(Circulation. 2000;102:2650.)
© 2000 American Heart Association, Inc.
Basic Science Reports |
From the Department of Cardiology, Leiden University Medical Center (M.J.S.), and the Department of Physiology, Cardiovascular Research Institute, Maastricht University (L.B., M.H., M.A.A.), Netherlands.
Correspondence to Martin J. Schalij, MD, Leiden University Medical Center, PO Box 9600, 2300 RC Leiden, Netherlands. E-mail m.j.schalij{at}lumc.nl
| Abstract |
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Methods and ResultsA Langendorff-perfused epicardial sheet (1.0±0.4 mm, n=35) was created by freezing the intramural layers of the rabbit left ventricle. Epicardial activation maps were constructed by use of different high-resolution mapping arrays connected to a mapping system. In 5 experiments, monophasic action potentials were recorded. In the intact left ventricle, no arrhythmias except VF could be induced. After freezing, programmed electrical stimulation or rapid pacing led to the induction of sustained VT (cycle length 130±11 ms). VT was caused by reentry around a functional line of block oriented parallel to the epicardial fiber direction. Action potential recordings demonstrated that the central line of block was kept refractory by electrotonic currents generated by the depolarization waves propagating at either side of the line of block. At the pivot points of the line of block, the pronounced curvature of the turning wave and abrupt loading changes created an excitable gap of 30 ms in the reentrant pathway.
ConclusionsIn uniform anisotropic myocardium, reentry around a functional Z-shaped line of block may occur. The core of the circuit is kept refractory by electrotonic currents. The pronounced wave-front curvature and abrupt loading changes at the pivot points cause local conduction delay and create a small excitable gap.
Key Words: anisotropy reentry tachycardia electrophysiology
| Introduction |
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This study was performed to determine the influence of uniform anisotropy on functional reentry. To avoid confounding ischemic alterations, we used a 2D preparation of perfused left ventricular epicardium.9 11 18 19
| Methods |
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Experimental Model
To create a 2D preparation, the endocardial and intramural
layers of the left ventricle (LV) were cryoablated by freezing with
liquid nitrogen (-192°C). Cryoablation resulted in a surviving
epicardial layer 1.0±0.4 mm thick. Epicardial conduction velocity
and refractory period were not affected by the freezing
procedure.9 An extensive evaluation of this preparation
has been given previously.9 19
Mapping System
Unipolar electrograms were recorded with the stainless steel
aortic cannula used as indifferent electrode. After amplification and
filtering (bandwidth 1 to 400 Hz), the signals were multiplexed
(sampling rate 1000 Hz), digitized (8 bits), and stored on
tape.19 Local activation times were detected
automatically. In case of fragmented electrograms, the component with
the steepest negative slope was taken as the actual local activation
time.
The hearts were stimulated with a pulse width of 2 ms by a constant-current stimulator (Medtronic). The output of the stimulator could be connected to any pair of electrodes in the mapping array (regular pacing: stimulus strength, 2 times diastolic threshold; premature stimuli: 4 times diastolic threshold). During VT, reset curves of several recording sites were obtained by premature stimulation at decreasing coupling intervals (V1S). At the pacing site, the V2V3 interval represents the return cycle of the premature stimulus.
Total epicardial mapping was performed with a "spoon-shaped" electrode (384 silver electrodes, diameter 0.3 mm, resolution 2 mm) covering the apex and entire free wall of the LV. For high-resolution mapping of part of the epicardium, a rectangular (13x15-mm) array containing 192 silver electrodes (diameter 0.3 mm, interelectrode distance 1 mm) was used. A double-row electrode of 2x48 electrodes (diameter 0.05 mm, interelectrode distance 0.185 mm) was used to map the central line of block.
Action Potential Recordings
Monophasic action potentials (MAPs) were recorded by use of
standard microelectrode techniques (glass capillaries filled with 3
mol/L KCl and a tip resistance of 10 to 30 M
).3 The
microelectrode was impaled in the core of the circuit at 0.5-mm
intervals with an electrically driven micromanipulator. Because of
mechanical movement of the 2D layer, the tip of the microelectrode
frequently broke during the first impalement. However, MAPs of lower
amplitude could still be recorded, allowing reliable evaluation of
the shape and duration of the local action potentials. During MAP
recordings, a bipolar electrode sutured to the LV served as
time reference.
| Results |
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Sustained VT
During VT, single-loop reentry was present in 28 of 30
preparations. In 2 cases, a figure-8 reentry was found. In Figure 3
, VT maps of 4 different hearts are
shown. The upper panels show 2 examples of counterclockwise reentry.
