pacemakers in Tyrode solution effects different from those on dominant pacemakers (see [26, 27]). In Tyrode solution (n = 8), 4.4 ± 1.2 mM Cs+ induced the following changes: rate -18.7%*, APa 1.5%, APd 93%*, DDa -81%*, DDs -87%* and force 0.0%. The increase in APd was due to a slowing of the late phase 3 repolarization (the "tail") whose amplitude was 31.8 ± 2.9* mV and slope was 311 ± 18.9* mV s-1 (see ).
Cesium and the positive chronotropic effect of norepinephrine
Even if SAN oscillatory potentials do not appear to involve If, still the positive chronotropic effect of NE could be mediated by a positive shift of the activation curve of If [2, 21]. If it were so, then Cs+ should antagonize the acceleratory action of NE by blocking If, thereby making its positive shift irrelevant. This was tested by giving Cs+ first (to block If) and then by adding NE.
In Fig. 10A control, a spontaneous AP is shown in the first panel and the lower part of the same AP (followed by diamond pattern and quiescence) is shown in the second panel. Cs+ administration made ThVos re-appear, gradually increase in size and re-initiate spontaneous discharge. Typically, each AP was followed by Vos and by the temporary suppression of ThVos. The latter reappeared when DD re-entered the oscillatory zone. Discharge gradually increased until a steady rhythm was present (29 beats min-1, Fig. 10B, panel a). Thus, (in contrast to early afterdepolarizations) the pre-potential ThVos can occur at the resting potential in the absence of APs and it is temporarily suppressed by an action potential.
When NE was added to the Cs+ solution, Vos amplitude (short bars) and ThVos slope (dash lines) increased and attained the threshold with each ThVos (64.8 beats min-1, panel b). The greater Vos and much steeper slope of ThVos further increased the rate (130 beats min-1, panel c) and led to U-shaped DD (176 min-1, panel d). Contractile force increased during NE exposure by 633%. In inset 1, the traces (superimposed by the MDP) show that the marked increase in rate from trace a (Cs+) to trace b (+NE) was due to NE-induced steepening of depolarizing phase of ThVos, which allowed it to initiate an AP. The subsequent increase in rate involved both an increase in Vos amplitude and a much steeper slope of ThVos (trace c), until Vos and ThVos became fused and no longer distinguishable (trace d). During the recovery from NE in the Cs+ solution, the rate slowed through the decrease of Vos and ThVos amplitude (panel e).
In inset 2 (n = 4), in SAN active in 13.6 ± 1 mM [K+]o, 1.6 ± 0.2 mM Cs+ induced the following changes: rate 84%, APa 4.6%, APd 1.1%, DDa -6.5%, Vosa -7.7%, Vosds 17.9%, ThVosds 280% and force 471%. Adding 351 ± 58 nM NE induced the following changes with respect to the Cs+ values: rate 87.2%*, APa 7.8% APd -9.6%, DDa 15.7%, Vosa 36.9%, Vosds 17.8%, ThVosds 56.6%, and force 1118.5%.
If Cs+ did not prevent the acceleratory action of NE, NE did not prevent a further increase in rate of discharge by Cs+, indicating that Cs+ has the same effect in the absence (basal rhythm) and in the presence of NE. The effects of Cs+ were reversible in NE solution, showing that the further acceleration during Cs+ exposure was not due to a still increasing positive chronotropic effect of NE. In n = 2 (inset 3), in SAN active in 13.6 ± 1 mM [K+]o, NE (279 ± 95 nM) induced the following changes: rate 1378%*, DDa 18.1%, Vosa 82.3%*, Vosds 90%*, ThVosds 260% (APa 6.1%, APd -11.5%, not shown). Adding Cs+ (1.96 ± 8 mM) induced the following changes with respect to the NE values: rate 91.6%*, DDa 79.4%, Vosa 45%*, Vosds 12.4% and ThVosds 241% (APa -0.08%, APd 4.3%, not shown).
Barium and the oscillatory potentials
The block of If by Cs+ did not abolish the oscillatory potentials. Instead, Cs+ actually increased the rate of discharge, certainly not through its block of If and possibly through a decrease in K+ conductance. If so, barium should also increase the rate of discharge, since Ba2+ blocks K+ currents, but not If .
