(Circulation. 1997;96:3136-3147.)
© 1997 American Heart Association, Inc.
Articles |
From the Departments of Pharmacology and Medicine, College of Physicians and Surgeons of Columbia University, New York, NY.
Correspondence to Andrew L. Wit, PhD, Department of Pharmacology, College of Physicians and Surgeons of Columbia University, 630 W 168th St, New York, NY 10032.
| Abstract |
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Methods and Results Reentrant VT was initiated by PES in twelve 4-day-old infarcted dog hearts. The relationship between V1V2 and V2T1 was always direct. Mapping of the epicardial border zone (EBZ) indicated that initiation of VT was secondary to functional orthodromic block of V2, propagation of V2 around the line of block, and antidromic propagation through the original location of the block. In 7 dogs, the line of orthodromic block and the pathway of orthodromic propagation were similar for different V1V2 coupling intervals. Orthodromic conduction time around the line to its distal side was longer at shorter V1V2 intervals, but a shorter antidromic delay in the area of unidirectional block for shorter V1V2 intervals, possibly reflecting small changes in the conduction pathway involving deeper layers of the EBZ, resulted in shorter V2T1 intervals. In the other 5 dogs, the orthodromic conduction pathway of V2 around the line of block changed markedly, with a shorter pathway for shorter V1V2 intervals resulting in shorter V2T1 intervals.
Conclusions An inverse relationship between V1V2 and V2T1 is not a specific indicator of functional reentry.
Key Words: arrhythmia myocardial infarction electrophysiology mapping reentry tachycardia
| Introduction |
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40% of
clinical VTs that all other evidence indicates are caused by
reentry.4 6 7 The question of what mechanisms might
underlie the lack of an inverse relationship during initiation of
reentry has not been answered and was the focus of our study in a
laboratory model, the infarcted canine heart.8 9 10 A
preliminary report of these data has been published in abstract
form.11 | Methods |
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Electrode Array and Recording Instrumentation
In some of the experiments, the electrode array consisted of 292
bipolar electrodes10 made of silver disks with a diameter
of 1 mm and a distance between poles in the bipolar pair of 2
mm. The distance between bipolar pairs was 5 to 10 mm. In other
experiments, the electrode array consisted of 312 bipolar electrode
pairs also made of 1-mm-diameter silver disks with a distance between
poles of 3.2 mm. The distance between bipolar pairs was 4.8 to
6.4 mm.
For the studies with the 292-electrode array, signals from 192 electrodes could be recorded simultaneously. The electrode leads, chosen with a switch box, were led into preamplifiers with automatic gain controlled by a microprocessor. The electrograms were filtered (10 to 1000 Hz), multiplexed, sampled (2000 samples per second), and digitized by an 8-bit analog-to-digital converter.9 For experiments with the 320-electrode array, signals from all electrodes were simultaneously bandpass filtered (15 to 500 Hz), sampled at 1000 samples per second, and digitized by a 16-bit analog-to-digital converter. All digitized signals were pulse-code modulated and stored on a wide-band tape recording system (Ampex).
Experimental Protocol
Two ECG leads and arterial blood pressure were
continuously monitored on an Electronics for Medicine DR-12
oscillographic recorder. For induction of VT, the heart was
stimulated through bipolar electrodes on the noninfarcted right
ventricle adjacent to the LAD with a basic train of stimuli
(S1S1) at the longest cycle length that ensured
capture (250 to 350 ms). Single premature stimuli (S2) were
applied at progressively decreasing coupling intervals until they could
not initiate a premature response. Basic and premature stimuli were 2
ms in duration and 2 to 4 times diastolic threshold.
Sustained VT was defined as tachycardia lasting longer than
30 seconds. All sustained tachycardias were monomorphic,
whereas nonsustained tachycardias (<30 seconds in
duration) were either monomorphic or polymorphic.
