From the Center for Experimental Cardiac Electrophysiology, Section of
Cardiology, Department of Medicine, Baylor College of Medicine, Houston, Tex.
Correspondence to Dirar S. Khoury, PhD, The Methodist Hospital, 6565 Fannin St, M941A, Houston, TX 77030. E-mail dkhoury{at}bcm.tmc.edu
Methods and ResultsA 128-electrode probe was inserted into the
intact canine LV. Probe unipolar electrograms were
simultaneously acquired during sinus, artificially paced,
and spontaneous premature beats. Representative
endocardial electrograms were measured directly using eight needle
electrodes (the "gold standard"). A probe-cavity realistic,
three-dimensional geometric model was constructed using two-dimensional
epicardial echocardiography. Boundary element
methods and numeric regularization were used to compute electrograms at
194 sites on the endocardium. In eight pacing protocols, computed
endocardial electrograms correlated well with directly measured
electrograms (r=.88). Corresponding activation times
were also in agreement with those determined from measured endocardial
electrograms (activation error, 4.7 ms). The earliest region of
activation was invariably in the vicinity of the pacing needle (spatial
error, 9.2 mm). Subsequently, the site of origin of
ischemia-induced spontaneous ventricular premature
beats and the ensuing sequence of depolarization was identified.
ConclusionsNoncontact mapping provides realistic,
three-dimensional electrophysiological
images of the endocardium, on a beat-by-beat basis, that localize the
sites of origin of premature beats and reconstruct their activation
sequences.
In patients with ischemic heart disease, the earliest site of
activation during monomorphic ventricular
tachycardia has often been located on the endocardial
surface of the left ventricle (LV).5 Furthermore,
because the endocardium is more safely accessible than the epicardium,
most electrophysiological mapping
techniques have focused on endocardial approaches. However, current
techniques of mapping the endocardium have certain limitations.
Traditional electrode-catheter mapping performed during
electrophysiology procedures is confined to a limited number of
recording sites, is time consuming, and is carried out over
several heartbeats without accounting for possible beat-to-beat
variability in activation.6 On the other hand,
although recently introduced multielectrode
basket-catheters7 8 measure endocardial
electrograms at multiple sites simultaneously by expanding
the basket inside the heart so the electrodes are in direct contact
with the endocardium, the system is limited to a fixed number of
recording sites, may require multiple deployments for
recording additional sites, and may result in complications
such as irritation of the myocardium and difficulty in
collapsing and withdrawing the basket.
Earlier, an alternative mapping approach was introduced that used a
cavitary noncontact multielectrode
catheter-probe.9 The probe measures cavitary
electrical potentials (electrograms) from multiple directions
simultaneously and can be easily inserted into the
blood-filled cavity without occluding it. Unlike the basket, however,
the probe is not necessarily in direct contact with the surface of the
endocardium. Theoretical and experimental models have shown that
noncontact sensing by the probe results in low-amplitude and
smoothed-out electrical potential patterns.10 11
Recently, endocardial surface potentials and activation sequences have
been mathematically computed, during selected intervals, from measured
cavitary probe electrograms (the "inverse problem") in the
isolated, Langendorff-perfused canine LV.12 More
recently, endocardial electrograms have been computed in the same
model.13 The computed electrograms successfully
identified the sites of origin of artificially paced ectopic foci and
further demonstrated the potential clinical applicability of the
technique for routine electrophysiology procedures without the use of a
basket-catheter or the need for surgery. However, this initial study
was limited to controlled paced rhythms, the probe-cavity geometric
model was approximated manually after the completion of the experiment,
and the number of sampling points on the endocardium were limited to
the same number of probe electrodes.
The objectives of the present study were (1) to develop and test
mathematical and experimental methods to compute
simultaneous endocardial surface electrograms and
activation sequences at multiple sites, on a beat-by-beat basis, from
cavitary electrograms measured with a noncontact multielectrode probe
in the intact canine LV, and (2) to use epicardial
echocardiography in situ to construct
high-resolution, realistic, three-dimensional
electrophysiological images of the LV
during sinus as well as artificially paced control rhythms and, for the
first time, during ischemia-induced spontaneous premature
depolarization.