The lower left panel represents a clockwise VT, and the lower
right panel shows a figure-8 reentry. The conduction velocity along the
circuit varied with the fiber orientation. Longitudinal conduction
velocity was 60 cm/s. Transverse conduction velocity at the pivot
points was <20 cm/s (Figure 4
). In 75%,
the line of block (length 20±5 mm, CL 129±20 ms) was oriented
parallel to the fiber direction (Figure 5
). In 25%, the line of block was
L-shaped (lower panel). The length of the L-shaped lines of block
(19±16 mm) and the CL (123±4 ms) were not different from the
longitudinally oriented lines.
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During VT, it was possible to capture the myocardium with
single stimuli, elucidating an excitable gap of 30±7 ms. However,
although premature stimuli (Figure 6
)
captured the myocardium, they did not reset VT, indicating
that an excitable gap was present only in parts of the circuit. MAP
recordings (see below) showed that the excitable gap was absent
at the pivot points of the circuit.
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Extracellular electrograms were recorded across the line of block
(n=10) with the double electrode. Figure 7
shows a clockwise circuit. The
electrograms in 7B were recorded from the center of the line of
block. At the line of block, double potentials were recorded,
reflecting the 2 wave fronts propagating in opposite directions at
either side. An isoelectric segment was present between the 2
potentials; the absence of fragmented potentials indicates that slow
conduction across the line of block did not occur. Because multiple
fragmented potentials are considered to be the hallmark of nonuniform
anisotropy, the absence of multiphasic deflections in the extracellular
waveforms recorded across the line of block demonstrates the
uniformly anisotropic nature of the tissue. Near the pivot point (7A),
the interval between the double potentials shortened. At the pivot
point (7C), single potentials were recorded together with a
low-amplitude electrotonic potential. Proximal to the pivot points, the
local deflection preceded the electrotonic potential, whereas distal to
the pivot points, local activation occurred after the electrotonic
potential.
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Monophasic Action Potentials
MAPs were recorded in 5 hearts. A detailed map showing reentry
around a Z-shaped line of block could be constructed in 3 experiments;
in the other 2 experiments, only incomplete maps could be
constructed.
In Figure 8
, clockwise reentry around a
Z-shaped line of block (thick line) caused VT. Normal MAPs, without
steps in the depolarization phase or electronic humps during the
repolarization phase, were recorded along the circuit. A short
(30-ms) isoelectric segment was present between the action
potentials, indicating complete repolarization and a gap of full
excitability. Recordings obtained across the center of the line
of block (Figure 9
) showed a phase shift
of 180° between the opposite limbs. Low-amplitude electrotonic
potentials were recorded at the line of block with a total width of
1.5 mm, showing that the central line of block was kept
nonexcitable by electrotonic current flowing between the opposed limbs
of the circuit. This electrotonic current kept the cells depolarized,
although sometimes the nonexcitable core was excited (Figure 10
, electrodes 3 and 4). Because of
electrotonic prolongation of the action potentials, the cells at the
central line of block thus responded in a 2:1 or 3:2 manner to the
circulating impulse. At the pivot points, the potentials were clearly
prolonged but still responded in a 1:1 manner (Figure 10
, electrodes 1, 2, 9, and 10). The short limbs of the Z-shaped line of
block (Figure 11
) were a result of 2
mechanisms. First, clear steps in the depolarization phase of the
action potentials occurred at the pivot points (Figure 11
, electrodes 3 to 5 and 9 to 11). This interruption of the rapid
depolarization is explained by the high current drain encountered by
the transverse conducting impulse when, after crossing the line of
block, it had to activate the longitudinal limbs of the circuit
(along the longitudinal fiber axis). Second, because of this
delay in propagation, the duration of the action potentials proximal to
the pivot points was electrotonically prolonged (Figure 11
, electrodes 1, 2, 7, and 8). In contrast to other parts of the circuit,
no isoelectric segment was present, and the next depolarization
occurred immediately after the cells were repolarized (no phase 4).