Data Processing
Our methods for determining local activation times and drawing
isochronal maps have been described.9 10 We defined
conduction block as occurring where there were more than three
interpolated isochrones between adjacent electrodes (>40 ms) with
the wave front moving in opposite directions on different sides of the
region designated as block. Because the bipolar electrodes were 5 to
10 mm apart, 40 ms between adjacent electrodes provides a
conduction velocity of 10 to 20 cm/s, assuming conduction directly from
one electrode to the next, which is possible in nonuniformly
anisotropic myocardium.12 However, it is
unlikely that slow conduction is occurring when adjacent wave fronts
are moving in opposite directions. The probable exit route of the
reentrant impulse from the EBZ to the ventricles was determined by
locating the electrodes on the margin of the array that were excited
just before the onset of the QRS, on the assumption that the impulse
does not enter the ventricles through intramural connections at the
center of the EBZ.13 This assumption may not always be
correct; the detailed anatomy of the EBZ was not studied in
these experiments. The relationship between
V1V2 (coupling interval of
ventricular activation by the last basic impulse,
V1, and by the premature impulse, V2) and
V2T1 (coupling interval between premature
ventricular activation, V2, and activation by
the first tachycardia impulse, T1) was measured
on the ECG (time between the peaks of the R waves of the QRSs) and on
epicardial electrograms adjacent to the site of stimulation (time
between activations). The data were fitted by a linear regression
model. To test the hypothesis that the slope of the regression line was
different from zero, a significance level of P<.05 was
selected (SigmaStat; Jandel Scientific Software). All data are
expressed as mean±SD.
| Results |
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We did not find an inverse relationship between
V1V2 and V2T1 in any of
the 12 experiments when measured on the ECG or at electrograms near the
stimulus site. In fact, in 11 of the 12 experiments the relationship
was direct: as the V1V2 interval decreased, the
V2T1 interval also decreased. In 1 experiment,
the relationship measured on the ECG was flat (ie,
V2T1 did not change over a range of
V1V2), but it was direct when measured on the
electrograms at the stimulus site. Fig 1A
shows the initiation of a sustained monomorphic VT at the longest and
shortest premature coupling intervals (V1V2) of
190 ms (top) and 163 ms (bottom), at a basic drive cycle
(V1V1) of 280 ms. In this experiment, all
tachycardias had the same QRS morphology as the first
nonstimulated beat. To the right is the direct relationship measured on
the ECG. Fig 1B
shows the initiation of VT at premature coupling
intervals of 205 ms (top) and 190 ms (bottom), at a basic cycle length
of 300 ms in a different experiment in which only a
V1V2 coupling interval of 190 ms resulted in
sustained monomorphic tachycardia. The ECG morphology of
the sustained tachycardia was different from the morphology
of the initiating impulses (Fig 1B
, bottom). The QRS morphologies of
the first tachycardia impulse at each coupling interval for
nonsustained tachycardia were similar to each other and to
the QRS of the first two beats of the sustained
tachycardia. To the right is the direct relationship
on the ECG.
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From the activation maps, we found two different general patterns of initiation of VT that were responsible for the direct relationships, although there were some similar features between the two.
Conduction of Premature Impulses With Different Coupling Intervals
Over Similar Reentrant Pathways (Pattern 1 in Table
)
In these hearts, conduction of the premature impulse that
initiated reentry blocked in the orthodromic direction. Propagation of
the premature impulse proceeded around the ends of the line of block
and activated its distal side. Antidromic reexcitation of the
proximal side of the line of block then completed the reentrant circuit
and caused the onset of the tachycardia. The premature
impulses initiated at different coupling intervals had similar
activation patterns on a macroscopic level. As the coupling of the
premature impulse decreased, orthodromic conduction time around the
line of block increased, but antidromic conduction time decreased. The
summation of the orthodromic and antidromic conduction decreased with
decreasing coupling intervals. In Fig 2A
, the direct relationship for the seven experiments that had this
characteristic is plotted. The regression lines have a positive slope
(P<.05).
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Activation maps from one of the experiments in this group are shown in
Fig 3
(ECG in Fig 1A
). Fig 3A
shows the
activation pattern of the last stimulated impulse, S1,
initiated at the LAD margin (pulse symbol) (arrows show the direction
of propagation). There is a small region of conduction
disturbance at the basal margin (activation times 58 to 64),
but the remainder of the EBZ is activated without block. The
fingerlike pro- jection of the 10-ms isochrone into the EBZ
suggests some intramural connections in this region. The electrograms
in Fig 4A
, recorded from the sites
circled in Fig 3A
, show impulse propagation during the basic drive
(V1). Fig 3B
shows propagation of the premature impulse
(long V1V2 coupling interval of 190 ms) that
initiated sustained VT. At isochrones 20 to 30 ms, the stimulated
wave front blocked orthodromically, shown by the long heavy black line.