Experimental Model
Electrogram Potential Measurement
Endocardial electrograms were directly measured from eight
representative sites through the use of needle
electrodes (Fig 1B
Geometry Measurement
Six parallel short-axis planes (8-mm separation) of the probe-cavity
geometry were acquired that depict the LV from apex to base (Fig 3
To identify the role of geometry, an idealized, three-dimensional model
of the probe-cavity geometry was constructed by
representing the LV endocardial surface as an ellipsoid, of
similar major and minor axes, with the probe located concentrically
inside the cavity (Fig 4
Electrophysiology Protocols
Once all pacing protocols had been completed, the left anterior
descending coronary artery was ligated at a point just above
the first diagonal branch near the base of the heart. Approximately 15
minutes after occlusion, spontaneous ventricular premature
depolarizations were observed in the surface ECG, and for the first
time, representative cavitary and endocardial
electrograms were simultaneously recorded. The dog
subsequently developed ventricular fibrillation.
After the experiment, the heart was fixed in formalin.
Histological examination was performed to determine
myocardial fiber direction at the pacing sites as well as the site of
spontaneous ventricular premature depolarization.
Histological sections, parallel to the epicardium, were
obtained in epicardial, midwall, and endocardial regions.
Data Acquisition, Processing, and Display
Using probe electrograms and probe-cavity geometry, endocardial surface
potentials were computed at each of the 194 endocardial nodes for any
instant of time. Because the number of nodes on the endocardial surface
was twice the number of nodes on the probe, endocardial potentials were
computed in two steps. The endocardium was divided into two intertwined
surfaces, each composed of 98 nodes (same number of nodes on probe
surface). For any time frame, electrical potentials were computed on
each surface separately using the previously described equation
(A=98x98), and the results were then merged to produce a complete
high-density image of endocardial potentials. High sampling with 194
nodes provided better spatial resolution than that with 98 nodes. The
average distance between the pacing sites and immediate neighboring
nodes on the endocardium (ie, circumferential resolution) was 6.7
mm for the 194-node mesh, whereas the resolution was 12.9 mm for
the 98-node mesh.
Endocardial electrograms were constructed by computing the potentials
every 1 ms over a duration of 100 ms. During periodic rhythms,
electrograms were computed for 10 consecutive cardiac cycles, and the
results were temporally averaged.
Isopotential and isochrone contour maps were superimposed on a
realistic three-dimensional endocardial surface as seen from the
epicardial side. A primary potential minimum in the isopotential map
was defined as the earliest nadir of the negative potential region
reaching -5 mV during ventricular depolarization.
Activation times were determined from unipolar endocardial electrograms
by determining the time of occurrence of the negative peak of the first
derivative of QRS. During paced rhythms, the beginning of the pacing
stimulus was selected as the reference point.
Results of all 8 pacing protocols are summarized in Table 1
Isopotential contour maps of endocardial potentials computed early
after pacing are shown in Fig 6A
Histological sections of the LV in the apical pacing
regions showing fiber direction are provided in Fig 6E
Maps of isochrones (activation maps) determined from computed
electrograms are shown in Fig 7
Spontaneous Ventricular Premature Depolarization Versus
Sinus Rhythm
Endocardial electrograms were initially computed during 5 sinus rhythm
beats preceding 5 ventricular premature depolarizations.
Compared with endocardial electrograms measured at the same 8 sites in
Fig 5
Isopotential contour maps of endocardial potentials computed during
sinus rhythm are shown in Fig 10
Unlike sinus rhythm, the initial primary potential minimum (potential
<-5 mV) appeared during spontaneous ventricular premature
depolarization in high anteroseptal region just below the mitral valve
(Fig 11A
Role of Geometry
The present study confirmed that LV wall pacing
consistently gave rise to a potential minimum during early
activation that was invariably in the vicinity of the pacing
electrode.21 Paced rhythms served as controls for
subsequent analysis of intrinsic sinus and spontaneous
premature beats. During pacing, electrograms computed on the
endocardial surface were in excellent agreement with electrograms
measured directly at selected sites (8 sites) on the endocardium
(r=.88). Furthermore, activation times determined from
computed electrograms correlated well with those determined from
measured electrograms (average error, 4.7 ms). Earliest region of
activation in isochrone maps, determined from computed
electrograms, envelope the pacing site, with the earliest site of
activation always in close proximity to the pacing site (average
spatial error, 9.2 mm). It should be noted that these
discrepancies were determined assuming that recordings obtained
with the endocardial needle electrodes represented the gold
standard, ignoring possible measurement or spatial errors in the
needles.