In Fig. 11A, in SAN superfused in high [K+]o, the control panel shows two APs, followed by the diamond pattern and quiescence. Exposure to a low concentration of Ba2+ made ThVos re-appear and initiate discharge that quickly accelerated due to earlier and larger ThVos (dots) as well as larger DD2 (traces a-d). As shown in panel e, after the peak of Vos (short bar), the depolarizing slope of ThVos reached the threshold for the upstroke. The section of trace d labeled with the line terminating with dots and displayed at a greater time base in inset 1 (top trace) shows that Ba2+ quickly increased the depolarizing phase of sub-threshold ThVosso that it consistently reached the threshold (shaded areas).
In Fig. 11B, during the recovery from Ba2+ exposure, the amplitude of the depolarizing phase of ThVos gradually decreased and intermittently missed the threshold. ThVos began gradually later during DD (traces f-h). Eventually, ThVos appeared only during the late DD2 (trace i) and quiescence followed shortly thereafter. The section of trace f labeled with a line terminating with squares and displayed at greater time base in inset 1 (bottom trace) shows the converse changes with respect to the top trace. Namely, the depolarizing phase of ThVos missed the threshold and quickly decreased in size (shaded areas) with a consequent decrease in rate.
In inset 2, the superimposed traces show that Ba2+ increased the amplitude of DD and caused ThVos to appear gradually sooner. Conversely, during the recovery from Ba2+ (inset 3), ThVos became smaller and started later during a more negative DD2.
In inset 4, n = 6, in SAN mostly quiescent in 15.1 ± 0.9 mM, [K+]o, Ba2+ (89.6 ± 13.7 nM) depolarized the resting membrane by 4.2 ± 0.9 mV and induced the following changes: rate 1078%*, APa -5.8%, DDa 13.5%, Vosa 36.2%*, Vosds 63.4%*, ThVosds 162.1%*, and force 588% (APd 20.4%*, not shown). Thus, in high [K+]o, Ba2+ (a blocker of K+ conductance) increased the rate through an increase in amplitude of Vos, ThVos and DD, as Cs+ does.
From the results obtained, we conclude that adrenergic activation increases the SAN rate by increasing the pacemaking components DD1, Vos and ThVos. Their fusion by NE in high [K+]o or during the recovery from high [K+]o to Tyrode solution leads to the U-shaped DD, typical of dominant pacemakers. In quiescent SAN, adrenergic agonists initiate spontaneous discharge by decreasing the resting potential, thereby inducing ThVos. Gradually earlier and larger ThVos are mainly responsible for a gradual acceleration in rate, and the sudden fusion of large Vos and ThVos for the induction of fast rhythms.
Adrenergic agonists appear to act by increasing [Ca2+]i, since other procedures known to increase cellular calcium (e.g., lowering high [K+]o and overdrive) also increased SAN discharge by increasing the size and slope of Vos and ThVos and by shifting the oscillatory zone in a negative direction. Conversely, low [Ca2+]o antagonizes the effects of adrenergic agonists. A larger calcium load by NE, lower [K+]o and faster overdrives facilitates the abrupt onset of fast rhythms.
Even though it has been reported that adrenergic stimulation can change the gating and amplitude of If in SA nodal cells (see ), the experiments with Cs+ show that If modulation does not contribute to the oscillatory potentials involved in dominant discharge or to their modifications by adrenergic agonists. The increase in rate of discharge by Cs+ appears to involve a decrease in potassium conductance, since similar results were obtained with Ba2+. The different effects of Cs+ on dominant pacemakers in high [K+]o and in subsidiary pacemakers in Tyrode solution suggest to a role of If in the more negative subsidiary diastolic depolarization.