The line of block as defined (see "Methods") was characterized by
a long delay between adjacent electrodes with wave fronts moving in
opposite directions on either side of the line and was
35 to 40
mm long. The line was located within 10 to 20 mm of the region
with intramural connections (possibly the margin with normal
myocardium), as indicated by the relatively large area
activated nearly simultaneously within
isochrones 10 to 20. It is doubtful that such rapid activation of
large regions can occur only by propagation over a narrow epicardial
layer. During sinus rhythm, there was epicardial breakthrough in this
region, supporting this interpretation. Fig 4A
shows electrograms recorded across
the line of block (V2). Electrogram c, with an activation
time of 16 ms, was proximal to the line of block, whereas electrode d
(asterisk) was at or just distal to the line. The propagating wave then
proceeded around the edges of the line of block (isochrones 30 to
70 ms in Fig 3B
) and activated the distal side (isochrones
90 to 140 ms) antidromically. In Fig 4A
, electrodes e and d were
activated at 146 and 156 ms by the premature wave front that
reached the distal side of the line of block.
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Fig 3C
shows activation resulting in the first beat of the
tachycardia. Activation in this time window begins at the
asterisk (the 6-ms activation time that is circled is equal to the
156-ms circled activation time in Fig 3B
). The proximal side of the
line of block was reactivated antidromically (isochrones 10
to 70 ms). The antidromic activation time on the epicardial surface in
the region in which the original line of block was located
(isochrones 10 to 50 ms) was prolonged, requiring 46 ms to
activate a region of
4.8 mm. Although the apparent
conduction velocity is
10 cm/s, a true conduction velocity cannot be
calculated because the exact pathway of propagation on a microscale is
not known. In fact, conduction velocity may not be so slow, because an
altered pathway of activation involving deeper layers of myocardial
cells might have been used (see "Discussion"). Electrograms
recorded in this region (electrodes b and c in Fig 4A
within the
dashed rectangle) show double potentials: two deflections separated by
an isoelectric segment. The delay in antidromic propagation corresponds
to the delay between the two potentials at each of these
recording sites. The relative sharpness of the two deflections
in electrogram c might not be expected if the delay was a result of
only very slow conduction on the epicardial surface and favors the
interpretation of the involvement of deeper layers in the antidromic
conduction pathway (see "Discussion"). Farther away, activation
proceeded more rapidly (isochrones 50 to 90 ms in Fig 3C
) to the
LAD margin of the electrode array (electrode a [T1] in
Fig 4A
). The exit route to the ventricles causing the first beat of
tachycardia was toward the LAD margin. The
V2T1 interval at electrode a (Fig 4A
) was 214
ms. That the exit route was close to the stimulating electrode explains
why the morphology of the first beat of the tachycardia is
similar to the stimulated beats (Fig 1A
). After reaching the LAD
margin, the propagating wave split (Fig 3C
) and proceeded
counterclockwise to the apical margin (isochrones 80 to 130 at the
left) and clockwise to the basal margin (isochrones 80 to 130 at
the right). Later, the two waves coalesced around isochrone 190 to
200 (Fig 3C
) near the left lateral margin of the electrode array, and
activation proceeded toward the LAD margin (isochrones 190 to 250)
to complete the circuit (circled activation 249 and Fig 4A
, electrode
e, T2). Fig 3D
shows the activation map of the second beat
of the tachycardia. Activation begins in the 10-ms
isochrone (asterisk) where the map in Fig 3C
ends and moves around
two lines of block (heavy black lines) (isochrones 30 to 130 to the
left and right). Activation time of the region in which the original
line of block was located (isochrones 10 to 30 ms) was faster, with
an apparent conduction velocity of
1 m/s. Because this velocity
seems too high for ventricular myocardium, the
rapidity of activation may result from a contribution to activation
from deeper layers of surviving myocardial cells in this region. Note
that in electrogram b (Fig 4A
, T2), the second deflection of the double
potential is much smaller in amplitude and the delay between the two
deflections is decreased, whereas in electrogram c (T2), a
very small undulation in the isoelectric potential may be the remnant
of the double potential. The pattern of activation shown in Fig 3D
is
similar to the pattern of activation that occurred later on during the
sustained tachycardia.