Approximately 2 mm distal to the turning points (Figure 11
, electrodes 6 and 12), the depolarization showed no steps,
and the action potentials exhibited a clear excitable gap. The short
limbs of the Z-shaped line of block thus were caused by discontinuous
propagation due to the interplay between the anisotropic tissue
properties and the curvature of the turning wave front.
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| Discussion |
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Line of Block
Activation maps obtained during initiation of VT did not reveal
large anatomic obstacles. Only after application of shortly coupled
premature stimuli did local conduction block develop. During VT (75%),
the impulse circulated around a line of block oriented parallel to the
epicardial fiber direction. In 25%, the line of block was oriented in
a different direction or related to an epicardial blood vessel.
Microelectrode recordings revealed that the longitudinal block lines were in fact Z-shaped. When the central line of block was oriented parallel to the fiber orientation, the extracellular waveforms recorded across the line of block showed double potentials without the characteristic multiphasic components as found in the central line of block of VT in infarcted tissue.11 Together with the transverse electrotonic interaction over 1.5 mm, this rules out a longitudinal side-to-side uncoupling of fibers occurring in nonuniform anisotropic preparations. In our preparation, the effective transverse space constant was much higher than the space constant in nonuniform anisotropic tissue. This implies a major difference between the central line of block in uniform anisotropic tissue and the very slow transverse conduction zones identified during VT in infarcted tissue.11 13 18
Several mechanisms were involved in the creation of the Z-shaped line of block. As in the computer simulations by van Capelle and Durrer21 and reentry within small pieces of atrial myocardium,1 the core of the circuit was kept nonexcitable by electrotonic current from the longitudinal limbs of the circuit at either side of the central part of the Z line. The low-amplitude electrotonic potentials visible in the recordings from these sites prevented activation of the center of the circuit.
Depending on the amount and timing of these currents, some sites within the core of the circuit were activated in a 2:1 or 3:2 manner. At the pivot points, the curvature of the circulating wave front is high. Because a convex wave front must excite more tissue ahead than a planar wave front, the excitatory current is dissipated, and consequently, a curved wave front propagates at reduced speed. Above a certain critical curvature, the current drain becomes so high that conduction block occurs despite full excitability of the tissue ahead.16 22 At the pivot points, the impulse made a sharp U turn, first changing its direction from longitudinal to transverse propagation and then back to longitudinal. The current drain during the transition from transverse to longitudinal propagation resulted in delayed activation and created the short limbs of the Z-shaped line of block.
Excitable Gap
Originally, reentry involving a functional block was thought to
have only a partially excitable gap because of the tight fit between
the crest and the tail of the reentrant wave.1 Later, it
was recognized that during functional reentry, an excitable gap might
exist.12 13 23 In this study, an excitable gap of 30 ms
was present during functional reentry. Several mechanisms
contributed to the creation of this excitable gap. First, microscopic
barriers may anchor the functional circuit at a fixed position. Such
barriers may arise when adjacent fibers become separated by
interposition of collagenous septa.24 25 Although during
pacing, no indication for fixed conduction barriers were found, it
cannot be excluded that small barriers provide stable pivot points for
the anisotropic circuit. Also, during functional reentry, local
conduction delay at the pivot points may create an excitable
gap.22 23 As shown, at the pivot points, propagation
temporarily stopped, resulting in a step in the depolarization phase of
the action potentials. Activation of the longitudinal limbs occurred
only after the wave had made a wider turn.22 The
conduction delay of 30 ms at the pivot points resulted in an excitable
gap in other parts of the circuit and caused a clear difference in
activation at either side of the pivot point. This resulted in a
prolongation of the action potentials proximal to the pivot
points by current flowing during the repolarization phase from cells
distal to the pivot points (which are still depolarized because they
were activated later).26 27 The electrotonic
prolongation of the action potentials proximal to the pivot points
closed the excitable gap at the beginning of the U turn and contributed
to the stability of the pivot points. The excitable gap during
anisotropic reentry thus is caused primarily by local conduction delay
at the pivot points due to the curvature of the turning wave front and
the low longitudinal resistance (resulting in a high current drain) at
the exit of the pivot points. Because the action potentials at the
entrance of the pivot points were prolonged, premature activation of
the pivot points was not possible. This explains why it was not
possible to reset VT with single stimuli. Although it was possible to
capture the myocardium, the reentrant wave was forced to
turn around the pivot points because no excitable gap was present
at these sites.
