(Circulation. 1999;99:206-210.)
© 1999 American Heart Association, Inc.
Brief Rapid Communications |
From the Department of Cardiology (P.G.A.V., R.L.H.M.G.S., H.J.J.W., M.A.V), Cardiovascular Research Institute Maastricht (E.C.), Maastricht University, Netherlands, and the Laboratory of Experimental Cardiology, University of Leuven, Belgium (K.R.S.).
Correspondence to Paul G.A. Volders, MD, Department of Cardiology, Cardiovascular Research Institute Maastricht, Academic Hospital Maastricht, PO Box 5800, 6202 AZ, Maastricht, Netherlands. E-mail p.volders{at}cardio.azm.nl
| Abstract |
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Methods and ResultsSingle RV and LV M cells were used for microelectrode recordings and whole-cell voltage clamping. Action potentials showed deeper notches, shorter APDs at 50% and 95% of repolarization, and less prolongation on slowing of the pacing rate in RV than LV. ITO1 density was significantly larger in RV than LV, whereas steady-state inactivation and rate of recovery were similar. IKs tail currents, measured at -25 mV and insensitive to almokalant (2 µmol/L), were considerably larger in RV than LV. IKr, measured as almokalant-sensitive tail currents at -50 mV, and IK1 were not different in the 2 ventricles.
ConclusionsDifferences in K+ currents may well explain the interventricular heterogeneity of action potentials in M layers of the canine heart. These results contribute to a further phenotyping of the ventricular action potential under physiological conditions.
Key Words: action potential myocytes ions potassium arrhythmia
| Introduction |
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Only limited information is available on action potential and ionic differences in right ventricular (RV) versus left ventricular (LV) comparisons. A larger ITO1 in RV versus LV epicardial cells has been correlated with a larger notch in the former cell type.8 Because an interventricular comparison of K+ currents in M cells is lacking, we examined action potentials and the K+ currents ITO1, IKs, IKr, and IK1 in RV and LV M cells of the same adult canine hearts.
| Methods |
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30 minutes of collagenase perfusion, the epicardial
surface layer was removed from both wedges until a depth of
3 mm
was reached,4 7 and softened tissue samples were removed
by pipette from the M layer underneath while contamination with the
endocardium was avoided. Samples were gently agitated, filtered, and
washed. Isolated myocytes were stored at room temperature in standard
buffer solution.
The setup was built around an inverted microscope.10
Microelectrodes (standard glass) had resistances of 30 to 60 M
when
filled with 3.0 mol/L KCl. Intracellular pacing was done at various
cycle lengths (CLs). For the recording of ionic currents, we
used the whole-cell variant of the patch-clamp technique. Patch
pipettes (borosilicate glass) had resistances of 1.0 to 3.0 M
when
filled with internal solution. Experiments were performed at 37°C.
Cell capacitance, measured by hyperpolarizing steps from -60 mV, was
similar in RV (n=27) and LV (n=25) M cells, being 226±12 and 226±11
pF, respectively (P=NS). L-type Ca2+
current was blocked with nifedipine (5 µmol/L).
Na+ current was inactivated by 10-ms
prepulses to -45 mV. The voltage-clamp protocols are illustrated in
Figures 1
and 2
. ITO1
amplitudes were measured as peak amplitudes minus steady-state values
at the end of the test pulses (Vtest). For
IKr, we measured the tail currents on
repolarization to -50 mV sensitive to almokalant (2 µmol/L; a
specific IKr blocker).11
For IKs, we measured the
almokalant-insensitive tail currents on repolarization to -25 mV. For
IK1, we measured steady-state values at the
end of Vtest.
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The standard-buffer solution used for the experiments was composed of (in mmol/L) NaCl 145, KCl 4.0, CaCl2 1.8, MgCl2 1.0, NaH2PO4 1.0, glucose 11, HEPES 10, pH 7.4 with NaOH at 37°C. The patch-pipette solution contained (in mmol/L) potassium aspartate 125, KCl 20, MgCl2 1.0, MgATP 5, HEPES 5, EGTA 10, pH 7.2 with KOH.
Data are expressed as mean±SEM. Intergroup comparisons were made with the Student's t test for unpaired and paired data groups, after testing for the normality of distribution. Differences were considered significant if P<0.05.
| Results |
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Properties of ITO1
ITO1 activated at
Vtest
-20 mV in both ventricles, but
amplitudes were significantly larger in RV than LV at all
Vtest (Figures 1
and 2A
).
4-Aminopyridine (5 mmol/L) nearly completely
suppressed ITO1 in both cell types.