Fig 5
shows isochronal maps during
initiation of VT in this same experiment by a shorter coupled premature
impulse with a V1V2 of 166 ms (electrode a in
Fig 4B
and bottom of Fig 1A
). The sequence of activation during the
basic drive was similar to the map in Fig 3A
and is not shown. The
pattern of propagation of the premature impulse (Fig 5A
) was similar to
the premature impulse with the longer coupling interval (Fig 3B
). A
long line of block formed during propagation in the orthodromic
direction (heavy black line); propagation proceeded around the edges of
the line of block and excited antidromically the distal side of the
line at
179 to 219 ms. However, there were some quantitative
differences. The line of block seemed to shift slightly (
5 mm)
toward the LAD margin, between electrodes b and c (Fig 4B
, V2) instead of between electrodes c and d as for the longer
coupling interval (Fig 4A
, V2), and was
10 mm
longer (50 to 55 mm). The time for propagation of the premature
impulse from the LAD margin to the distal side of the line of block
increased to 160 ms (difference between the activation times at circled
electrodes 27 and 187 in Fig 5A
) at the shorter coupling interval from
the 139 ms (difference between the activation times at circled
electrodes 17 and 156 in Fig 3B
) at the longer premature coupling
interval. The increase was the result of slower activation and the
longer line of block. Fig 5B
shows the pattern of antidromic
propagation that caused the first beat of the tachycardia.
The pattern was similar to the premature impulse with the longer
coupling interval: the proximal side of the original line of block was
antidromically activated (isochrones 0 to 10 ms, asterisk).
However, the region of antidromic breakthrough was wider. The interval
between the time of activation of the distal side (electrode c, Fig 4B
)
and the reactivation of the proximal side (electrode a) during
antidromic propagation was 37 ms for the shorter coupled premature
impulse, in contrast to 75 ms for the longer coupled impulse (Fig 4A
).
The shorter time to reactivate the region antidromic to the
block may have resulted from a change in the antidromic pathway to
involve less of the deeper myocardium (see
"Discussion"). Note that a double potential is not prominent at
electrode c, although there is a very small second slow deflection at
electrode b (dashed rectangle in Fig 4B
) for this shorter coupling
interval that corresponds to the more rapid antidromic activation. In
addition, the slight shift in the location of the line of block may
influence the occurrence of the double potential. Activation continued
then following a pattern of figure-eight reentry, with the exit route
located at the LAD margin. Therefore, despite the longer time required
to activate the distal side of the line of block for the
shorter coupling interval (Fig 4C
orthodromic, solid circles), the
resulting V2T1 interval at the electrode near
the stimulating site (electrode a) was 197 ms for the shorter coupling
interval and 214 ms for the longer coupling, indicating a direct
relationship between V1V2 and
V2T1 (Fig 4C
, solid triangles) because of the
more rapid antidromic activation (Fig 4C
, solid squares). Activation of
the second beat of the tachycardia and the subsequent
tachycardia was similar to the activation pattern shown in
Fig 3D
.
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The patterns of activation for the other experiments in this group were
almost identical to the example shown in Figs 3 through 5![]()
![]()
. Double
potentials occurred in the region of antidromic activation at long
V1V2 intervals and diminished or disappeared
with the decreased antidromic activation time that occurred when
V1V2 decreased.
Conduction of Premature Impulses With Different Coupling Intervals
Over Different Macroscopic Reentrant Pathways (Pattern 2 in
Table
)
The activation patterns associated with initiation of
tachycardia for the experiments in this group were more
diverse. The stimulated premature impulses that initiated reentry still
blocked, but activation of the distal side of the line of block
occurred through different pathways for short and long coupling
intervals, as shown by the activation maps. The pathway was shorter and
took less time to activate the distal side of the line of block
for the shorter coupling intervals than for the longer coupling
intervals, accounting for the shorter V2T1
intervals at shorter V1V1 intervals. Fig 2B
plots that relationship for all experiments. The regression lines have
a positive slope (P<.05).