Mechanisms of initiation of pacemaker activity by adrenergic agonists
For NE to decrease the resting potential, an increase in a net inward current is required. Several currents do not appear to be involved in NE-induced depolarization. The block of If by Cs+ did not suppress the depolarization in the absence (present results) and in the presence of nifedipine . ICaT is not increased by adrenergic agonists [7, 9] and, at the holding potential of -40 mV, ICaT  and voltage-dependent Na+ channels would be inactivated. A decrease or positive shift of IK is ruled out, since isoproterenol increases the amplitude of IK and causes a negative shift of its activation curve . A decrease in the outward Na+-K+ pump current is also unlikely to be involved, since NE stimulates the Na+-K+ pump activity [30, 31]. Therefore, both an increase in IK and in Na+-K+ pump activity would hyperpolarize (not depolarize) the resting membrane.
Adrenergic activation decreased the resting potential in guinea pig SAN arrested by 10 μM nifedipine , demonstrating that the depolarization occurs after the block of ICaL. Exogenous NE caused depolarization by releasing calcium from SR stores through the activation of metabolic pathways . This intracellular release of calcium activates an inward INa-Ca, which depolarizes the resting membrane.
In the present experiments, in the absence of nifedipine, adrenergic activation would be expected to increase also ICa. Thus, adrenergic agonists lead to a cAMP-mediated PKA-dependent phosphorylation not only of the ryanodine receptors and of phospholamban, but also of the L-type Ca2+ channels [3, 12]. A contribution of sub-threshold ICa to the decrease of the resting potential is made likely by the fact that the resting potential of the SAN (~-40 mV) is fairly close to the threshold for ICa activation . In high [K+]o, nifedipine stopped SAN discharge by preventing the attainment of the threshold . In SAN quiescent in high [K+]o, high [Ca2+]o decreased the resting potential, thereby leading to the appearance of ThVos and of discharge .
During the decrease of the resting potential, sub-threshold Ca2+ entry induced by NE or high [Ca2+]o could also release Ca2+ from the SR. However, the primary event would be the enhanced Ca2+ influx through the surface membrane, as in the case of the latent atrial pacemakers  and of an inward calcium component elicited either by a small depolarizing step during late DD  or at -40 mV during ramps from -60 to -20 mV .
The decrease in resting potential, by entering the oscillatory zone, allowed ThVos to appear and initiate discharge (Fig. 1; Fig. 3, panel f). Therefore, not the depolarization per se, but the onset of ThVos was responsible for the initiation of discharge. Also, in quiescent Purkinje fibers, NE decreased the resting potential, induced ThVos and initiated spontaneous discharge . However, in Purkinje fibers, not only the resting potential is much more negative to the threshold for ICa, but the depolarizing phase of ThVos is related to a slowly inactivating sodium current (INa3) which is activated in the oscillatory zone of Purkinje fibers (~-60 to -50 mV) .
Mechanisms of gradual increase in rate by adrenergic agonists
The gradual increase in SAN discharge by adrenergic agonists involves (in addition to ThVos) two additional mechanisms, namely, DD1 and Vos. Both events obligatorily follow the action potential, in contrast to ThVos.
As for DD1, in the presence of background sodium current, the decay of IK leads to DD (e.g., see [4, 10, 19, 32]). NE increases the magnitude of IK, shifts its activation curve in a negative direction  and speeds up its rate of deactivation [10, 35], thereby accounting for the shortening of the AP, the increase in MDP and the steepening of a larger DD1.
With a resting potential of -40 mV, the already deactivated If can not decrease during the AP to account for the subsequent undershoot to the MDP . Further, If activates too slowly at the MDP to account for DD (see ). In any case, the undershoot was not abolished by Cs+, as it would be expected if it were due to the deactivation of If during the AP. Instead, the undershoot persisted, because Cs+ does not block IK.
As for Vos, NE-induced phosphorylation of L-type Ca2+ channels increases ICa  and the Ca2+ transient [8, 14]. At the same time, the phosphorylation of phospholamban and of the ryanodine receptors increases Ca2+ uptake into as well as release from the SR (see ). The greater SR release of calcium during late diastole results in larger INa-Ca [8, 11] and in a faster and larger Vos. In turn, Vos steepens DD1 and brings it closer to the oscillatory zone.