Inactivation during the Vtest was best fitted
with a single exponential function yielding similar time constants for
RV and LV. The voltage dependence of ITO1
steady-state inactivation (Figure 2B
) was well described by a
Boltzmann fit with half points (V0.5) of
-52±0.6 and -50±0.5 mV and slope factors of 6.8±0.6 and 4.5±0.5
mV in RV and LV, respectively (P=NS). Time-dependent
recovery from inactivation was not different between the
ventricles.
Properties of IKs and
IKr
IKs tail currents were evaluated on
repolarization to -25 mV with IKr blocked
by almokalant. Examples of current traces are shown in Figure 1
.
Pooled data are given in Figure 2C
. There was no saturation of
tail-current amplitudes. Voltage dependence of
IKs activation was similar for both cell
types, but density was significantly larger in RV (0.72±0.12 pA/pF)
than in LV (0.38±0.13 pA/pF) (P<0.05; depolarization to 50
mV). This difference persisted after increasing
IKs in K+-free
solution (0 [K+]O):
0.98±0.21 pA/pF in RV versus 0.58±0.17 pA/pF in LV. Deactivation
proved similar in RV and LV myocytes. Tail currents in 0
[K+]O were best fitted by
biexponential functions on repolarization to -10 to -40 mV and by
monoexponential functions on more negative
repolarizations (-50 to -80 mV). At -20 mV, time constants of the
fast and slow components were 228±25 and 1105±199 ms in RV (n=7) and
278±35 and 1486±269 ms in LV (n=6), respectively; at -60 mV,
monoexponential time constants were 99±16 in RV and
94±11 in LV (P=NS for all).
IKr was quantified as the
almokalant-sensitive tail-current portion measured by digital
subtraction at -50 mV in 4.0 mmol/L
[K+]O (Figure 2D
).
Activation showed saturation at conditioning voltages >20 mV.
Boltzmann fits to the data revealed V0.5 of
2.9±1.0 and 4.3±2.5 mV in RV and LV, respectively, while
corresponding slope factors were 6.2±2.1 and 5.3±0.8 mV
(P=NS). IKr density was not
different between RV and LV M cells. Voltage dependence and time course
of IKr deactivation were also not
different.
Properties of IK1
Whole-cell recordings of IK1
are shown in Figure 1
. IK1 rapidly
activated and showed inactivation at the more negative
voltages. In all cases, this current was fully inhibited in 0
[K+]O. There were no
differences in the magnitude of IK1
(initial minimal values as well as steady-state levels) between RV and
LV throughout the voltage range tested (Figure 2E
).
| Discussion |
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The presence of IKr and IKs was confirmed in M cells from the LV and was also demonstrated in RV M cells. Densities of IKr were similar in both ventricles. IKs density however, was significantly larger in RV, and this difference could explain, at least in part, why APD50 and APD95 were longer and why the APD/pacing CL relationship was steeper in LV than in RV M cells. Heterogeneity of IKs across the transmural LV wall has been linked to dispersion of repolarization and the danger of torsade de pointes.4 6 Our results on IKs (and ITO1) suggest that arrhythmogenic electromotive gradients could also arise at the septal junction of the RV and LV.
In human ventricular myocytes, the presence of IKr and IKs has also been demonstrated.13 Interestingly, Li et al13 made their observations in apparently undiseased RV myocytes of patients with left-sided heart failure. The finding of substantial amplitudes of IKr and IKs, as well as the sensitivity of both components to their blockers (E-4031 and indapamide), may underscore the importance of these currents for human ventricular repolarization, as expected from the clinical response to class Ia and class III agents in patients and from molecular studies on K+ channels in human myocardial tissue.
Our finding of a large ITO1 in RV M cells is in keeping with the prominent spike-and-dome morphology of the action potentials. Yan and Antzelevitch14 presented evidence that the distribution of ITO1 across the canine ventricular wall is causally linked to the J wave of the ECG. The joint results of this and another study8 indicate that a large ITO1-mediated notch can be found throughout most of the RV mass, which suggests that the contribution of the RV to the formation of the J wave on the ECG may be larger than previously assumed. Furthermore, this may have important consequences for our understanding of the Brugada syndrome. ST-segment elevation in the right precordial ECG leads of patients suffering from this disorder has been linked to the concept of "all-or-none repolarization" in the RV epicardium.15 If our data are applicable to patients, then the substrate predisposed to all-or-none repolarization may cover most of the RV transmural wall.
Received September 21, 1998; revision received November 4, 1998; accepted November 12, 1998.
| References |
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