(Circulation. 1997;96:3079-3086.)
© 1997 American Heart Association, Inc.
Articles |
From the Laboratorio de Cardiología Experimental, Servicio de Cardiología, Hospital General Universitari Vall d'Hebron, Universitat Autònoma de Barcelona, Spain.
Correspondence to Juan Cinca, MD, Servicio de Cardiología, Hospital General Universitari Vall d'Hebron, Passeig Vall d'Hebron 119-129, 08035 Barcelona, Spain. E-mail jcinca{at}ar.vhebron.es
| Abstract |
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Methods and Results Myocardial impedance (resistivity
[
· cm] and phase angle [°]), epicardial ST segment,
and ventricular arrhythmias were analyzed
during 4 hours of coronary artery occlusion in 11
anesthetized open-chest pigs; these were compared with 13 other
pigs submitted to a similar coronary occlusion preceded by
ischemic preconditioning. Myocardial resistivity rose slowly
during the first 34±7 minutes of occlusion (237±41 to 359±59
· cm), increased rapidly to 488±100
· cm at 60
minutes, and reached a plateau value (718±266
· cm, ANOVA;
P<.01) at 150±69 minutes. By contrast, phase-angle changes
began after 17 minutes of ischemia (-3.0±1.6° to
-4.2±1.2° at 29±8 minutes) and evolved faster thereafter
(-12.5±5.3° at 144±56 minutes). Marked changes in myocardial
impedance were observed during the reversion of ST-segment elevation
that occurred 1 to 4 hours after occlusion, but impedance changes were
less apparent during the early ST-segment recovery seen at 15 to 35
minutes of ischemia. The second arrhythmia peak (30±5
minutes) coincided with the fast change in tissue impedance, and both
were delayed (P<.05) by ischemic
preconditioning.
Conclusions A rapid impairment of myocardial impedance occurs after 30 minutes of coronary occlusion, and its onset is better defined by shift in phase angle than by rise in tissue resistivity. Phase 1b arrhythmias are associated with marked impedance changes, and both are delayed by preconditioning. Reversion of ST-segment elevation is partially associated with impairment of myocardial impedance, but other factors play a role as well.
Key Words: ischemia infarction arrhythmia electrophysiology
| Introduction |
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Increases in intracellular resistance caused by ongoing ischemia may reduce the magnitude of intracellular and extracellular currents that are driven by membrane potential differences created between normal and ischemic cells.8 9 In these circumstances, the extracellular potential gradients that are responsible for the TQ- and ST-segment shifts in local electrograms may decrease and, hence, account for the spontaneous reversion of TQ-segment changes in experimental models8 and for the reduction of ST-segment elevation in patients with acute myocardial infarction.10 11 However, studies correlating myocardial impedance and ST-segment changes in ischemic conditions are lacking.
The rise in intracellular resistance impairs electrical conduction in the ischemic myocardium, and this may favor the genesis of ventricular arrhythmias.12 Recent studies performed in swine13 14 reported a temporal relationship between early phases of acute ischemic arrhythmias (called phase 1a and 1b15 ) and the steep rise in tissue resistivity that is thought to reflect the onset of cellular electrical uncoupling.1 13 Conversely, studies in perfused rabbit heart16 have shown that the onset of the steep rise in myocardial resistivity can be postponed by preconditioning of the myocardium with short-lasting ischemia.16 Therefore, preconditioning could allow us to assess whether an artificially induced adjournment of changes in resistivity is associated with a parallel delay in phase 1b arrhythmias. Such an investigation has not been performed in vivo and could contribute to our insight into the hypothesis that unlike phase 1a, phase 1b arrhythmias are associated with alterations in tissue electrical impedance.
This study was designed to analyze the effects of coronary artery occlusion on myocardial impedance in open-chest pigs with and without ischemic preconditioning and to correlate these changes with local epicardial ST-segment potential and ventricular arrhythmias.
| Methods |
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-chloralose (100 mg/kg IV) followed
by a continuous perfusion of this drug (25 mg ·
kg-1 · min-1).
