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Am J Physiol Heart Circ Physiol 276: H1295-H1304, 1999;
0363-6135/99 $5.00
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Vol. 276, Issue 4, H1295-H1304, April 1999

Heterogeneity of 4-aminopyridine-sensitive current in rabbit sinoatrial node cells

Haruo Honjo1, Ming Lei2, Mark R. Boyett2, and Itsuo Kodama3

Departments of 1 Humoral Regulation and 3 Circulation, Research Institute of Environmental Medicine, Nagoya University, Nagoya 464-8601, Japan; and 2 Department of Physiology, University of Leeds, Leeds LS2 9JT, United Kingdom


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The electrophysiological properties of sinoatrial (SA) node pacemaker cells vary in different regions of the node. In this study, we have investigated variation of the 4-aminopyridine (4-AP)-sensitive current as a function of the size (as measured by the cell capacitance) of SA node cells to elucidate the ionic mechanisms. The 10 mM 4-AP-sensitive current recorded from rabbit SA node cells was composed of transient and sustained components (Itrans and Isus, respectively). The activation and inactivation properties [activation: membrane potential at which conductance is half-maximally activated (Vh) = 19.3 mV, slope factor (k) = 15.0 mV; inactivation: Vh = -31.5 mV, k = 7.2 mV] as well as the density of Itrans (9.0 pA/pF on average at +50 mV) were independent of cell capacitance. In contrast, the density of Isus (0.97 pA/pF on average at +50 mV) was greater in larger cells, giving rise to a significant correlation with cell capacitance. The greater density of Isus in larger cells (presumably from the periphery) can explain the shorter action potential in the periphery of the SA node compared with that in the center. Thus variation of the 4-AP-sensitive current may be involved in regional differences in repolarization within the SA node.

electrophysiology; patch clamp; transient outward current; regional difference


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

PREVIOUS HISTOLOGICAL and electrophysiological studies have shown that the sinoatrial (SA) node is structurally and functionally heterogeneous (for review, see Ref. 29). In the center of the node (normally the leading pacemaker site), the cells are small and have "empty" cytoplasm with relatively few organelles and poorly organized myofilaments, whereas, in the periphery of the node near the crista terminalis, the cells are larger and more densely packed with mitochondria and well-organized myofilaments (4, 35). In the center of the SA node, action potentials are longer, the maximum diastolic potential is less negative, the upstroke velocity is lower, and the intrinsic pacemaker activity is slower than in the periphery (31, 32, 39, 40). We previously reported that the electrical activity of single pacemaker cells isolated from the rabbit SA node shows a similar heterogeneity (27): in small SA node cells (presumably from the center of the SA node), the action potential upstroke is slower, the diastolic and take-off potentials are more positive, and the pacemaker activity is slower than in large cells (presumably from the periphery). This work suggests that variations in membrane properties may underlie the regional differences in the electrical activity within the SA node. The more positive take-off potential, the slower action potential upstroke, and the slower pacemaker activity, in part at least, can be explained by lower densities of the tetrodotoxin (TTX)-sensitive Na+ current and the hyperpolarization-activated current (If) in smaller cells.

As mentioned above, the action potential in the center of the SA node is longer than that in the periphery. We recently showed (5) that this is part of a downward gradient in action potential duration along the conduction pathway in and around the SA node. This downward gradient in action potential duration is similar to, but more marked than, that elsewhere in the heart, e.g., from the ventricular subendocardium to the ventricular subepicardium (2, 34), and its function, as elsewhere in the heart, is presumably to help prevent reentry. Transient outward K+ current (Ito) may be responsible for the gradient in action potential duration from the center to the periphery of the SA node, because in the presence of 4-aminopyridine (4-AP; blocker of Ito) the gradient is reduced and no longer significant (7). The presence of 4-AP-sensitive Ito has been reported by various investigators in rabbit SA node pacemaker cells (15, 24, 25, 30, 37), as well as in the remaining part of the heart (for review, see Ref. 9). The present study was undertaken to investigate possible variation in the 4-AP-sensitive current (I4-AP) as a function of SA node cell size to understand the mechanisms underlying the regional differences in action potential duration within the SA node. The results obtained suggest that a lower density of the sustained component of I4-AP in smaller cells can explain the longer action potential in the center of the SA node. Thus variation of I4-AP may be involved in regional differences in repolarization in the SA node.