Discharge is enhanced also by the negative shift of the oscillatory zone (the threshold for ThVos becomes more negative). The increase in [Ca2+]i could shift the oscillatory zone in a negative direction for the same reason that an increase in [Ca2+]o shifts the threshold for the fast sodium current INa in a positive direction, namely, by screening surface membrane negative charges.
Also in Purkinje fibers, NE increases the amplitude of Vos induced by other interventions [39–41]. In fact, interventions that increase cellular Ca2+ (low [K+]o, high [Ca2+]o, repetitive depolarizing steps, strophanthidin as well as NE) markedly increased the slope and amplitude of Ios (the current underlying Vos) and therefore also the slope of the pacemaker current upon which Ios is superimposed .
The NE-induced gradual increase in rate was predominantly due to the changes in ThVos, but the amplitude of Vos and DD also increased. Eventually, the fusion of the enhanced DD1, Vos and ThVos resulted in a steeper slope of the U-shaped DD. In Tyrode solution, adrenergic agonists steepen the slope of the U-shaped DD through the same changes, since an increased calcium load increases Vos and ThVos when visible in the SAN (e.g., ) as well as in Purkinje fibers (e.g., [22, 41]). Therefore, the U-shaped DD due to the fusion of larger Vos, ThVos and DD1 is present not only when norepinephrine is administered in high [K+]o, but in other conditions that also increase intracellular calcium, such as a suitable reduction in high [K+]o, after fast overdrive and during recovery from high [K+]o to Tyrode solution.
Mechanisms of sudden onset of fast rhythms by adrenergic agonists
As for the sudden onset of fast rhythms, the mechanism of initiation required at least one AP, pointing to the essential role of Vos. However, the simultaneous growth of ThVos and the negative shift of the oscillatory zone contributed to the initiation and maintenance of sudden fast rhythms. Both Vos and ThVos grew prior to the onset of the sudden fast rhythm, but (when Vos and ThVos fused suddenly) it was ThVos that attained the threshold for the upstroke (see Fig. 6).
The contribution of both Vos and ThVos to the fast discharge is also indicated by the large oscillations unmasked by the sudden cessation of the fast rhythm. Damped oscillations are seen also with large Vos(e.g., ) and Ios (e.g, ), but the contribution of fused ThVos is suggested by the fact that the largest hyperpolarizing phase of the oscillations undershot DD: ThVos does that , but not Ios .
Since an increase in rate per se enhances calcium loading, the further increase in Vos and ThVos accounts for the increase in rate during the fast rhythm, as also suggested by the large oscillations that followed its sudden cessation. Therefore, the initiation of sudden fast rhythms depends on a sudden fusion of larger Vos and ThVos, whereas the gradual acceleration of the rate is due to the increment in the oscillatory potentials, the gradually earlier onset of ThVos and more negative oscillatory zone.
The induction of sudden fast rhythms by fast (but not slow) overdrive suggests that a sudden increase in rate is due to a greater Ca2+ load. Thus, a slow/short overdrive induced a ThVos-dependent slow rhythm, whereas fast/long drives often induced a sudden fast rhythm. The fast rhythms in high [K+]o reflect the mechanism underlying the SAN fast discharge in Tyrode solution, as demonstrated here in the guinea pig by the unmasking of diastolic oscillations by high [K+]o and their progressive growth and fusion on return to Tyrode solution.
The induction or acceleration of discharge by overdrive is not unique to the SAN, since it was first described and labeled "overdrive excitation" in Purkinje fibers overdriven in the presence of NE  (later on, overdrive excitation was also labeled "triggered activity").
In vivo, in animals with chronic complete atrio-ventricular (A-V) block, stimulation of the stellate ganglion  or of the splanchnic nerves to the adrenal medulla  induced a gradual increase in idioventricular rate. In animals with acute A-V block, the operative and postoperative stress is associated with an increased plasma level of catecholamines. When calcium load was increased by left stellate ganglion stimulation, NE administration, Ca2+ infusion, overdrive could induce ventricular tachycardias, which initiated and stopped abruptly . In Purkinje fibers superfused in vitro, when the Ca2+ load was increased by lower [K+]o, high [Ca2+]o, low [Na+]oor NE administration, overdrive induced Vos and ThVos, and fast discharge [22, 41].