Pulmonary ventilation was maintained with a pressure respirator
(TransPAC 5K257) at 41% oxygen concentration. The thorax was opened
through a midsternotomy, the pericardium was incised, and its free
margins were sutured to cradle the heart. The LAD was dissected above
the first diagonal branch and was looped with a Prolene 5/0 snare. The
two ends of the suture were threaded through a smooth plastic tube. The
artery was occluded by sliding the tubing over the suture and clamping
it with a small hemostat. Coronary reperfusion was established
by release of the ligature. In 13 pigs (group 1), the LAD was occluded
for 4 hours, whereas in the remaining 13 pigs (group 2), a similar LAD
ligature was preceded by preconditioning of the myocardium
with three LAD occlusion-reperfusion sequences lasting 5 minutes for
occlusion and 20 minutes for reperfusion. Systemic blood pressure was
sampled with a pigtail 7F catheter introduced
percutaneously through the right femoral artery.
Arterial blood gases were measured at regular intervals and
were kept within normal limits. Isotonic saline perfusion was
administered to compensate for blood losses. Pigs were handled in
accordance with the position of the American Heart Association and the
European Community Rules on Research Animal Use. This study was
approved by the ethics committee of our institution.
Myocardial Impedance
Theoretical Background
Myocardial electrical impedance (Z) is defined as the voltage
(V) measured across the tissue divided by the sinusoidal current (I)
applied through it (Z=V/I). Because the cell membranes have
capacitative properties,17 the myocardial tissue is not
purely resistive, and therefore, there will be a time delay between the
voltage and current waves that can be determined from the phase angle
of tissue impedance.7 In these circumstances, the
impedance (Z) will be a complex number (Z=R+jX), where R is the
resistance (in phase component of V with respect to I), j is the
imaginary unit (j=
), and X is the reactance (in quadrature
component of V with respect to I). Therefore, myocardial impedance can
be precisely defined by two components: tissue resistance (R) and phase
angle [
=arctan(X/R)]. To exclude the effects of the electrode
geometry on tissue resistance measurements, we calculated tissue
resistivity (
) from the relation r=k
, where k is the
electrode constant obtained by measuring the electrical resistance of a
0.9% saline solution at 25°C of known resistivity (70
· cm) with each electrode probe. We also monitored phase-angle
changes because, theoretically, they may allow better definition of the
rise in intracellular resistance that impairs cell-to-cell electrical
coupling.1 Because phase angle is due to the cell membrane
capacitance, the changes in intracellular resistance, which in an
equivalent circuit modeling the myocardium is in series
with the capacitance,7 will produce a phase-angle
shift.
Electrode Probe and Measuring Technique
The probe consisted of four platinum electrodes (5 mm long,
0.4 mm in diameter) mounted as a linear array on an insulating
substrate separated by an interelectrode distance of 2.5 mm. This
electrode arrangement allows us to consider the current electrodes as
point sources.18
Myocardial impedance was measured by an alternating current (10 µA,
1110 Hz) applied through the outer pair of electrodes and by
determination of both the in-phase and in-quadrature components of V
across the inner pair of electrodes with a high-input impedance lock-in
amplifier (Princeton Applied Research model 5110). This
technique was chosen because electrode polarization affects tissue
measurements to a lesser extent than when a single pair of electrodes
is used for both current injection and potential
measurement.19 20 Before each impedance measurement, the
current flowing through the tissue was determined by measurement of the
voltage across a resistance of 56 k
placed in series with the
tissue. This procedure was undertaken to account for the possible
current variations caused by the changes in tissue impedance in the
ischemic area. Changes in myocardial impedance were measured at
the center of the ischemic area and at remote normal myocardial
zones with two probes that were sutured to the epicardium and were
connected to the lock-in amplifier via an automatic multiplexor system.
The appropriate position of each probe with respect to the
ischemic area was verified at the end of the study by
injection of 10 mL of 25% fluorescein into the left
atrium. The ischemic area appears unstained, whereas the
normal myocardium is stained by the dye.
Data Analysis
Previous studies on isolated myocardial
preparations1 21 have shown a relationship between the
sharp increase in tissue resistance and the onset of cellular
electrical uncoupling assessed by intracellular potential
recordings. Because in the present intact heart model we do
not have a direct estimation of cellular uncoupling, the onset of this
condition can be only indirectly inferred from the steep impedance
changes. Conversely, uncoupling may not start
simultaneously in all ischemic cells, because
electrical and metabolic derangements are
heterogeneously distributed across the ischemic
region. The onset of the steep rise in resistivity was determined as
the moment at which the first derivative of resistivity versus time was
maximal. Phase-angle changes are more sharply demarcated, and in these
curves we measured both the maximal rate of change and the earliest
time at which a value exceeds 10% of baseline.