    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Single SA node pacemaker cells. Single SA node cells were enzymatically isolated from adult rabbit hearts by methods similar to those described previously (27, 28, 47, 48). In brief, a New Zealand White rabbit (6-10 wk old) weighing 1.0-1.5 kg was anesthetized with an intravenous injection of pentobarbital sodium (30-40 mg/kg). Heparin (300-1,000 U/kg) was injected at the same time. The chest was opened, and the heart was rapidly excised into oxygenated Tyrode solution at 32°C. The SA node region was then isolated and cut into several strips (0.5-1.0 mm in width) perpendicular to the crista terminalis. Atrial muscle and fat tissue on the epicardial surface were carefully removed under a dissecting microscope. The SA node tissue strips were digested with an enzyme solution containing collagenase, elastase, and protease for 40 min at 36°C after a brief treatment with Ca2+-free Tyrode solution for 5-10 min. The digested tissue specimens were placed in high K+, low Cl- solution (Kraft-Brühe, K-B) and gently triturated to produce a cell suspension. The cells were kept at 4°C before they were used experimentally. In the present study, only spindle-shaped cells showing regular spontaneous activity were used. The morphological and electrophysiological characteristics of the cells were similar to the characteristics of the cells used in our previous studies (27, 28, 47, 48); these cells were spindle shaped with no obvious or faint striations, showed regular spontaneous beating when perfused with normal Tyrode solution, and exhibited If during hyperpolarizing voltage-clamp pulses (not shown) as well as a high input resistance (1.6-3.0 GOmega ) at a holding potential of -60 mV. These characteristics suggest that these cells are SA node pacemaker cells (29).

Electrophysiological measurements. Membrane currents were recorded using the whole cell patch-clamp technique at room temperature (24-26°C). Patch pipettes with a resistance of 2-4 MOmega were used. The pipette and cell capacitance (Cm) and the series resistance (>80%) were electronically compensated, and the current signal was filtered by a low-pass Bessel filter with a cut-off frequency of 10 kHz (-3 dB). Cm, which is proportional to the cell surface area, was obtained from the capacitance compensation control of the amplifier after the whole cell capacity current (in response to ±5-mV voltage-clamp pulses at -60 mV) had been eliminated. The accuracy of these values was checked by integrating the area of the uncompensated capacity current and fitting an exponential function to the decay of the uncompensated capacity current. Cm of the SA node cells used in the present study ranged from 20.3 to 66.0 pF (mean ± SE = 44.2 ± 2.2 pF, n = 34). I4-AP was obtained by subtracting currents in the presence of 4-AP from control currents before 4-AP application. Ten millimolar 4-AP was usually used, but one millimolar 4-AP was used in some experiments. I4-AP had transient and sustained components (Itrans and Isus, respectively; see RESULTS): I4-AP at the end of 200-ms depolarizing clamp pulses was defined as Isus, and the difference of I4-AP at its peak and at the end of the pulse was defined as Itrans. Because Itrans did not reach steady state at the end of 200-ms pulses (see Fig. 6), Isus contains a small fraction of the time-dependent component of I4-AP. In these experiments, 3 µM TTX and 300 µM Cd2+ were added to the perfusate throughout the experiments to block Na+ current, L- and T-type Ca2+ currents, and Ca2+-activated transient outward current (if present). In some experiments, 1 µM nifedipine (Sigma) was used instead of 300 µM Cd2+ to block L-type Ca2+ current. Membrane currents and membrane potential were recorded with an Axopatch 1C amplifier (Axon Instruments) and acquired on a personal computer using a CED 1401 and Signal Averager or Voltage Clamp Software (Cambridge Electronic Design) at a sampling rate of 4-5 kHz for later analysis.

Solutions and drugs. Normal Tyrode solution contained (in mM) 137 NaCl, 5.4 KCl, 1.8 CaCl2, 0.5 MgCl2, 0.3 NaH2PO4, 5 HEPES, and 10 glucose (pH 7.4). Ca2+-free Tyrode solution was made by simply omitting CaCl2 from the normal Tyrode solution. Enzyme solution consisted of Ca2+-free Tyrode solution plus collagenase (350-400 U/ml, Yakult), elastase (12-20 U/ml, type IIA, Sigma), and protease (0.5 U/ml, type XIV, Sigma). K-B solution contained (in mM) 20 taurine, 70 l-glutamic acid, 25 KCl, 10 KH2PO4, 3 MgCl2, 0.5 EGTA, 10 HEPES, and 10 glucose (pH 7.4). The pipette solution contained (in mM) 140 KCl, 5 MgATP, 0.4 Na2GTP, 11 HEPES, 1 CaCl2, and 11 EGTA (pCa 8, pH 7.2). The liquid junction potential between normal Tyrode solution and the pipette solution was measured experimentally (-4 mV) and was corrected. A stock solution of 1 M 4-AP was prepared in double-distilled water, and the pH was titrated to 7.4 with HCl. This stock solution was added to the Tyrode solution to give a final concentration of 4-AP.