Therefore, in vitro as well as in vivo, in cardiac pacemakers sympathetic enhancement can induce both a gradual or sudden change in rate. The role of an adrenergically-increased Ca2+ load in increasing SAN rate is shown by similar results obtained with procedures that increase [Ca2+]i, such as decreasing high [K+]o, recovery in Tyrode solution and faster or longer overdrives. Reciprocally, a lower [Ca2+]o antagonized the effects of the adrenergic agonists. Because catecholamines increase cellular calcium whereas high [K+]o decreases it, it is not surprising that the resistance of SAN discharge to high [K+]o in part depends on the degree of sympathetic activation .
If, oscillatory potentials and increase in rate by norepinephrine
The experiments with Cs+ addressed three separate issues. The first issue was the role of the hyperpolarization-activated If in the oscillatory potentials. If the hyperpolarization-activated If were responsible for the oscillatory potentials, cesium (by blocking If) should have suppressed them and stopped SAN discharge under basal conditions. This did not occur, indicating that If is not involved in the mechanism of the oscillatory potentials.
The second issue was related to the suggestion that adrenergic agents increase the discharge of SAN by shifting the activation curve of If to less negative potentials [2, 21]. If so, then cesium (by blocking If) should have prevented its positive shift by NE and, therefore, would have abolished the consequent increase in rate. Since NE increased SAN discharge by enhancing the oscillatory potentials also in the presence of cesium, the result indicates that the positive chronotropic effect of NE does not involve an action of If on the oscillatory potentials. This agrees with the finding that epinephrine increases the rate of discharge of SAN in the presence of a demonstrated block of If by Cs+ . Also, in canine SAN, blockade of If with ZD 7288 decreased SAN rate by 8.3%, but neither prevented the isoproterenol-induced increase in rate nor the late diastolic Ca2+ elevation .
The third issue was that the mechanism by which cesium increased the basal rate of discharge. This mechanism could not be the block of If and might be related to a decrease in potassium conductance. Indeed, in ventricular myocytes  and in Purkinje fibers (see ), high [K+]o increases IK1 conductance, although IK1 is far less expressed in SAN dominant pacemaker cells than in ventricular or Purkinje cells. This hypothesis was tested by using barium, that (like cesium) decreases potassium conductance, but (unlike cesium) does not block If . The results show that the decrease in potassium conductance appears responsible for the increase in rate by cesium or barium.
The major action of adrenergic agonists appears related to the greater calcium load. The greater Ca2+ influx and the greater Ca2+ release from SR during systole increase contractile force. The greater release of Ca2+ during diastole in SAN dominant pacemakers increases INa-Ca and therefore amplitude and slope of Vos. An increase in [Ca2+]i also increases the slope and magnitude of ThVos and shifts the threshold to more negative values by shifting the oscillatory zone. The overall changes result in a faster rate of discharge, faster conduction and stronger contraction, which, in turn, lead to a larger cardiac output. Therefore, in all cells adrenergic control of the heart involves an increase in [Ca2+]i. In dominant pacemaker cells, such a Ca2+ increase enhances the factors involved in SAN discharge (DD, Vos and ThVos).
As for clinical implications, in a healthy person, the activation of the sympathetic system, would be expected to lead to the gradual increase in heart rate, which contributes to an increase in cardiac output (e.g., exercise). In a patient in cardiac arrest, intracardiac injection of NE may initiates spontaneous activity by eliciting ThVos in Purkinje fibers. If the SR of the cardiac cells is already calcium overloaded by disease (see ), then an increased adrenergic activation may lead to abrupt tachycardias by allowing the fused Vos and ThVos in pacemaker tissues or large Vos in myocardial tissues to suddenly attain the threshold for the upstroke.
Because Vos and ThVos size as well as the negative shift of the oscillatory zone are a function of [Ca2+]i, a sudden tachycardia implies a larger Ca2+ overload and/or a diminished ability of cardiac cells to cope with such a load. This may result from an increased Ca2+ load, e.g., a prolonged adrenergic activation, a persistent increase in rate (e.g., cardiac failure), a reduced Ca2+ extrusion due to a reduced Na+-K+ pump activity (e.g., ischemia or toxic concentrations of cardiac glycosides) (see ) or to a decrease in [K+]o(hypokalemia).