Functional Reentry
Three types of functional reentry have been distinguished so far.
During leading-circle reentry, the core of the circuit is formed by
centripetal wavelets colliding in the center of the
circuit.1 The reentrant pathway is determined by the
smallest circuit in which the wave front can circulate. Because the
head of the impulse propagates in just recovered
myocardium, only a small partially excitable gap exists,
and the CL is determined mainly by the refractory period of the
tissue.1 Only in case of an extreme shortening of the
action potential may the circuit become so small that the high
curvature of the wave front limits a further shortening of the circuit,
thus creating an excitable gap.21 28 Similar to
leading-circle reentry, during anisotropic reentry, the 2 opposed
longitudinal limbs of the circuit cannot reexcite each other, because
they are mutually refractory. Instead, the central line of block is
continuously depolarized by electrotonic current flowing between the
depolarizing waves passing at either side. During anisotropic reentry,
a clear excitable gap exists, caused by conduction delay at the pivot
points. Because of the existence of an excitable gap, anisotropic
reentry is anchored at a fixed position and long-lasting. The stability
of anisotropic reentry is enhanced by the electrotonic prolongation of
the action potentials at the entrance of the pivot points, thereby
acting as functional anchoring points. At the pivot points, no
excitable gap is present, and the circulating impulse is unable to
short-circuit the reentrant pathway. In nonuniform anisotropic
myocardium, the transverse conduction velocity may be <5
cm/s, and the conduction delay at the transverse pivot points may be
larger than in uniform anisotropic
myocardium.6 8 13 Consequently, the line of
block shortens, and the impulse rotates around a small functional
fulcrum.8 13
Self-sustained rotating spiral waves can occur in any excitable medium.14 Because of the pronounced curvature of the wave front, at the tip of the spiral, the current load is high and the safety factor for conduction may become <1.15 16 17 22 29 Therefore, the core of a spiral wave, although fully excitable, is not excited.16 29 However, it is questionable whether the core of a spiral wave in cardiac tissue is fully excitable.16 As in leading-circle and anisotropic reentry, the center of a spiral wave will be depolarized electrotonically by the cells around the core. In fact, recordings obtained from the core of a spiral wave clearly show multiple low-amplitude potentials.16 This suggests that the core is kept depolarized above its threshold for excitation by the depolarization wave wrapped around it. As in anisotropic reentry, an excitable gap is present, caused by the curvature of the turning wave preventing it from approaching closer to its tail of refractoriness.22
Clinical Implications
Reentry is the mechanism of most VT after myocardial infarction in
patients. Surviving nonuniform anisotropic cell layers within the
infarcted myocardium play a key role in the induction and
perpetuation of reentry.11 25 Although the structure of
these surviving cell layers will be more complex, the model of
anisotropy presented in this study may be useful to study the
mechanism of VT in anisotropic myocardium.
Limitations of the Study
Although activation maps during pacing did not reveal anatomic
obstacles, histological studies were not performed to
confirm the electrophysiological data.
Therefore, it could not be excluded that microanatomic lesions served
to anchor the pivot points and determined the length of the central
line of block during VT.
Conclusions
In uniform anisotropic myocardium, reentry around a
functional Z-shaped line of block may occur. The central line of block
was kept depolarized by electrotonic currents flowing between the
depolarization waves at either side of the line of block. At the pivot
points, the pronounced wave-front curvature and the high current drain
along the longitudinal axis caused local conduction delay, thus
creating an excitable gap. The mechanisms involved are not fully
understood and warrant further study, however, and detailed descriptors
of anisotropic resistive properties at each size scale are needed.
Received March 21, 2000; revision received June 15, 2000; accepted June 21, 2000.
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