Statistics. Data are presented as means ± SE (n = number of cells). All curve fitting was performed by a nonlinear least-squares method (see Figs. 4, 5C, and 6A) using Fig.P software (Fig.P Software). Statistical analysis was performed by a linear regression analysis (see Fig. 3) and Student's unpaired t-test (see Fig. 6, B and C). Values of P < 0.05 were considered to indicate significance.


    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

I4-AP in SA node cells. In the majority of SA node cells studied (31 of 34 cells: Cm 20.3-66.0 pF, mean ± SE = 44.2 ± 2.5 pF) membrane depolarization from a holding potential of -60 or -80 mV activated transient outward current. Figure 1 shows representative records of membrane current in response to 200-ms depolarizing voltage-clamp pulses from -60 mV before (Fig. 1A, second panel) and after (Fig. 1A, third panel) the application of 10 mM 4-AP. Under control conditions in the absence of 4-AP, the depolarization caused a rapid activation of outward current that declined during the 200-ms pulse. Application of 4-AP resulted in a reduction of the outward current mainly at the beginning of the depolarizing pulse. After the application of 10 mM 4-AP, however, a small, rapidly decreasing transient outward current remained. A higher concentration (20 mM) of 4-AP did not abolish this small transient outward current. The nature of the remaining current was not investigated in detail in the present study, but it is possible that an outward tail of If at positive potentials could be responsible for a part of this current. I4-AP was obtained by subtraction (Fig. 1A, fourth panel). There were two components of I4-AP; it showed a transient component (Itrans) with rapid activation and inactivation and a small sustained component (Isus) at the end of the 200-ms pulse. The inactivation kinetics of Itrans were faster at more positive potentials. Figure 1B shows current-voltage relationships of Itrans and Isus as well as I4-AP. The threshold potential for activation was roughly the same (-40 mV) for Itrans and Isus (Fig. 1B).


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Fig. 1.   4-Aminopyridine (4-AP)-sensitive outward current (I4-AP) in a sinoatrial (SA) node cell. A: calculation of I4-AP. Currents were recorded during 200-ms depolarizing pulses to potentials from -50 to +50 mV (in 20-mV increments) from a holding potential of 60 mV. First panel: voltage-clamp protocol. Second panel: superimposed records of membrane current under control conditions [3 µM tetrodotoxin (TTX) and 300 µM Cd2+ present]. Third panel: superimposed records of membrane current after addition of 10 mM 4-AP. Fourth panel, superimposed records of I4-AP calculated by subtracting currents after addition of 4-AP from those under control conditions. Arrowheads show zero-current level. B: current-voltage relationships of peak I4-AP and transient (Itrans) and sustained (Isus) components of I4AP. Cell capacitance (Cm), 54.3 pF.

I4-AP activated by depolarization from a holding potential of -80 mV was essentially the same as that from the holding potential of -60 mV. However, there was a marked activation of If at a holding potential of -80 mV. A decrease of I4-AP as a result of rundown of the channel was minimal and negligible (<2% in 3 min). One millimolar (rather than 10 mM) I4-AP was also made up of transient and sustained components, and its peak amplitude was 59.3 ± 4.1 (-10 mV), 62.8 ± 2.9 (at +20 mV), and 65.0 ± 3.9% (+50 mV) (n = 4) of that of 10 mM I4-AP.

Among 34 SA node cells tested, 31 cells showed I4-AP with Itrans and Isus components as described above. In the remaining three cells (Cm 40.8, 43.0, and 63.6 pF), however, there was no substantial Itrans in I4-AP; in these cells membrane depolarization activated only Isus.