Fig 6
shows the pattern of activation for
one experiment in this group during initiation of a monomorphic
nonsustained VT lasting 6 impulses by a premature stimulus delivered
near the LAD margin (pulse symbol in A and B), with the longest
V1V2 coupling interval (172 ms). Activation of
the EBZ by the last impulse of the basic train (arrows) (cycle length
300 ms) is shown in Fig 6A
. Several of the electrograms recorded
during the basic drive (recording sites are circled and labeled
a through f on the map), when the reentrant circuit was located after
premature stimulation, are shown in Fig 7A
(V1). Fig 6B
shows the
premature impulse. Activation proceeded from the stimulus site (pulse
symbol) for about 20 to 50 ms before blocking (horizontal heavy black
line). Additional lines of block also formed toward the apex (heavy
black lines). Electrograms recorded proximal to the line of block
(a, b, f) and distal to the line of block (c, d, e) are shown in Fig 7A
(V2), with their activation times indicated. Propagation
occurred around both ends of the line of block, with the distal side
activated after 147 to 178 ms. The electrograms recorded
from the circled electrodes on the distal side of the line of block on
the map (Fig 6B
) are shown in Fig 7A
(e, d, c, with activation times of
147, 152, and 178 ms). The map in Fig 6C
overlaps the one in Fig 6B
; it
has a time window that starts (asterisk) at the 140-ms isochrone of
Fig 6B
. It shows antidromic activation (isochrones 10 to 30).
Unlike in Figs 3 through 5![]()
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, there was no long delay in activation by
the antidromic impulse in the region in which the line of orthodromic
block was located (isochrones 10 to 30 and curved black arrow)
(electrogram recordings d, c, b, and a during T1 in
Fig 7A
). The region in which the antidromic wave front crossed the
right side of the line of block was also close to the exit route to the
ventricles (at the basal margin) that caused the first impulse of the
tachycardia. Conduction time from the stimulus site near
electrode a (circled activation time 4 ms in Fig 6B
) to the right
distal side of the line of block (electrode d; circled activation time
152 ms in Fig 6B
) was 148 ms. Conduction time from this region back to
electrode a was 9 ms, accounting for the V2T1
coupling interval of 157 ms near the site of stimulation (Fig 7A
). A
reentrant circuit then formed around the right end of the line (curved
black arrows; isochrones 10 to 150 in Fig 6C
). Fig 6D
shows the
reentrant activation around the line of block to the right during the
second tachycardia impulse (curved black arrows,
isochrones 10 to 150). Block occurred in this circuit, terminating
the tachycardia after 6 impulses (not shown).
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Fig 8
illustrates the activation patterns
during initiation of a nonsustained VT lasting 7 impulses, with a
premature impulse having the shortest V1V2
coupling interval of 148 ms in this same experiment. Propagation of the
basic drive was the same as before (Fig 6A
). There is a long delay in
epicardial activation by the premature impulse after isochrones 30
to 40 (Fig 8A
) in the same region as where the longest coupled
premature impulse blocked (see Fig 6B
). However, there is evidence from
the activation times that block of this early premature impulse did not
occur, despite the large differences in activation times at adjacent
electrodes where the heavy dashed line is located, because the wave
front is moving in the same direction on both sides of this line. The
region distal to the center of the line is activated between
111 and 126 ms in an orthodromic direction (open arrows and shaded
area; see electrodes c, d, e, and f during V2 in Fig 7B
).
Because electrograms recorded here did not show fractionation (see
Fig 7B
, electrodes b, c, and d), the slow activation may have involved
a change in pathway through deeper surviving myocardial cell layers
rather than slow conduction on the epicardial surface. From this shaded
area there is orthodromic activation (isochrones 120 to 140), so
that wave fronts on opposite sides of the region of delay are moving in
the same direction. There is collision of this orthodromic wave front
(open arrows) with the wave front propagating around the right side of
the line of block (curved black arrows). Therefore, the true line of
block was shorter (solid heavy black line). The map in Fig 8B
overlaps
the one in Fig 8A
; time 117 ms in Fig 8A
corresponds to time 10 ms in
Fig 8B
. The small region activated between 0 and 10 ms at the
asterisk indicates the premature wave front moving in the orthodromic
direction (straight black arrow); the region at the end of the right
line of block activated between 0 and 10 ms (asterisk)
indicates the premature wave front coming around the right end of the
line of block (curved arrows). The merging of the two wave fronts
occurs in the shaded region between the 30-ms isochrones. Because
this large (shaded) region is activated within 6 ms, there may
also be some contribution to epicardial activation from deeper cell
layers. From this area, reexcitation of the proximal side of the line
of block occurred (curved open arrows). Activation continued to the
right around the remnants of the line of block in a reentrant pattern
(isochrones 40 to 120 and curved black arrows). Conduction time
from the stimulus site near electrode a (circled activation time 4 ms
in Fig 8A
) to the right distal side of the line of block where the
impulse crossed the line in the antidromic direction (electrodes c and
d; circled activation times 117 to 118 ms in Fig 8A
) was 113 to 114 ms
(compare with 148 ms for the longer coupled premature impulse in Fig 6
). Conduction time from this region back to electrode a was 10 ms
(compare with 9 ms for the longer coupled premature impulse).