Epicardial ST-Segment Potential
Extracellular DC epicardial electrograms were recorded with
a multichannel differential amplifier system. Electrodes were made with
polyethylene tubes 0.5 mm in diameter containing a cotton thread
saturated with isotonic saline solution and were connected to the
amplifiers through a Ag/AgCl interface. Thirty-two cotton electrodes
were sutured to a rubber membrane at interelectrode distances of 5
mm, forming three parallel rows. This membrane was sutured to the left
ventricular epicardium in a direction parallel to the LAD
covering an area extending from the acutely ischemic region to
the normal myocardial zone. The two impedance probes were inserted
parallel to the rows of epicardial cotton electrodes (Fig 1
), and impedance measurements were
correlated to the mean ST-segment potential values measured in the six
cotton electrodes surrounding the impedance probe. Epicardial
electrograms were recorded at samples of 2-second duration,
digitized at a frequency of 500 Hz, and stored in a computer. In
addition, selected analog signals were continuously recorded with a
7-channel Elema ink-jet polygraph. ST segment was expressed as total
TQ+ST-segment displacement, because this corresponds to the ST segment
recorded by conventional ECG.22
|
Arrhythmia Analysis
VPBs, VT, and VF occurring during the 4 hours of LAD occlusion
were monitored by continuous recording of a conventional ECG
with an Elema Mingograf 82 ink-jet polygraph. VT was defined as a
succession of more than three VPBs at a rate >100 bpm. Sustained VT
was considered to be a VT lasting >30 seconds. Sustained VT and VF
were terminated by direct DC electrical countershock of 10 J.
Study Protocol
Myocardial impedance, epicardial electrograms, conventional
ECGs, and blood pressure were recorded at baseline and during 4
hours of LAD occlusion. ECG and blood pressure were recorded
continuously, impedance measurements were taken every 2 minutes, and
samples of epicardial electrograms of 2-second duration were acquired
every minute during the first 60 minutes of ischemia and every
15 minutes thereafter.
Data Analysis
Differences in myocardial resistivity, phase angle, and
ST-segment potential during 4 hours of coronary occlusion were
assessed by repeated-measures ANOVA with a commercially available
software (SYSTAT Inc). Samples were taken at baseline and every hour.
Because preconditioning affects primarily the onset of the rapid
changes in myocardial resistivity and phase angle, we assessed the
differences between groups by applying the ANOVA test to the samples
taken at 30, 40, 50, 60, and 70 minutes after coronary
occlusion. For this analysis, we normalized the individual
curves to their baseline values by subtracting them from each
measurement. To assess group differences in early ST-segment changes,
the ANOVA test was performed at baseline and at 10, 20, 30, 40, 50, and
60 minutes. Results are expressed as mean±SD, and as a significance
test for linear, quadratic, and cubic contrasts, the level was set to
P<.05. The assumption of normality for ANOVA residuals was
graphically verified with normal probability plots. Correlation between
myocardial impedance and ST-segment potential was assessed by linear
regression, and results are presented as subject-adjusted
regression coefficient.23 Group differences in the onset
and in maximal changes of myocardial resistivity and phase angle, in
the time to peak of phase 1a and 1b arrhythmias, and in the
total number of VPBs were evaluated by Student's t
test.
| Results |
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Changes in Tissue Resistivity
As illustrated in Fig 1
, 2
to 4 minutes after coronary
occlusion, the nonpreconditioned pigs showed an initial
slight increase in myocardial resistivity (from 237±41 to 259±41
· cm), which was followed by a progressive rise up to
359±59
· cm at 34±7 minutes. A second phase began
thereafter and was characterized by a rapid increase in resistivity
leading to values of 488±100
· cm at 60 minutes of
coronary occlusion. This second phase was followed by a slow
rise until maximal plateau values (718±266
· cm) were
reached 150±69 minutes after coronary occlusion.
Ischemic preconditioning induced significant
(P=.004) differences in the time course of myocardial
resistivity during the first 30 to 70 minutes of ischemia (Fig 2
). As shown in Fig 3
, preconditioning postponed the steep
rise in myocardial resistivity (from 34±7 to 52±25 minutes,
P=.04), although this treatment did not significantly affect
the baseline (209±47
· cm) or the maximal (569±178
· cm) resistivity values.
