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From the Department of Physiology, Faculty of Medicine, Kyoto University, Kyoto, Japan.
Correspondence to Akinori Noma, Department of Physiology, Faculty of Medicine, Kyoto University, Sakyo-Ku, Yoshida-Konoe, Kyoto 606-8501, Japan. E-mail noma{at}card.med.kyoto-u.ac.jp
| Abstract |
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Key Words: cardiac pacemaker sinoatrial node sustained inward current
| Introduction |
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In addition to the above basic mechanisms, involvement of voltage-dependent inward currents, such as If, is necessary9 to explain dynamic changes in the pacemaker depolarization under physiological conditions, such as during the positive chronotropic effect of ß-adrenergic stimulation. Verheijck et al10 demonstrated that a small ICa, L can be activated on depolarization to -60 mV from a holding potential of -90 mV, suggesting a role for ICa, L in the pacemaker modulation, although most studies report that ICa, L is activated only at potentials less negative than -40 mV.11 12 Recently, a novel inward current, Ist, was identified in spontaneously active SA node cells of rabbits,13 guinea pigs,14 and rats15 and in the atrioventricular (AV) node cells of rabbits.16 17 Because Ist is activated by depolarization within the range of slow diastolic depolarization, contribution of Ist to pacemaker depolarization was suggested. In support of this, Ist was identified in spontaneously active cells but was not observed in quiescent cells dissociated from either SA or AV nodes.
The characteristics of Ist in comparison
with ICa, L are summarized in the Table
.
Ist is increased nearly 2-fold by
ß-adrenergic stimulation (isoprenaline 100 nmol/L), and this increase
is reversed by adding acetylcholine.14
Ist is resistant to tetrodotoxin
(30 µmol/L) and is blocked by the classical
Ca2+ antagonists, such as
verapamil (1 µmol/L), D600 (0.1 µmol/L),
nicardipine (0.25 to 0.5 µmol/L), and heavy metal
cations (1 mmol/L Ni2+ and
Co2+).13 Interestingly, 40
µmol/L Ni2+, which completely blocks
ICa, T,11 also blocks
Ist by
50%.13
Ist is increased by the
Ca2+ agonist Bay-K8644.14 These
pharmacological characteristics of Ist are
similar to those of ICa, L. However,
Ist is distinct from the window component
of ICa, L, various types of
Ca2+ channels, persistent
Na+ current in ventricle, the background
Na+ current, and the
Na+/Ca2+ exchange current.
These comparisons were presented elsewhere in the mutual
disruption of Ist.13
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Although Ist has been described only by our group, similar currents were identified by Denyer and Brown.18 They used a ramp pulse (0.1 mV · ms1 from -70 to +30 mV) and recorded inward current activation on depolarization beyond -60 mV. The current density of 2 pA/pF is comparable with Ist described in rabbit SA node cells. Denyer and Brown18 attributed the current to a window component of ICa, L, because it was blocked by 2 µmol/L nifedipine. The ionic selectivity was not examined; this information may have separated Ist from ICa, L. DiFrancesco9 observed a nitrendipine- and Ni2+ (100 µmol/L)-sensitive background component, positive to -45 to -50 mV. On hyperpolarization from holding potential of -35 to -45 or -55 mV, the current shifted in the outward direction (negative slope) by 10 to 20 pA. This negative slope in the I-V relation disappeared after administration of nitrendipine. Again, the current was attributed to the ICa, L window component. However, if the liquid junction potential of the pipette solution10 is subtracted, the corrected activation threshold of -55 to -60 mV is close to the voltage range for attraction of Ist. However, no current similar to Ist was described in the recent study by Verheijck et al.10
| Dissection of Ist From the Whole-Cell Current |
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The conductance sequence of Ist for monovalent cations was determined to be Na+>Li+>K+=Cs+ by totally replacing external Na+.21 Ist is different from the Na+-dependent background current, which is recorded in the presence of Ca2+ antagonists and shows a different ion selectivity (K+>Cs+>Na+>Li+).22
| Current Density and Kinetics of Ist |
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The relationship between Ist density in primary as opposed to follower pacemaker cells has not been examined, because no clear criteria are available to distinguish the true pacemaker cells from follower cells after dissociating myocytes. Even when cell dissociation is started using a very small tissue segment, dissected from the leading pacemaker site within the SA node, a variety of cell types are found. In the rabbit and guinea pig SA node, most cells with Ist also express If.13 14
If Ist has no inactivation gate, Ist will continuously flow at a holding potential of -40 mV and can be deactivated on hyperpolarization. This should result in an outward current jump on hyperpolarization, provided that all currents other than Ist are appropriately blocked. However, no such outward jump is observed. The first study describing Ist13 addressed this question and demonstrated very slow inactivation; a 5-second pulse to -10 mV largely inactivated Ist, which recovered with a time constant of 1.36±0.4 seconds at a holding potential of -80 mV. Because this slow inactivation was more apparent when the Ca2+ current ICa, L was intact, Ca2+-mediated inactivation was suggested.