The spatial distribution of reconstructed endocardial potentials
(position and orientation of initial maxima and minima) reflected
underlying cardiac fiber direction. This result was consistent
with previous studies identifying the effect of myocardial anisotropy
(fiber direction) on propagation of excitation wave fronts and on the
ensuing potential distribution.12 22 Due to
anisotropy, ectopic excitation spread faster in a direction parallel to
cardiac fibers than perpendicular to them. As a result, this generated
potential maxima in the areas toward which excitation propagated along
fibers, thereby reflecting fiber direction at the level of the ectopic
event within the myocardium.
For the first time, endocardial electrograms were computed in the
present study during sinus rhythm. Similar to artificially paced
ventricular rhythms, electrograms computed during intrinsic
sinus rhythm correlated well with endocardial electrograms measured at
8 selected sites. More importantly, the reconstructed sequence of
depolarization during sinus rhythm was consistent with
published reports on the overall pattern of LV
activation.23 24 Detailed mapping studies by
Durrer et al24 on isolated human hearts showed
that endocardial areas that activate early include the
posterior paraseptal area at about one third the distance from apex to
base and the anterior paraseptal area toward the apex. Furthermore,
areas of early activation become confluent at 15 to 20 ms, and the
latest part to be activated is the posterobasal area. This
apparent initial scattering of the wave fronts at different sites,
before merging with one another, was similarly described by Arisi et
al25 by recording potential fields on the
ventricular epicardial surface of the exposed canine heart
during sinus rhythm. The depolarization at different sites was perhaps
a reflection of the underlying bifascicular nature of the left bundle
branch of the Purkinje system.26
Recently, analysis of cavitary electrograms was conducted
before and after experimental myocardial infarction produced by
occlusion of the left anterior descending coronary
artery.27 More recently, the use of an
electrocardiographic inverse solution, coupled with body surface
potential mapping, was demonstrated in localizing acute
ischemia in patients undergoing percutaneous
transluminal coronary angioplasty.28 For
the first time, endocardial surface electrograms were computed in the
present study during ischemia-induced spontaneous
ventricular premature depolarization. The objective of the
study was not to fully describe the mechanism of arrhythmogenesis or
underlying tissue electrophysiology but rather to substantiate the
quality of the computed potential patterns and sequence of
depolarization during spontaneous premature depolarization. Computed
endocardial electrograms were in excellent agreement with measured
electrograms. Furthermore, the site of origin of the initial primary
potential minimum and the subsequent sequence of depolarization were
distinctly different from those computed in the preceding sinus rhythm
cycle. Consistent with previous
reports,29 30 this site of origin was in the
vicinity of the area of occlusion of the coronary artery. The
LV endocardium required a longer time to completely depolarize compared
with sinus rhythm. Unlike sinus rhythm, which is initiated by the rapid
conduction system, activation initiated by spontaneous
ventricular premature depolarization may have originated
from an epicardial site. This was corroborated by the similarity
between the alignment of the initial maximum and minimum potentials and
the direction of fibers in the epicardial/midwall region. The effect of
myocardial anisotropy on spontaneous premature depolarization was also
consistent with results of artificial pacing.
As described in this as well as previous
reports,12 computation of endocardial surface
potentials requires a knowledge of both cavitary probe potentials and
probe-cavity geometry. Geometry is a requisite to obtain the transfer
relation between the probe and endocardial surfaces (matrix A). In the
present study, the volume conductor geometric model, including
probe position and orientation, were determined in situ, for the first
time, using epicardial echocardiography. Unlike
previous work, the endocardial surface was sampled (discretized) at
twice the number of probe nodes (electrodes). This approach therefore
enabled us to construct
electrophysiological images at higher
spatial resolution. Epicardial echocardiography
used in the present study provided an improved and more accurate
approach in determining the geometry compared with previous
work.12 Yet, to be applicable for use in routine
catheterization procedures, other less invasive
real-time methods for determining the geometry will have to be
implemented.31 32
Endocardial electrograms were in excellent agreement with directly
measured electrograms while using a realistic probe-cavity geometry.