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Changes in Phase Angle
In contrast to the prompt onset of resistivity changes,
phase-angle shift was <10% of baseline until 17 minutes of
ischemia had elapsed (Figs 1
and 4
). After this interval, phase angle
slowly decreased from -3.0±1.6° to -4.2±1.2° at 29±8 minutes
of occlusion. These initial changes were followed by a sharp shift to
-12.5±5.3° at 144±56 minutes, leading to a maximal plateau phase
that lasted until the end of the study. The slope of the phase-angle
shift after 30 minutes of coronary occlusion was greater than
the slope of the concurrent rise in resistivity (% change from
baseline per minute, 4.9±3.1% versus 2.3±1.3%, P=.01).
Ischemic preconditioning induced significant
(P=.004) differences in the time course of tissue
phase-angle shift during the first 30 to 70 minutes of ischemia
(Fig 2
). This treatment postponed (Fig 3
) the onset of the sharp
phase-angle deviation (29±8 versus 53±27 minutes, P=.01)
but did not exert a significant influence on baseline (-2.3±2.3°)
or on maximal (-11.3±4.3°) phase-angle values. Preconditioned pigs
showed slight phase-angle changes during the first 17 minutes of
ischemia, but these were not significantly different from those
in the nonpreconditioned series.
|
ST-Segment Changes
Epicardial electrodes located in the ischemic area showed
significant (P<.01) ST-segment elevation during the 4 hours
of coronary occlusion in both series of pigs. In the
nonpreconditioned group (Fig 1
), ST-segment potential
depicted an early sharp rise up to 22.1±4.8 mV at 15 minutes. This was
followed by a transient reversion of ST segment to 11.4±6.3 mV at 35
minutes and by a subsequent reelevation up to 18.0±4.8 mV at 60
minutes of ischemia. From 1 hour onward, ST-segment elevation
declined progressively to 9.2±2.8 mV. Preconditioned pigs attained a
similar ST-segment peak at 15 minutes of ischemia (23.5±6.8
mV) and a comparable ST-segment decline (8.8±2.1 mV) at 4 hours of
occlusion (Fig 2
). By contrast, during the first 30 to 35 minutes of
ischemia, the preconditioned series showed a less marked
ST-segment recovery (21.5±13.1 mV, P=.01) than
nonpreconditioned pigs, although the ST-segment
dispersion was larger because four preconditioned pigs still showed
transient ST-segment recovery (Fig 2
).
Ventricular Arrhythmias
VPBs depicted a three-phase pattern (Fig 5
). The first phase began 2 minutes after
occlusion, peaked at 6±2 minutes, and ended
20 minutes later. After
a brief arrhythmia-free period, there was a second
arrhythmia phase peaking at 30±5 minutes, which vanished 1
hour after occlusion. The third arrhythmia period began
75±3 minutes after occlusion and lasted until the third hour of
coronary occlusion. Ischemic preconditioning (Fig 5
, bottom) attenuated the incidence of VPBs (total events, 2110 versus
2905, P<.05), especially during the third phase. In
addition, preconditioning delayed the time to the peak of the second
phase of ventricular ectopic activity (53±25 versus 30±5
minutes, P=.02) but had no significant effect on the time to
peak of the first arrhythmia phase.
|
The incidence and temporal distribution of more severe forms of
ventricular arrhythmias are illustrated in Fig 6
. Two of the 13
nonpreconditioned pigs (Fig 6A
) died prematurely
because of nonreversible VF. Episodes of nonsustained VT occurred in 8
of these remaining 11 pigs and tended to group into two phases, like
those of ventricular ectopic activity. Sustained VT
developed in 5 pigs, whereas VF occurred in 9 of the 13
nonpreconditioned pigs. Preconditioning (Fig 6B
) did
not significantly modify the incidence of malignant
ventricular arrhythmias.
|
Correlative Analysis
The relationship between ST-segment and myocardial impedance is
complex (Fig 1
). ST-segment elevation peaking at 15 minutes of
ischemia was not accompanied by phase-angle shift, and only a
slight rise in resistivity was observed. Between 15 and 60 minutes of
ischemia, resistivity and phase angle shifted monotonically
while ST-segment elevation depicted a reversion followed by a
transitory reelevation. From 1 hour of coronary occlusion
onward, ST-segment elevation decreased progressively, and tissue
resistivity and phase angle attained maximal plateau values in both
nonpreconditioned (Fig 1
) and preconditioned series
(Fig 2
). However, during this late period of time, the correlation
between ST-segment potential and tissue resistivity (r=-.26
for nonpreconditioned and r=-.17 for
preconditioned series) and between ST segment and phase angle
(r=.31 and r=.16 for each group, respectively)
did not reach statistical significance.