Brown HF, DiFrancesco D, Noble SJ: How does adrenaline accelerate the heart?. Nature. 1979, 280: 235-236. 10.1038/280235a0.
DiFrancesco D: Pacemaker mechanisms in cardiac tissue. Annu Rev Physiol. 1993, 55: 455-472. 10.1146/annurev.ph.55.030193.002323.
Maltsev VA, Vinogradova TM, Lakatta EG: The emergence of a general theory of the initiation and strength of the heartbeat. J Pharmacol Sci. 2006, 100: 338369-10.1254/jphs.CR0060018.
Irisawa H, Brown HF, Giles W: Cardiac pacemaking in the sinoatrial node. Physiol Rev. 1993, 73: 197-227.
Vassalle M: The vicissitudes of the pacemaker current IKdd of cardiac Purkinje fibers. J Biomed Sci. 2007, 14: 699-716. 10.1007/s11373-007-9182-2.
Noma A, Kotake H, Irisawa H: Slow inward current and its role mediating the chronotropic effect of epinephrine in the rabbit sinoatrial node. Pflügers Arch. 1980, 388: 19-10.1007/BF00582621.
Hagiwara N, Irisawa H, Kameyama M: Contribution of two types of calcium currents to the pacemaker potentials of rabbit sino-atrial node cells. J Physiol. 1988, 395: 233-253.
Ju YK, Allen DG: How does β-adrenergic stimulation increase the heart rate? The role of intracellular Ca2 release in amphibian pacemaker cells. J Physiol. 1999, 516: 793-804. 10.1111/j.1469-7793.1999.0793u.x.
Freeman LC, Kass RS: Delayed rectifier potassium channels in ventricle and sinoatrial node of the guinea pig: molecular and regulatory properties. Cardiovasc Drugs Ther. 1993, 7: 627-635. 10.1007/BF00877630.
Lei M, Brown HF, Terrar DA: Modulation of delayed rectifier potassium current, iK, by isoproterenol in rabbit isolated pacemaker cells. Exp Physiol. 2000, 85: 27-35. 10.1017/S0958067000019151.
Zhou Z, Lipsius SL: Na+Ca2+ exchange current in latent pacemaker cells isolated from cat right atrium. J Physiol. 1993, 466: 263-285.
Vinogradova TM, Bogdanov KY, Lakatta EG: β-adrenergic activation modulates ryanodine receptor Ca2+ release during diastolic depolarization to accelerate pacemaker activity in rabbit sinoatrial nodal cells. Circ Res. 2002, 90: 73-79. 10.1161/hh0102.102271.
Allen DG, Blinks JR: Calcium transients in aequorin-injected frog cardiac muscle. Nature. 1978, 273 (5663): 509-513. 10.1038/273509a0.
Ju YK, Allen DG: Intracellular calcium and Na+-Ca2+ exchange current in isolated toad pacemaker cells. J Physiol. 1998, 508: 153-166.
Kim EM, Choy Y, Vassalle M: Mechanisms of suppression and initiation of pacemaker activity in guinea-pig sino-atrial node superfused in high [K+]o. J Mol Cell Cardiol. 1997, 29: 1433-1445. 10.1006/jmcc.1997.0382.
Choy Y, Kim EM, Vassalle M: Overdrive excitation in the guinea pig sino-atrial node superfused in high [K+]o. J Biomed Sci. 1997, 4: 179-191. 10.1007/BF02255647.
Nett MP, Vassalle M: Obligatory role of diastolic voltage oscillations in sino-atrial node discharge. J Mol Cell Cardiol. 2003, 35: 1257-1276. 10.1016/S0022-2828(03)00236-0.
Catanzaro JN, Nett MP, Rota M, Vassalle M: On the mechanisms underlying diastolic voltage oscillations in the sino-atrial node. J Electrocardiol. 2006, 39: e1-342. 10.1016/j.jelectrocard.2006.03.006.