Simplifying the geometry to an ellipsoidal endocardium and a concentric
probe reduced the correlation between computed and measured
electrograms and doubled the discrepancy in activation time. These
results confirm the importance of obtaining detailed
representation of the probe-cavity geometry when computing
endocardial electrograms. Furthermore, idealization of the geometry
almost doubled spatial error in localizing the site of origin of paced
beats. This can lead to misinterpreting features of underlying
activation pattern. Therefore, in situ determination of the geometry is
paramount to successful application of the noncontact mapping technique
in routine clinical catheterization procedures.
Study Limitations
Study Significance
Received May 21, 1997;
revision received September 17, 1997;
accepted September 25, 1997.
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Khoury DS, Marks GF. Mathematical methods for imaging
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© 1998 American Heart Association, Inc.
Basic Science Reports
Three-Dimensional Electrophysiological Imaging of the Intact Canine Left Ventricle Using a Noncontact Multielectrode Cavitary Probe: Study of Sinus, Paced, and Spontaneous Premature Beats
![]()
Abstract
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
BackgroundThe feasibility of
measuring cavitary electrograms using a noncontact probe and
reconstructing endocardial surface electrograms and activation
sequences during paced beats was previously demonstrated in the
isolated canine left ventricle (LV). The objective of the present
study was to develop and test a high-resolution, three-dimensional,
endocardial electrophysiological imaging
technique that simultaneously reconstructs endocardial
surface electrograms and their corresponding activation sequences
during normal and abnormal beats with the use of cavitary electrograms
measured with a noncontact multielectrode probe in the intact canine
LV.
Key Words: electrophysiology endocardium mapping
![]()
Introduction
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
In the United States,
300 000 patients die annually from sudden cardiac death, primarily
due to cardiac arrhythmias (ventricular
tachycardia and ventricular fibrillation).
Current antiarrhythmic pharmacological therapy often is ineffective and
can be proarrhythmic.1 2 With an increased
emphasis on nonpharmacological therapy, catheter ablation has been
routinely used as a safe and effective first-line therapy for managing
supraventricular
arrhythmias.3 However, for ablation to be
clinically successful in managing ventricular
arrhythmias, catheter mapping of brief,
hemodynamically unstable, or polymorphic
ventricular arrhythmias on a beat-by-beat basis and
at multiple simultaneous sites is
required.4 Therefore, the selection of
appropriate pharmacological therapies and the advancement of catheter
ablation techniques for managing ventricular
arrhythmias are contingent on the development of advanced
mapping techniques that enable identification of the mechanisms of
these arrhythmias and localization of their sites of
origin.
![]()
Methods
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
Mathematical Formulation
The electrical potential within the blood cavity, bounded by the
probe surface on one side and the endocardial surface on the other, is
described mathematically by Laplace's
equation.12 13 14 15 To solve this equation in a
realistic probe-cavity geometry, a standard boundary element method was
used.16 The resulting equation is
VP=A·VE, where
VP and VE are values of
potentials at NP and NE
sampling points (nodes) on the probe and endocardial surfaces,
respectively, and A is a matrix (of order
NPxNE) that describes the
geometric relation between the endocardial surface and the probe
surface (including position and orientation within the cavity). The
problem of computing the endocardial potentials in the above equation,
for a given set of measured probe potentials, is ill posed; that is,
small variations in the data VP caused by
measurement noise or errors in determining the geometry result in an
unphysical solution VE. Similar to previous
methods,12 17 a physical solution was obtained by
using the Tikhonov zero-order numeric regularization
technique18 in conjunction with the composite
residual and smoothing operator19 for selecting
the regularization parameter.
A 25-kg mongrel dog was anesthetized with sodium
pentobarbital (30 mg/kg). The dog was intubated and ventilated with
room air with the use of an external respirator. The heart was exposed
through a median sternotomy and suspended in a pericardial cradle. The
study was conducted in accordance with institutional guidelines.
A custom-made cylindrical probe, containing 128 silver
electrodes on its surface arranged in 16 circumferential rings (8
electrodes per ring), was used to measure LV cavitary electrograms. The
probe was 9 mm in diameter, and the distance between the proximal
and distal rings was 60 mm (Fig 1A
).