Ventricular ectopic activity peaking at 6 to 10 minutes of
coronary occlusion was associated with a slight rise in tissue
resistivity but was not accompanied by phase-angle changes. By
contrast, the second arrhythmia period, occurring at
30
minutes of ischemia, was accompanied by a sharp change in
resistivity and phase angle, and all these variables were delayed
by ischemic preconditioning. The third arrhythmia phase
was associated with maximal resistivity and phase-angle values.
| Discussion |
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The mechanism underlying the changes in myocardial impedance in the in situ ischemic heart is not well known. The sharp rise in tissue resistivity has been related to cell-to-cell electrical uncoupling in ischemic heart preparations,1 2 24 but data on phase-angle changes elicited by coronary occlusion are scant.25 The major determinants of myocardial impedance are the extracellular and intracellular resistance, the gap junction conductance, and the cell membrane capacitance.5 6 7 Extracellular resistance increases during the first 10 to 15 minutes of ischemia in the perfused papillary muscle1 as a result of the collapse of the extracellular compartment caused by cessation of coronary perfusion and by osmotic cell swelling.26 By contrast, intracellular resistance increases after 10 to 15 minutes of ischemia1 and leads to cellular electrical uncoupling as a result of a drop in gap junctional conductance induced by, among other things, the intracellular accumulation of both free Ca2+2 and amphipathic lipid metabolites4 and the reduction of ATP content3 in the ischemic myocardium. Intracellular acidosis affects gap junction conductance,27 but it does not appear to be a major trigger for cellular uncoupling during ischemia.2
Assuming that the time course of extracellular and intracellular resistance changes in the ischemic papillary muscle1 could be extrapolated to the in situ heart, there would be a temporal relationship between the initial increase in extracellular resistance and the immediate slow rise in tissue resistivity. Likewise, the subsequent increase in intracellular resistance would correlate with the sharp phase-angle and resistivity changes. To further interpret the alterations in myocardial impedance, an equivalent circuit composed by two parallel branches modeling the passive electrical elements of the myocardium7 may be considered: one branch modeling the extracellular resistance and a second branch composed of a series of three elements modeling the membrane capacitance, the intracellular resistance, and gap junctional resistance, respectively. Because phase-angle shift is caused by membrane capacitance,17 the initial changes in extracellular resistance, which in the equivalent circuit is in parallel with this capacitance, will affect tissue resistivity more than phase angle, as seen during the first 17 minutes of coronary occlusion in our study. By contrast, the ensuing rise in intracellular resistance,1 which in the equivalent circuit is in series with the capacitance, may account for both the phase-angle shift that begins after 17 minutes of ischemia and the further rise in resistivity seen in this study as well. Thus, the alterations in intracellular resistance that lead to cell-to-cell electrical uncoupling may be better defined by the changes in phase angle than by the changes in tissue resistivity. However, because no direct assessment of the uncoupling process is made in this study, we cannot precisely ascertain which moment of the phase-angle changes indicates the onset of uncoupling. Moreover, uncoupling is not expected to begin simultaneously in all ischemic cells, provided that electrical and metabolic derangements are not uniformly distributed in the ischemic area.
This study reveals that ischemic preconditioning postpones the steep changes in both tissue resistivity and phase angle, and this is in agreement with the delayed rise in resistivity seen in preconditioned papillary muscle.16 The mechanism by which preconditioning postpones the impairment of passive myocardial properties has been linked to activation of the IK-ATP channel, because this delay can be abolished by the channel blocker glibenclamide or, to the contrary, reproduced by the IK-ATP opener cromakalim.16 Conversely, preconditioning postpones the onset of intracellular Ca2+ accumulation,2 a circumstance that impairs gap junctional conductance.27 Compared with nonpreconditioned series, preconditioned pigs show slight phase-angle changes during the first 17 minutes of ischemia, suggesting that the three episodes of ischemia and reperfusion performed before the sustained coronary occlusion might have yielded residual abnormalities in intracellular resistance, but this needs to be confirmed.