Therefore, the shorter orthodromic conduction time to the distal side
of the line of block accounted for the shorter
V2T1 coupling interval of 124 ms near the site
of stimulation (Fig 7B
). The corresponding value for the longer coupled
premature impulse was 157 ms (Fig 7A
), which indicates a direct
relationship between V1V2 and
V2T1.
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The variability of the pattern of propagation of premature impulses in
this group is illustrated in another experiment in Fig 9
in which nonsustained VT was induced.
Activation during the basic drive is not shown. Propagation of a long
coupled (170-ms) premature impulse (Fig 9A
) created a long
"horseshoe"-shaped line (heavy black lines) that was not
present during basic drive. Propagation moved around the extension
of this line of block at the right to activate its distal side
(isochrones 40 to 130; circled activation times 132 and 138),
although there also may have been some orthodromic activation, as
indicated by activation at one site distal to the line at 110 ms (open
arrows), before arrival of the wave front moving around the right end
of the line. The distal side of the rest of this complex line of block
was activated by wave fronts moving around both its right and
left ends (curved arrows, isochrones 100 to 240). Fig 9B
illustrates the initiation of the first nonstimulated beat. The time
window of the map overlaps Fig 9A
; the 10-ms isochrone in Fig 9B
is
equal to the 110-ms isochrone in Fig 9A
. The wave front at the
right moves antidromically to reexcite the proximal side of the line of
block after 80 ms at the asterisk (activation time 82). Despite
reexcitation of the proximal side at the basal margin, the exit route
to the rest of the ventricles was closer to the LAD margin of the
electrode array (near circled activation times 110). The onset of the
QRS in the ECG (not shown) occurred at time 110 ms. Excitation
continued to rotate around the line of block at the right
(isochrones 90 to 150, curved arrows). The orthodromic conduction
time from time 10 ms (near the stimulus site) to time 138 ms (distal to
the right edge of the line of block) in Fig 9A
was 128 ms. The
antidromic conduction time from time 38 in Fig 9B
(which is the same as
time 138 in Fig 9A
) to time 110 (near the stimulus site) was 72 ms.
Therefore, at this premature coupling interval (170 ms),
V2T1 was 200 ms. Fig 9C
shows the pattern of
propagation of a premature impulse with a short coupling interval of
140 ms. The location, shape, and size of the line of block were similar
to the longer coupled premature impulse (Fig 9A
). Activation occurred
around the rightmost branch of the line of block (isochrones 40 to
110) to activate its distal side between 149 and 153 ms
(circled). However, in contrast to the long coupled premature impulse,
the distal side of the line of block closer to the LAD margin was
activated slightly earlier (asterisk, 141 ms circled) by a wave
front that moved to the left around the line of block. Isochrone 10
in Fig 9D
is the same as isochrone 120 in 9C and shows the
initiation of the nonstimulated response. Reactivation of the proximal
side of the line of block started close to the LAD margin of the
electrode array (asterisk and circled activation times 21 and 18). The
exit route was at the LAD margin of the electrode array (the onset of
the QRS of the ECG occurred at time 35 ms), similar to the exit route
for the longer coupled premature impulse (Fig 9B
). However, the time of
antidromic activation of the proximal side to the exit point (at the
LAD margin of the electrode array) was shorter for the shorter coupling
(139 ms) than for the longer coupling interval (200 ms). As a
consequence, the relationship between V1V2 and
V2T1 was direct.
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| Discussion |
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40% of clinical cases of
VT4 6 7 that all other lines of evidence strongly suggest
are reentrant. Mechanisms that might be responsible for the lack of an
inverse relationship during initiation of reentry had not been
previously determined in clinical or laboratory studies.