Heterogeneity of I4-AP. Figure 2 compares I4-AP in SA node cells of different sizes. Figure 2A illustrates superimposed records of I4-AP in response to depolarizing pulses to various potentials from a holding potential of -60 mV from small, medium-sized, and large SA node cells (Cm 20.3, 34.5, and 63.4 pF, respectively). The current-voltage relationships of Itrans and Isus are shown in Fig. 2, B and C, respectively. The amplitude of peak I4-AP and Itrans increased with the increase of cell capacitance (Fig. 2, A and B). The amplitude of Isus at the end of 200-ms depolarizing pulses was minimal in the small cell (Cm 20.3 pF) but increased with the increase of Cm (Fig. 2, A and C). The threshold potential for activation of Itrans was similar in the three cells (Fig. 2B), as was that of Isus (Fig. 2C).


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Fig. 2.   I4-AP in SA node cells of different sizes. A: superimposed records of I4-AP during 200-ms pulses to potentials from -50 to +50 mV (in 20-mV increments) from a holding potential of -60 mV in a small (Cm 20.3 pF; a), a medium-sized (Cm 34.5 pF; b), and a large (Cm 63.4 pF; c) cell. Arrowheads show zero-current level. B: current-voltage relationships of Itrans. C: current-voltage relationships of Isus.

Figure 3 shows the relationship between the density (current normalized by Cm) of I4-AP and the size (as measured by Cm) of 19 SA node cells isolated from five rabbits. The values of Cm ranged from 20.3 to 65.4 pF (mean ± SE = 42.0 ± 3.1 pF, n = 19). Figure 3A shows that there is no significant correlation between the density of Itrans during a 200-ms depolarization to +50 mV and Cm (r = -0.26, P > 0.1, n = 19). In contrast, there is a significant correlation between the density of Isus at the end of the 200-ms depolarization to +50 mV and Cm (r = 0.75, P < 0.0005, n = 19; Fig. 3B); the density of Isus was greater in larger SA node cells. Total charge movement by I4-AP per unit Cm was also compared in SA node cells of different sizes. Charge movement was calculated in each cell by integrating I4-AP during a 200-ms depolarizing voltage-clamp pulse to +50 mV. The normalized charge movement carried by I4-AP was greater in larger cells; there is a significant correlation between the normalized charge movement and Cm (r = 0.54, P < 0.02, n = 19, Fig. 3C). These results suggest that I4-AP may play a greater role in larger cells.


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Fig. 3.   Correlation of I4-AP and cell size. A: density of Itrans plotted against Cm. B: density of Isus plotted against Cm. C: charge carried by I4-AP normalized to Cm plotted against Cm. In A-C, each point was obtained from a different cell. I4-AP was measured during a 200-ms pulse to +50 mV from holding potential of -60 mV, and charge movement was calculated by integrating I4-AP during a clamp pulse. Data are fitted with straight lines; results of linear regressions are shown.

Voltage dependence of activation and inactivation of I4-AP. Figure 4 shows activation curves for I4-AP. In these experiments I4-AP was recorded in the presence of 300 µM Cd2+ to block Ca2+ current, and it is reported in rat ventricular cells that extracellular divalent cations, including Cd2+, cause a rightward shift of voltage dependence of Ito (1, 19). The effect of 300 µM Cd2+ on I4-AP in rabbit SA node cells was evaluated first. In these experiments, 1 µM nifedipine, instead of Cd2+, was used to block L-type Ca2+ current. The results obtained from rabbit SA node cells were inconsistent with those from rat ventricular cells: voltage dependence of I4-AP activation was similar both in the presence (n = 6) and in the absence (n = 4) of Cd2+. Therefore, quantitative analysis was performed on data obtained in the presence of 300 µM Cd2+.


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Fig. 4.   Activation curves in SA node cells of different sizes. A: activation curves for I4-AP in small (Cm 20.3 pF), medium (Cm 34.5 pF), and large (Cm 63.4 pF) cells. Data were obtained from experiments shown in Fig. 2A. From peak I4-AP during a pulse, chord conductance (G) was calculated and is plotted against membrane potential. Data are fitted with Boltzmann equation, with membrane potential at which G is half-maximally activated (Vh) of 19.7 mV and slope factor (k) of 16.4 mV for small cell, (Vh) of 19.1 mV and k of 15.2 mV for medium-sized cell, and Vh of 21.0 mV and k of 15.3 mV for large cell. B: normalized activation curves for 7 cells. Maximum G (Gmax) was obtained from Boltzmann equation. Normalized G (G/Gmax) is plotted against potential. Data are fitted with Boltzmann equation with Vh of 19.3 mV and k of 15.0 mV. In A and B, different symbols are used for different cells. See text for further explanation.