To minimize motion artifacts, a 5-mm-long needle was fixed at the
tapered tip of the probe. Guided by epicardial
echocardiography, the probe was inserted through a
purse-string suture in the LV apex and positioned along the center of
the cavity, with the tip anchored between the mitral and aortic valves
(Fig 1B
). The 4 proximal rings of electrodes were not completely inside
the cavity and were not used. This resulted in an effective probe of 96
electrodes. To prevent rotation artifacts, the extracardiac portion of
the probe shaft was affixed to the rib spreader.

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Figure 1. A, The 128-electrode probe. B, An intact canine
heart preparation. Probe shaft indicates the apical insertion of the
probe into the left ventricular (LV) cavity. Eight needle
electrodes were inserted into the LV myocardium for pacing
and recording. LAD indicates left anterior descending
coronary artery; RV, right ventricle.
). The needles were 15 mm long and contained 5
electrodes (2-mm interelectrode separation starting from the tip). The
tip electrode protruded slightly into the cavity and was used to
measure endocardial electrograms. Four electrodes along the needle
shaft were used for pacing. Measured endocardial electrograms were used
to evaluate the accuracy of computed endocardial electrograms.
Probe-cavity geometry was determined using two-dimensional
epicardial echocardiography. Similar to previous
work,20 a 5-MHz
echocardiography transducer (model SONOS 1000;
Hewlett-Packard) was hand-held perpendicular against an external marker
that was in turn attached parallel to the shaft of the probe (Fig 2
). The marker contained eight
equidistant points that allowed obtaining parallel images (cross
sections) at fixed distances from one another. The tomographic sections
were aligned using an additional marker placed on the surface of the
probe. These two markers were also used to determine the needle sites
on the epicardium.

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Figure 2. External marker attached parallel to the probe
shaft. An epicardial echocardiography transducer
was hand-held perpendicular to the marker to acquire parallel,
equidistant tomographic sections of the probe-cavity geometry.
). The borders were traced in the
tomographic sections at end diastole in three consecutive
cardiac cycles. The digitized distances were then averaged and used to
construct the realistic, three-dimensional, geometric model. The
probe-cavity geometric model consisted of 12 parallel cross sections.
In each section, the probe contained 8 nodes, whereas the endocardium
contained 16 nodes. The probe and endocardial surfaces were then
constructed by connecting the nodes with triangles (Fig 3I
). Each
surface was artificially closed off by the addition of a node at the
apical and basal ends, giving node totals for the probe and endocardium
of 98 and 194, respectively.

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Figure 3. A through F, Tomographic, short-axis views of
probe-cavity geometry obtained with two-dimensional epicardial
echocardiography. The views, plotted at different
scales, depict the left ventricular (LV) cavity from apex
(A) to base (F). A marker on the probe (+ in B) was used to align the
sections. G, Short-axis view of the mitral and aortic valves, with the
tip of the probe anchored in between. H, Long-axis view of probe and LV
cavity. I, Three-dimensional probe-cavity geometric model. Ao indicates
aortic valve; RV, right ventricle.
). The same
number of sections, nodes, and triangular elements were used on the
probe and endocardial surfaces as in the realistic geometry.

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Figure 4. Idealized probe-cavity geometric model
represented as an ellipsoidal left ventricular
endocardial surface with the probe located concentrically within the
cavity.
Cavitary and endocardial electrograms were initially
recorded during baseline sinus rhythm. Electrograms were then
recorded during LV pacing at 8 subendocardial sites using needle
electrodes (base, 2 sites; midway, 2 sites; and apex, 4 sites). Bipolar
pacing was applied using 4-ms pulses at twice-diastolic
threshold at a cycle length of 300 ms with an external stimulator
(model S8800; Astro-Med).
Multiple unipolar probe and needle (endocardial) electrograms,
along with surface ECGs (leads I, II, and III), were
simultaneously acquired with the use of a 128-channel
cardiac mapping system (CardioMapp; Prucka Engineering) that amplified
and displayed the signals at a 1-ms sampling interval per channel. The
common reference electrode was placed on the right hind leg.