Zhang H, Vassalle M: Role of dual pacemaker mechanisms in sino-atrial node discharge. J Biomed Sci. 2000, 7: 100-113. 10.1007/BF02256616.
Noma A: Mechanisms underlying cessation of rabbit sinoatrial node pacemaker activity in high potassium solutions. Jpn J Physiol. 1976, 26: 619-630.
Zaza A, Robinson RB, DiFrancesco D: Basal responses of the L-type Ca2+ and hyperpolarization-activated currents to autonomic agonists in the rabbit sinoatrial node. J Physiol. 1996, 491: 347-355.
Spiegler P, Vassalle M: Role of voltage oscillations in the automaticity of sheep cardiac Purkinje fibers. Can J Physiol Pharmacol. 1995, 73: 1165-1180.
Anderson RH: The disposition, morphology and innervation of the cardiac specialized tissue in the guinea-pig. J Anat. 1972, 111: 453-468.
Vassalle M, Knob RE, Lara GA, Stuckey JH: The effect of adrenergic enhancement on overdrive excitation. J Electrocardiol. 1976, 9: 335-343. 10.1016/S0022-0736(76)80026-X.
Denyer JC, Brown HF: Pacemaking in rabbit isolated sino-atrial node during Cs+ block of the hyperpolarization-activated current, if. J Physiol. 1990, 429: 401-409.
Zhang H, Vassalle M: On the mechanisms of adrenergic control of the sino-atrial node discharge. J Biomed Sci. 2003, 10: 179-192. 10.1007/BF02256053.
Kreitner D: Electrophysiological study of the two main pacemaker mechanisms in the rabbit sinus node. Cardiovasc Res. 1995, 19: 304-318. 10.1093/cvr/19.5.304.
Yanagihara K, Irisawa H: Potassium current during pacemaker depolarization in rabbit sinoatrial node cell. Pflügers Arch. 1980, 388: 255-260. 10.1007/BF00658491.
Cohate JK, Edwards FR, Hirst GDS, O'Shea JE: Effects of sympathetic nerve stimulation on the sino-atrial node of the guinea-pig. J Physiol. 1993, 471: 707-727.
Vassalle M, Barnabei O: Norepinephrine and potassium fluxes in cardiac Purkinje fibers. Pflügers Arch. 1971, 322: 287-303. 10.1007/BF00587747.
Lee CO, Vassalle M: Modulation of intracellular Na+ activity and cardiac force by norepinephrine and Ca2+. Am J Physiol. 1983, 244: C11O-C114.
Brown HF, Giles WR, Noble SJ: Membrane currents underlying activity in frog sinus venosus. J Physiol. 1977, 271: 783-816.
Vassalle M, Carpentier R: Hyperpolarizing and depolarizing effects of norepinephrine in cardiac Purkinje fibers. Research in Physiology, A Liber Memorialis in Honor of Prof. C. McC. Brooks. Edited by: Kao FF, Koizumi K, Vassalle M. 1971, Gaggi Publisher, 373-388.
Rota M, Vassalle M: Patch-clamp analysis in canine cardiac Purkinje cells of a novel sodium component in the pacemaker range. J Physiol. 2003, 548 (1): 147-165. 10.1113/jphysiol.2003.039263.
Anumonwo JMB, Freeman LC, Kwok WM, Kass RS: Delayed rectification in single cells isolated from guinea pig sinoatrial node. Am J Physiol. 1992, 262: H921-H925.
Zhang H, Vassalle M: Role of IK and If in the pacemaker mechanisms of sino-atrial node myocytes. Canadian J Physiol Pharmacol. 2001, 79: 963-976. 10.1139/cjpp-79-12-963.
Liu YM, Yu H, Li CZ, Cohen IS, Vassalle M: Cs+ effects on if and iK in rabbit sinoatrial node myocytes: implications for SA node automaticity. J Cardiovasc Pharmacol. 1998, 32: 783-790. 10.1097/00005344-199811000-00015.