The chord conductance (G) was calculated from the peak of I4-AP during 200-ms depolarizing voltage-clamp pulses, by assuming that the reversal potential is -80 mV, and plotted against the test potential (Fig. 4A). In Fig. 4A, data obtained from three SA node cells of different sizes (Cm 20.3, 34.5, and 63.4 pF) are shown. Each set of data was fitted by the Boltzmann equation
<IT>G</IT> = <IT>G</IT><SUB>max</SUB>/[1 + exp(<IT>V</IT><SUB>h</SUB> − <IT>V</IT>)/<IT>k</IT>]
where Gmax is the estimated maximum G by fitting, V is the membrane potential, Vh is the potential at which the conductance is half-maximally activated, and k is the slope factor describing the steepness of the curve. The values of Vh and k were 19.7 and 16.4 mV in the small cell, 19.1 and 15.2 mV in the medium-sized cell, and 21.0 and 15.3 mV in the large cell, suggesting no variation of Vh and k with cell size. In Fig. 4B, the normalized conductance (G/Gmax) is plotted against the test potential. Data obtained from seven SA node cells (Cm 20.3-63.4 pF; mean ± SE = 40.9 ± 5.6 pF) are shown. The normalized data from cells of different size are similar, and there is no significant cell size-dependent variation in the activation curve. The combined data were fitted with the Boltzmann curve with Vh of 19.3 mV and k of 15.0 mV. The threshold potential for activation was around -40 mV (Fig. 4B).

The voltage dependence of steady-state inactivation of I4-AP was examined with a double-pulse protocol: a conditioning 1-s prepulse to various potential levels (from -80 to +10 mV in 10-mV steps) was followed by a test depolarizing pulse to +50 mV from a holding potential of -60 mV (Fig. 5). Figure 5A shows superimposed traces of I4-AP during the test pulse obtained from three SA node cells of different sizes (Cm 23.6, 47.1, and 63.4 pF). The peak value of the outward current during the test pulse is plotted against the prepulse potential in Fig. 5B. In all three cells I4-AP during the test pulse declined as the potential during the prepulse was made more positive (Fig. 5, A and B). However, in the large SA node cell (Cm 63.4 pF), there was a substantial sustained outward current during the test pulse that persisted even when the potential during the prepulse was increased to +10 mV (Fig. 5, A and B). The density of this sustained current was lower in the medium-sized cell (Cm 47.1 pF) and minimal in the small cell (Cm 23.6 pF). This is consistent with the result that the density of Isus was greater in larger SA node cells (Fig. 3B). The inactivating component of I4-AP during the test pulse was calculated by subtracting the noninactivating component from the total I4-AP during the test pulse (Fig. 5B). The inactivating component of I4-AP was normalized by the maximal current amplitude in each cell and plotted against the prepulse potential (Fig. 5C). In Fig. 5C, data were obtained from six SA node cells of different sizes (Cm 23.6-63.4 pF; mean ± SE = 44.0 ± 5.5 pF). There was no significant cell size-dependent difference in the steady-state inactivation curve, although a small variation was observed. Inactivation was fully removed at potentials more negative than -70 mV, and the current was half-maximally inactivated around -30 mV. The combined data were fitted by the Boltzmann equation
<IT>I</IT>/<IT>I</IT><SUB>max</SUB> = 1/[1 + exp(<IT>V</IT> − <IT>V</IT><SUB>h</SUB>)/<IT>k</IT>]
with Vh of -31.6 mV and k of 7.2 mV.


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Fig. 5.   Steady-state inactivation curves in SA node cells of different sizes. A: measurement of voltage dependence of inactivation. Top, protocol. A 1-s conditioning pulse to various potentials (from -80 to +10 mV in 10-mV increments) was followed after a 10-ms interval by a 200-ms test pulse to +50 mV. Holding potential was -60 mV. Bottom, superimposed I4-AP during test pulse after set of conditioning pulses in small (Cm 23.6 pF; a), medium-sized (Cm 47.1 pF; b), and large (Cm 63.4 pF; c) cells. Arrowheads and dashed lines show zero-current level. B: peak I4-AP during test pulse plotted against conditioning pulse potential in cells a-c. In the case of cell c, current components that could and could not be inactivated during conditioning pulse are shown. C: inactivation curves for 6 cells. Curves were produced from data like that in B by normalizing inactivating component of current (Itrans). Different symbols are used for different cells. Data are fitted with Boltzmann equation, with Vh of -31.5 mV and k of 7.2 mV.