Myocardial Impedance and ST-Segment Changes
Myocardial ischemia impairs active electrical cell
properties,8 9 and this creates membrane potential
differences between the ischemic and normal zones that are
responsible for TQ- and ST-segment shifts in extracellular
recordings.8 9 The current flowing as a result of
the regional membrane voltage differences is expected to decrease when
tissue resistivity increases in the ischemic
region,28 29 thus leading to TQ- and ST-segment potential
attenuation. This circumstance might explain the spontaneous decline in
the magnitude of the ST-segment elevation seen in patients with acute
myocardial infarction,10 11 but correlative studies
between ST-segment and myocardial impedance in ischemic intact
heart are lacking. Our study reveals that there is a transient
ST-segment recovery at 15 to 30 minutes of ischemia associated
with minor impedance changes, whereas 1 hour after occlusion,
ST-segment elevation declined progressively and impedance changes
attained their maximal values. The early ST-segment potential decline
has been described previously in the porcine model30 and
bears a temporal relationship with the well-recognized transitory
improvement of action potential characteristics of ischemic
cells,8 9 which coincide with the plateau phase of
extracellular K+ accumulation. It might therefore be
anticipated that the recovery of active cell properties will reduce the
regional membrane potential differences responsible for ST-segment
shift and hence play a major role in early ST-segment recovery. We
observed that ischemic preconditioning tends to lessen the
magnitude of transient ST-segment recovery, but the mechanism of this
action is uncertain. In accordance with the early ST-segment recovery,
other studies in pigs13 have reported reversion of
TQ-segment displacement 20 to 30 minutes after coronary
occlusion, although correlative ST-segment data were not available.
Reversion of ST-segment elevation after 1 hour of occlusion is
associated with marked myocardial impedance changes, suggesting a
relationship between these two phenomena. Other factors, however, such
as the loss of membrane potential caused by irreversible cell membrane
damage, may further reduce the regional membrane potential differences
between normal and ischemic myocardium and
therefore attenuate the ST-segment shift.
Myocardial Impedance and Ventricular Arrhythmias
Recent studies by Smith et al13 and by our
group14 in anesthetized pigs show that phase 1a
arrhythmias coincide with the initial slow rise in myocardial
resistivity and that phase 1b arrhythmias concur with the steep
rise in resistivity. Present data further evidence that these
arrhythmias can be better defined by the changes in tissue
phase angle, because phase 1a arrhythmias are not associated
with significant changes in tissue phase angle, whereas phase 1b
arrhythmias coincide with the fast phase-angle shift. The third
arrhythmia phase began 1 hour after coronary ligature
and coincided with maximal values of tissue resistivity and phase
angle. In addition to the relationship with tissue impedance changes,
phase 1a arrhythmias coincide with the first rise in
extracellular K+ accumulation and with progressive acidosis
in the ischemic area, whereas phase 1b arrhythmias
concur with the second rise in K+.13 Changes
in extracellular K+ concentration are
heterogeneously distributed in the ischemic
myocardium,31 and they can be used as a
surrogate for the ionic and metabolic derangements induced
by ischemia, because K+ changes correlate with the
alterations in intracellular Ca2+, intracellular and
extracellular pH, tissue resistance, and phosphocreatine and ATP
elicited in the ischemic
myocardium.24
Alterations in tissue impedance may depress conduction of the excitation wave front12 and favor the maintenance or the initiation of reentrant arrhythmias. The mechanism underlying the distinct phases of early ischemic arrhythmias is not entirely known. Multisite recordings of local electrograms28 32 suggest a reentrant mechanism for phase 1a arrhythmias. By contrast, attenuation of phase 1b arrhythmias after ß-blockade33 or after myocardial denervation34 may indicate that these arrhythmias might be caused by abnormal automaticity, provided that this arrhythmogenic mechanism is linked to the action of catecholamines. Present data suggest that alterations in intracellular resistance may play a role in the genesis of phase 1b and late (2 to 4 hours) ischemic arrhythmias but not those of phase 1a. This assumption is further strengthened by the fact that preconditioning postpones, in a parallel fashion, both the steep changes in myocardial impedance and the peak of the phase 1b arrhythmias.
The beneficial effect of preconditioning on reperfusion arrhythmias has been largely recognized,35 36 37 but its influence on arrhythmias during acute coronary occlusion is less well known. In our series, preconditioning attenuated the incidence of VPBs during coronary occlusion but not the incidence of more severe ventricular arrhythmias. Other studies report reductions in the number of severe ventricular arrhythmias during coronary occlusion in preconditioned hearts.35 38 39
| Selected Abbreviations and Acronyms |
|---|
|
| Acknowledgments |
|---|
Received March 6, 1997; revision received May 19, 1997; accepted May 28, 1997.
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