Maltsev VA, Lakatta EG: Dynamic interactions of an intracellular Ca2+ clock and membrane ion channel clock underlie robust initiation and regulation of cardiac pacemaker function. Cardiovasc Res. 2008, 77: 274-284. 10.1093/cvr/cvm058.
Paspa P, Vassalle M: Mechanism of caffeine-induced arrhythmias in canine cardiac Purkinje fibers. Am J Cardiol. 1984, 53: 313-319. 10.1016/0002-9149(84)90445-4.
Di Gennaro M, Carbonin P, Vassalle M: On the mechanism by which caffeine abolishes the fast rhythms induced cardiotonic steroids. J Mol Cell Cardiol. 1984, 16: 851-862. 10.1016/S0022-2828(84)80009-7.
Valenzuela F, Vassalle M: Overdrive excitation and cellular calcium load in canine cardiac Purkinje fibers. J Electrocardiol. 1985, 18: 21-34. 10.1016/S0022-0736(85)80031-5.
Vassalle M, Mugelli A: An oscillatory current in sheep cardiac Purkinje fibers. Circ Res. 1981, 48: 618-631.
Greenberg YJ, Vassalle M: On the mechanism of overdrive suppression in the guinea pig sino-atrial node. J Electrocardiol. 1990, 23: 53-67. 10.1016/0022-0736(90)90151-Q.
Hasegawa J, Satoh H, Vassalle M: Induction of the oscillatory current by low concentrations of caffeine in sheep cardiac Purkinje fibres. Naunyn-Schmiedeberg's Arch Pharmacol. 1987, 335: 310-320. 10.1007/BF00172803.
Vassalle M, Carpentier R: Overdrive excitation: the initiation of spontaneous activity in Purkinje fibers following a fast drive in the presence of norepinephrine. Pflügers Arch. 1972, 332: 198-205. 10.1007/BF00587447.
Vassalle M, Levine MJ, Stuckey JH: On the sympathetic control of ventricular automaticity: the effects of stellate ganglion stimulation. Circ Res. 1968, 23: 249-258.
Vassalle M, Stuckey JH, Levine MJ: Sympathetic control of ventricular automaticity: role of the adrenal medulla. Am J Physiol. 1969, 217: 930-937.
Vassalle M, Greineder JK, Stuckey JH: Role of the sympathetic nervous system in the sinus node resistance to high potassium. Circ Res. 1973, 32: 348-354.
Joung B, Tang L, Maruyama M, Han S, Chen Z, Stucky M, Jones LR, Fishbein MC, Weiss JN, Chen PS, Lin SF: Intracellular calcium dynamics and acceleration of sinus rhythm by beta-adrenergic stimulation. Circulation. 2009, 119: 788-796. 10.1161/CIRCULATIONAHA.108.817379.
Sung RJ, Wu SN, Wu JS, Chang HD, Luo CH: Electrophysiological mechanisms of ventricular arrhythmias in relation to Andersen-Tawil syndrome under conditions of reduced IK1: a simulation study. Am J Physiol. 2006, 291: H2597-H2605.
Vassalle M, Lin CI: Calcium overload and cardiac function. J Biomed Sci. 2004, 11: 542-565. 10.1007/BF02256119.
This work was supported in part by a grant from N.I.H. (HL56092) to MV.
The authors declare that they have no competing interests.
This work was a collaborative endeavor in which all authors were involved under the guidance, coordination and major participation of MV in all aspects of the research process in succession (design, experiments, discussion of results, measurements of results, preparation of figures, statistical analysis, and drafting of the manuscript). All experimental work was carried out in the Department of Physiology and Pharmacology, State University of New York, Downstate Medical Center, Brooklyn, NY 11203, USA. All authors read and approved the final manuscript.
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Vassalle, M., Catanzaro, J.N., Nett, M.P. et al. Essential role of diastolic oscillatory potentials in adrenergic control of guinea pig sino-atrial node discharge. J Biomed Sci 16, 101 (2009). https://doi.org/10.1186/1423-0127-16-101
- Oscillatory Potential
- Spontaneous Discharge
- Oscillatory Zone
- Adrenergic Agonist
- Purkinje Fiber