Inactivation kinetics of I4-AP. The time course of the decline of I4-AP during depolarizing pulses was quantitatively analyzed in eight SA node cells (Fig. 6). The time-dependent decay of I4-AP at membrane potentials more positive than +10 mV was best fitted by a double-exponential function
<IT>I</IT>(<IT>t</IT>) = <IT>A</IT><SUB>fast</SUB> exp(−<IT>t</IT>/&tgr;<SUB>fast</SUB>) + <IT>A</IT><SUB>slow</SUB> exp(−<IT>t</IT>/&tgr;<SUB>slow</SUB>) + <IT>A</IT><SUB>0</SUB>
where Afast and tau fast are the initial amplitude and time constant of the "fast" phase of inactivation, and Aslow and tau slow are the corresponding parameters for the "slow" phase. A0 is a time-independent component. An example is shown in Fig. 6A; the top panel of Fig. 6A shows I4-AP during a depolarizing pulse to +40 mV and the bottom panel shows a semilogarithmic plot of the current during the pulse. The filled circles show the current minus the asymptote (i.e., A0). Most of the points fall along a straight line with a tau  of 91.4 ms. This represents the slow phase of inactivation. However, at the start of the pulse, the filled circles deviate from the straight line. The difference between the filled circles and the line is plotted by the open circles. The open circles fall along a straight line with a tau  of 6.6 ms. This represents the fast phase of inactivation.


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Fig. 6.   Kinetics of inactivation of I4-AP. A: 2 phases of inactivation of I4-AP. Top, voltage-clamp pulse. Middle, I4-AP during pulse. Arrowhead shows zero-current level. Solid line indicates best fit by a double-exponential function. Bottom, semilogarithmic plot of decline in I4-AP during pulse as a result of inactivation. B and C: voltage dependence of time constant of fast phase of inactivation (tau fast; B) and slow phase of inactivation (tau slow; C). Means ± SE obtained from a group of small cells with Cm of <40 pF (mean ± SE = 30.5 ± 3.5 pF, n = 4) and a group of large cells with Cm of >40 pF (Cm mean ± SE = 50.2 ± 4.0 pF, n = 4) are shown.

Both tau fast and tau slow show appreciable voltage dependence at potentials between +10 and +60 mV (Fig. 6, B and C). The average tau fast and tau slow values at +20 to +60 mV were in the range of 7-9 ms and 60-90 ms, respectively, and the values were somewhat longer (~14 and ~140 ms, respectively) at +10 mV (Fig. 6, B and C). The percentage of fast inactivation was almost constant (0.65 to 0.75) at +10 to +60 mV. Figure 6, B and C, also shows that there was no significant difference in tau fast and tau slow between a group of small cells with a Cm of <40 pF (Cm 30.5 ± 3.5 pF, n = 4) and a group of large cells with a Cm of >40 pF (Cm 50.2 ± 4.0 pF, n = 4) at potentials ranging from +10 to +60 mV.


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The present study demonstrates that 4-AP-sensitive Ito exists in the majority (>90%) of rabbit SA node pacemaker cells. Although the presence of Ito in the SA node has been commented on by other investigators (15, 24, 25, 30, 37), the percentage of cells showing typical I4-AP in the present study (>90%) was much higher than in previous reports (15, 24, 25). Furthermore, Giles et al. (24, 25) reported that Ito was not recorded from rabbit SA node cells unless the cells were isolated from the most peripheral region of the node. In contrast, in the present study 4-AP-sensitive Ito could be recorded not only from large cells, which are presumably derived from a transitional or the peripheral region of the node, but also from small cells, which are presumably from the center of the node (27). There is no clear explanation for the discrepancy between previous reports and our present data, but it is possible that the presence of Ito in SA node cells was underestimated in previous studies, because in these studies 4-AP-sensitive current was not routinely recorded. In cell culture, Nathan (37) identified two morphologically distinct types of cells from the rabbit SA node (types I and II); the electrophysiological characteristics suggest that the type I cells possibly originated from the center and the type II cells were from the periphery. Both types of cells showed typical Ito (37).

The nature of I4-AP in SA node cells. The present study showed that I4-AP in most SA node cells is made up of two components, a component showing time-dependent inactivation (Itrans) and a sustained component (Isus). Ito and Ono (30) also reported the presence of time-dependent and sustained I4-AP in rabbit SA node cells. In the present study, in a small fraction of cells, there was no Itrans and only Isus existed. It is not known whether the two components are inactivating and noninactivating phases of current through a single type of 4-AP-sensitive channel or are separate currents through two types of 4-AP-sensitive channel.