Reentrant VT can be induced by programmed electrical stimulation in a
canine model of 4-day-old healing myocardial
infarction.8 9 The reentrant circuits causing
tachycardia often occur in a narrow epicardial rim of
surviving muscle, the EBZ, and propagation in the circuits can be
mapped.9 15 16 We investigated whether an inverse
relationship occurred during initiation of VT in this model and did not
find one. In fact, the relationship was always direct; as the coupling
interval of the premature impulse to the basic impulse decreased, so
did its coupling to the first impulse of the tachycardia
(Fig 2
). By necessity, these measurements could only be made in a
subset of the total number of hearts with tachycardia,
those in which tachycardia could be induced by single
premature impulses over a wide range of coupling intervals and complete
reentrant circuits could be mapped. In addition, we chose only those
examples in which the QRS complex of the first tachycardia
beat was the same for all coupling intervals, as has usually been done
when inverse relationships are sought during the initiation of clinical
VT. This characteristic suggests that the initiating series of
premature impulses might have traveled through the same reentrant
circuit, although this supposition turned out to be incorrect (see
below).
On a macroscopic level that could be resolved by the spatial resolution
of the electrode array, there were two different patterns of activation
that resulted in the direct relationship. In the first pattern (Figs 3 through 5![]()
![]()
), premature impulses with different coupling intervals to the
basic impulse blocked in the orthodromic direction in a similar region
of the EBZ. The premature wave fronts conducted around the ends of the
line of block to activate its distal side also similarly for
different coupling intervals. The premature wave fronts then propagated
antidromically past the region in which orthodromic block had occurred
to reexcite myocardium on the proximal side before exiting
the circuit to cause the first impulse of tachycardia. This
pattern of initiation has been described in previous
publications.9 15 16 17 Orthodromic conduction block has been
attributed to prolonged refractory periods of the EBZ17
but also may involve its anisotropic properties.9
Orthodromic conduction time to the distal side of the line of block
prolonged with increasing prematurity because of slowing of activation,
as if the premature impulse were conducting in progressively more
refractory myocardium, and because of lengthening of the
line of block. What was not expected was the characteristics of
antidromic conduction of the premature impulse to complete its transit
through the reentrant circuit. At relatively long premature coupling
intervals, antidromic activation took a long time, whereas at shorter
coupling intervals, this time decreased. There are several possible
interpretations for this observation. Because a large number of
isochrones needed to be interpolated in this region of antidromic
activation at long coupling intervals (Fig 3C
), antidromic conduction
block may have occurred in the most superficial epicardial cell layers
where the recording electrodes were located, because of
insufficient recovery time from the orthodromic activation. However,
because antidromic activation always continued away from this region in
the same direction in which the impulse was propagating when it entered
it, to complete the reentrant circuit, it seems likely that the impulse
was able to bypass this region of block in the epicardial layers
through alternative pathways involving deeper layers or tracts of
surviving myocardial cells. This possibility is favored by the location
of the line of block toward the margin of the EBZ, where its thickness
increases substantially and where there might be intramural
connections.18 19 Intramural reentry has previously been
shown to occur at the margins of the EBZ.20 The
electrograms recorded just proximal to this region of antidromic
activation showed a double deflection separated by an isoelectric
interval proportional to the activation delay (Fig 4
). The first
deflection in the double potential most likely resulted from activation
of the myocardium on the distal side of the line of block,
because the time of its occurrence followed closely the activation of
other electrodes in the conduction pathway of the premature impulse.