| Single-Channel Recordings |
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3.3 pA)
and L-type Ca2+ channels (9.6±0.32 pA at -60 mV
in the absence of divalent cations). The average unitary conductance of
sustained inward current (SIC) was 13.3 pS and showed a reversal
potential at
+13 mV. SIC was seen infrequently unless Bay-K8644 was
included in the pipette solution. Bath application of
nicardipine abolished SIC, and SIC was observed only in
spontaneously beating SA node cells. In the ensemble average, the SIC
activation occurred over a voltage range encompassing most of the slow
diastolic depolarization (>-70 mV). Cumulative histograms
for both open and closed times were composed of 2 exponential
components. The nicardipine sensitivity, bursting
behavior, and voltage-dependent gating of SIC are similar to in cardiac
L-type Ca2+ channel. However, their latency to
the first opening was 2 orders of magnitude longer than in L-type
Ca2+ channels. Although the kinetic
analysis is not completed, the presence of a new channel
underlying Ist is suggested by
single-channel recordings. | Ist During the Slow Diastolic Depolarization |
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-40 mV)
is attributable to Ist. Second, the
reversal potential is +18 mV according to both the single channel (+10
to 20 mV) and the whole-cell Ist obtained
in the 0.1 mmol/L
[Ca2+]o solution. Third,
the same formalism as ICa, L is applicable
to Ist.
![]() | (1) |
d,
ßd,
f, and
ßf
(sec-1) was adjusted to
simulate the experimental record.
![]() | (2) |
![]() | (3) |
![]() | (4) |
![]() | (5) |
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Panel B of the Figure
illustrates the time course and magnitude
of Ist during spontaneous action
potentials, sampled at 2 kHz. Gating parameters of
Ist were calculated bit by bit during each
sampling interval at the voltage of individual sample points using the
above equations. The amplitude of Ist
approaches zero at the overshoot, which is nearly equal to the reversal
potential of Ist. During the early phase of
repolarization, the driving force for Ist
becomes larger, and finally near the maximum diastolic
potential the channel is largely deactivated. During
diastole, the gradual increase in amplitude is due to the
time-dependent increase in the activation parameter
d. The action potential clamp experiment in SA node cells
revealed a D600-sensitive inward current component of -10 to -20 pA
during the diastolic period.23 The
authors attributed this current to ICa, L,
but part of this component might be due to
Ist.
The activation of Ist and gradual depolarization constitute a positive feedback loop during diastole to drive slow diastolic depolarization. The same mechanism is suggested for ICa, L in rabbits.10 The contribution of tetrodotoxin-sensitive Na+ current to spontaneous activity in newborn rabbit SA node cells is also due to a positive feedback.24 These effects are in contrast to the self-limiting process of voltage-dependent deactivation of IK during diastole. If is activated by hyperpolarization but not by depolarization.
The successful reconstruction of SA node action potentials by various types of computer models,4 5 6 7 8 without including Ist, indicates that the spontaneous activity can be generated by an appropriate but variable combination of time- and voltage-dependent currents. Furthermore, the amplitudes or kinetics of individual currents are not necessarily identical in different types of models. However, the kinetic characteristic for a given current system should confer a unique and important role to that current system in generating the pacemaker activity. Because the voltage-dependent kinetics are totally different among ICa, L, Ist, If, and IKr, they may take qualitatively different roles. To clarify the role specific to Ist, it is necessary to construct a mathematical model that includes Ist.
| Acknowledgments |
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Received February 2, 2000; accepted May 26, 2000.
| References |
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