The voltage dependence of activation and inactivation as well as inactivation kinetics of Itrans in SA node cells are similar to those of Ito in other types of cardiac cells (see below). Furthermore, in the present study 1 mM 4-AP blocked ~60-65% of I4-AP in rabbit SA node cells. Typical Ito in atrial and ventricular cells is reported to be blocked by 4-AP with an EC50 of 0.2-0.5 mM (12, 42), and therefore, the 4-AP dose dependence of I4-AP in SA node cells is comparable to that of Ito in atrial and ventricular cells. Kv4.2 and Kv4.3 channels are probably responsible for Ito (12, 17, 22), although it has also been suggested that Kv1.4 is responsible. We have recently cloned a Kv4.2 channel from a rabbit SA node cDNA library, and the channel when expressed in Xenopus oocytes is similar (but not identical) to I4-AP in the rabbit SA node (13). For example, for the cloned channel, Vh = +15 mV and k = 7 mV for activation and Vh = -81 mV and k = 16 mV for inactivation (13) (see Table 1 for corresponding values for I4-AP in rabbit SA node cells from present study). The sensitivity of the cloned channel to 4-AP, quinidine, and flecainide is less than that of the Ito in rabbit SA node cells (13, 33).

                              
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Table 1.   Properties of Ito in cardiac myocytes

Isus may be similar to the ultrarapidly activating delayed rectifier K+ currents described (IK,ur) in atrial cells of various species including rats (8), humans (46), and dogs (50). All these currents show rapid activation and slow and limited inactivation and can be distinguished from the rapid and slow delayed rectifier K+ currents (IK,r and IK,s). The rat atrial current is inhibited by 4-AP with an EC50 of ~600 µM (8), and the human and canine atrial currents are more sensitive to 4-AP with an EC50 of ~50 µM (46) and ~5 µM (50), respectively. Several types of cloned K+ channel may be responsible for these currents: Kv1.5 and possibly Kv3.1 channels for the human and canine IK,ur (20, 21, 50) and Kv1.2 for the rat atrial current (41). It is not known whether these K+ channels are expressed in rabbit SA node cells, but we have recently shown (18) by immunolabeling that Kv1.5 channels are present in the guinea pig SA node. Nevertheless, further electrophysiology, pharmacology, and molecular biology studies will be required to clarify the nature of this current, and it remains a possibility that Isus is the noninactivating component of Ito.

In the present study, a relatively high concentration (10 mM) of 4-AP was used, and this concentration of 4-AP has been shown to affect various K+ currents other than Ito and IK,ur; 4-AP can block the ATP-sensitive K+ current (IK,ATP) and the inwardly rectifying K+ current (IK1) and activate the muscarinic K+ current (IK,ACh) (14, 38, 44). In the present study, however, 10 mM 4-AP had no substantial effect on the holding current at -60 mV (at which potential the 3 currents, if present, should be substantial), and this suggests that IK,ATP, IK1, and IK,ACh (if present) were not being affected. Furthermore, IK,ATP should not be present under normal conditions in the SA node, and IK1 is absent from the SA node (29).

In some cells (see, e.g., Fig. 6A), there was an outward tail of I4-AP current after a pulse. Theoretically, this could be the result of block of IK,r or IK,s by 4-AP. However, such outward tails of I4-AP were not seen in the majority of cells (see, e.g., Figs. 1A, fourth panel, and 2A). Furthermore, it is unlikely that IK,r was substantially inhibited by 4-AP, because the current-voltage relationship of Isus (IK,r if inhibited by 4-AP would contribute to Isus) did not show any evidence of inward rectification at positive potentials (characteristic of IK,r; Refs. 30, 45) in the present study (Figs. 1B and 2C). IK,s is a small current in the rabbit SA node; furthermore, it activates over a time course of seconds, and, therefore, even if it is blocked by 4-AP (whether it does is not known) it would not be expected to make a major contribution to I4-AP during a 200-ms pulse typically used in the present study.

Under control conditions, outward tail current (residual Ito, IK,r, IK,s) is expected after a depolarizing pulse. However, under control conditions, in all cells, there was an inward tail current after a pulse (see, e.g., Fig. 1A). The inward tails could be the result of activation of inward currents in response to repolarization (e.g., inward Na+/Ca2+ exchange current). Alternatively, the inward tails could be explained by an outward current with a reversal potential of less than -60 mV. However, the reversal potential of Ito, at least, was more negative than -60 mV (data not shown).