The second deflection in the double potential occurred nearly
simultaneously with activation by the antidromic impulse at
electrodes on the proximal side of the line of block. The isoelectric
interval between deflections occurred during the delay between
activation on the distal side and the proximal side, during which the
premature wave front may have been propagating through deeper
myocardium out of the recording field of the
surface electrodes. Early coupled premature impulses, because of
increased orthodromic delay before they reached the distal side of the
line of block, in fact arrived at the distal side slightly later than
the long coupled premature impulses, allowing the
myocardium at the line of block more time to recover. In
addition, a shorter action potential duration resulting from
orthodromic propagation up to the line of block for shorter coupled
premature impulses21 may facilitate more rapid recovery of
excitability. Because of the increased time for recovery at the line of
block, antidromic activation through this region was much more rapid
and might involve more superficial epicardial pathways. The more rapid
antidromic activation of the region in which the line of block was
located was accompanied by the diminution or disappearance of the
double potentials (Fig 4B
). An alternative explanation for the slow
antidromic activation of long coupled premature impulses is that there
was very slow conduction through the region of block that did not
involve alternative pathways, because the myocardium in
this region had only barely recovered excitability by the time the
premature impulse reached the distal side. If the refractory period in
this region is longer than elsewhere in the border zone,17
such delayed recovery would be expected. However, one would also expect
to see low-amplitude, fractionated electrograms rather than double
potentials with an isoelectric segment, if such slow conduction
occurred,22 unless early premature excitation of the
distal side of the line resulted in very slow antidromic propagation of
nonregenerative graded response,23 in which case no
activity might be detectable between the two deflections.
A second type of activation pattern associated with a direct
relationship during initiation of reentry was a macroscopic change in
the activation pattern of the premature impulse detectable with the
resolution of the mapping electrode array, even though the exit route
and the QRS morphology remained unaltered. In some of these
experiments, there was a decrease in the time for orthodromic
activation of the distal side of the line of block with decreasing
coupling intervals of the premature impulse (Figs 6 through 8![]()
![]()
). The
decrease in time was a result of a decrease in the length of the
pathway traveled by the premature impulse to the distal side of the
line of block. Premature impulses with shorter coupling intervals
propagated orthodromically through a small segment of the large region
over which longer coupled premature impulses blocked (Fig 8A
). Even
though the activation time of this region was long, the distal side of
the line of block was still activated earlier than by the
longer coupled premature wave fronts that reached the distal side only
by propagating around the ends of the line of block. Here again, it is
likely that deeper layers of surviving myocardial cells may have
provided alternative pathways of conduction for the shorter coupled
premature impulses to the distal side of a line of superficial
epicardial block and that orthodromic conduction velocity may have been
faster than it appeared on the epicardial surface. Alternatively, more
slowly propagating early premature impulses might provide additional
time for recovery of critical sites within the zone of block, allowing
orthodromic propagation through the line of "block" (compare Figs 6B
and 8A
). However, fractionated electrograms, which would be expected
to occur if this were the case (see above), were not observed (Fig 7
).
As a result of the altered orthodromic propagation for the shorter
coupling intervals, the size of the reentrant circuit appears to be
smaller than for the longer coupling intervals (Fig 8B
). In other
experiments, such as the one shown in Fig 9
, orthodromic conduction of
early and late premature impulses occurred around the ends of the line
of block, but antidromic propagation to the same exit site occurred at
different regions of the block line. A shorter distance between the
site of antidromic activation and the exit site for earlier premature
impulses accounted for the direct relationship of
V1V2 to V2T1 (Fig 9
).
The absence of an inverse relationship in this experimental model does not mean that the concept of the association of an inverse relationship with the initiation of reentry is incorrect. This animal model may not be an accurate representation of clinical events, and the results may apply only to anisotropic reentry. However, the results do show some possible and previously unrecognized causes for the absence of an inverse relationship. An inverse relationship would most likely exist if the reentrant circuit was a fixed anatomic pathway and the region in which orthodromic block of premature impulses occurs is fully recovered by the time the distal side of the line of block is activated over the full range of premature impulses that initiate reentry. In this situation, increased conduction slowing in any part of the reentrant circuit that is expected to accompany increased prematurity would be manifested as an increase in transit time of the premature impulse around the entire circuit and an increased interval between the initiation of the premature impulse and the first impulse of the tachycardia. There would be no cause for decreased antidromic conduction delay with increased prematurity, because no alternative conduction pathways would be available. Therefore, the occurrence of an inverse relationship in some cases of clinical VT and its absence in others might indicate a different mechanism for reentry, with anatomic reentry favoring an inverse relationship and functional or anisotropic reentry not favoring an inverse relationship. In addition, the oc- currence of a direct relationship in clinical studies on VT is not sufficient, by itself, to discount a reentrant mechanism.
| Selected Abbreviations and Acronyms |
|---|
|
| Acknowledgments |
|---|
Received April 7, 1997; revision received June 5, 1997; accepted June 19, 1997.
| References |
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