4-AP-sensitive Ito in SA node cells compared with that in other cardiac tissues. The inactivation of I4-AP in rabbit SA node cells during depolarizing pulses was best approximated by a double-exponential function. Inactivation of Ito in other cardiac tissues has also been reported to be best fit by a double-exponential function in rabbit atrial and ventricular cells as well as atrioventricular node (11, 26, 36, 49). The inactivation kinetics of I4-AP in SA node cells are comparable to those reported for rabbit atrial and ventricular cells (26, 49) as well as rat and ferret ventricular cells (3, 10). However, faster or slower inactivation has also been reported in rabbit atrial cells (11, 49) (Table 1). The transient component of I4-AP (Itrans) in rabbit SA node cells was half-maximally inactivated at -31.5 mV (with a slope factor of 7.2 mV) in the present study (Table 1). These values are similar to those reported for Ito in rabbit atrial and crista terminalis cells (11, 24, 49) as well as rabbit, rat, and canine ventricular cells (3, 26, 34) (Table 1). In contrast, more positive Vh values (approximately -14 mV) have been reported for Ito in human atrial (42) and ferret ventricular (10) cells (Table 1). The activation curve for I4-AP obtained from SA node cells in the present study showed a weaker voltage dependence (k 15.0 mV) and a more positive midpoint (Vh +19.3 mV) than that for Ito in other cardiac tissues (11, 24, 42) with the exception of rabbit and ferret ventricular cells (10, 26) (Table 1). This apparent difference could be the result of the different methods used to determine the activation parameter; in the present study it was calculated as the chord conductance from peak I4-AP during depolarizing test pulses, whereas in other studies it was obtained from the amplitude of tail current in response to repolarization after depolarizing test pulses. An apparent more shallow voltage dependence in association with an apparent more positive Vh can arise when using the chord conductance method if the instantaneous current-voltage relationship is nonlinear (43).

Role of I4-AP in action potential in SA node. In atrial, Purkinje, and ventricular cells, block of Ito by 4-AP slows the initial phase of repolarization (phase 1), abolishes the notch, elevates the plateau, and prolongs the action potential (16, 23, 24, 26). In canine atrial cells, block of IK,ur by 4-AP results in a prolongation of the action potential (49). We have studied the effects of 4-AP in small ball-like preparations of tissue from different regions of the rabbit SA node (6, 7). In small balls of tissue from the periphery of the SA node, 4-AP had all of these actions: it slowed the initial phase of repolarization and abolished the notch if present, elevated the plateau, and prolonged the action potential (6, 7). In small balls of tissue from the center of the SA node, the effects of 4-AP were smaller: a smaller elevation of the plateau and a smaller increase in action potential duration (in the center, the action potential does not have a notch) (6, 7). The dose dependence of the 4-AP-induced action potential prolongation in the small balls of tissue was similar to that of I4-AP in the present study and Ito in other studies (6, 7).

The greater effects of 4-AP on tissue from the periphery of the SA node than on tissue from the center can be explained by the results from the present study. In the periphery of the SA node the cells are larger than those in the center (4). In the present study, the density of Isus was greater in larger cells and the charge carried by I4-AP normalized for Cm was greater in larger cells (Fig. 3). The role of I4-AP is expected, therefore, to be greater in the larger cells from the periphery of the SA node. There is a second reason why I4-AP is expected to play a more important role in the periphery of the SA node compared with the center. In the periphery of the SA node, the voltage-dependent inactivation of Itrans is expected to be less (because the diastolic potential is more negative in the periphery of the SA node), and thus greater Ito is expected to be activated during the action potential.

In conclusion, I4-AP is present in the majority of SA node cells but is less important in smaller cells as a result of a smaller density of the sustained component of I4-AP. The heterogeneity of I4-AP in SA node cells helps explain why the action potential is longer in the center of the SA node than in the periphery, a protective mechanism to help prevent reentry.


    ACKNOWLEDGEMENTS

This work was supported by the British Heart Foundation, the Ministry of Education, Science, and Culture of Japan, and the Japan Society for the Promotion of Science.


    FOOTNOTES

The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.

Address for reprint requests: H. Honjo, Dept. of Humoral Regulation, Research Institute of Environmental Medicine, Nagoya Univ., Nagoya 464-8601, Japan.

Received 14 May 1998; accepted in final form 3 December 1998.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

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