![]()
Results
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
Artificially Paced Ventricular Rhythms
Endocardial electrograms were computed at all 194 nodes using
cavitary electrograms obtained while pacing at 8 different needle
sites. Representative computed electrograms are shown
in Fig 5
(thick tracings) while pacing at
site 7. Electrograms measured simultaneously through the 8
needle electrodes while pacing at the same apical site are also shown
in Fig 5
(thin tracings). As noted from these
representative tracings, there was an excellent
agreement between computed and measured endocardial electrograms, with
a correlation coefficient of .86 to .98. There also was a high
correlation between activation times determined from computed
electrograms and activation times determined from measured endocardial
electrograms. Note that site 7 reflected the earliest activation time
compared with all other sites. Errors in activation time ranged from 0
to 8 ms in Fig 5
.

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[in a new window]
Figure 5. Schematic of anterior left ventricle (LV)
depicting the sites of 8 pacing/recording electrodes. Computed
(thick tracings) and directly measured (thin tracings) endocardial
electrograms are plotted over 100 ms while pacing at site 7.
Electrogram number corresponds to recording site. LAD indicates
left anterior descending coronary artery; Tc, activation time
determined from computed electrogram; and Tm, activation time
determined from measured electrogram.
. Compared with 8 measured endocardial
electrograms, computed electrograms resulted in an overall correlation
coefficient of .88 and error in activation time of 4.7 ms.
View this table:
[in a new window]
Table 1. Computed Endocardial Electrograms With Realistic
Geometry
through
6D). The maps are shown for the 4 apical pacing sites, needles 5
through 8 (Fig 5
). The separation between the needles is 8.8, 10.2, and
20.1 mm, respectively. Primary potential minima appeared at 5 ms
in Fig 6A
, 10
ms in Fig 6B
, 12
ms in Fig 6C
, and 19 ms in Fig 6D
. Note
that a primary potential minimum (depolarization) consistently
initiated in the vicinity of the pacing needle, so four unique sites of
origin could be identified from the isopotential maps.

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[in a new window]
Figure 6. A through D, Three-dimensional isopotential
contour maps constructed from computed electrograms at 194 left
ventricular nodes during apical pacing at sites 5 through
8, respectively, and plotted at 5, 10, 12, and 19 ms, respectively,
from the beginning of the stimulus. The pacing site is indicated by x.
Locations of the potential minimum and maximum are indicated by -
and +, respectively. Dashed line is a relative indication of
orientation between both extrema. All maps are plotted at the same
scale. Anterior left ventricle is displayed as viewed from the
epicardial side. E through H, Histological sections
from epicardium to endocardium obtained from myocardial blocks in the 4
pacing regions are shown below each map as viewed from the
epicardium.

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Figure 10. Isopotential maps constructed from computed
electrograms at 194 left ventricular nodes during a sinus
beat (indicated in Fig 8
). A, Map showing the earliest primary
potential minimum in the posterior paraseptal area. B, Map, plotted 4
ms after A, showing another primary potential minimum in the anterior
paraseptal area. C, Map, plotted 11 ms after A, showing almost complete
depolarization of the endocardium. The latest part to depolarize was
the posterobasal region. Both the anterior and posterior aspects of the
left ventricle (LV) are shown as viewed from the epicardial side.

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Figure 12. Endocardial electrograms computed using an
idealized probe-cavity geometric model (Fig 4
). The pacing site and
measured electrograms are the same as in Fig 5
; see Fig 5
for format of
presentation.
through 6H for
the 4 apical pacing regions. The alignment of the region of peak
positive potential (maximum) with respect to the primary potential
minimum in the isopotential maps in Fig 6A
through Fig 6C
agreed
qualitatively with the endocardial fiber direction in Fig 6E
through
Fig 6G
, respectively. The appearance of the primary potential minimum
in Fig 6D
at a later time and the alignment of the maximum and minimum
potentials compared with the direction of underlying endocardial fibers
in Fig 6H
suggest that pacing might have been applied at a deeper
myocardial site.
. The maps
correspond to the same four apical pacing protocols of Fig 6
(needles 5
through 8). The pacing needle site was always the region of earliest
activation. Earliest activation appeared at 6 ms in Fig 7A
, 13 ms in
Fig 7B
, 14 ms in Fig 7C
, and 22 ms in Fig 7D
. In all pacing protocols,
earliest activation appeared at an average of 16.5 ms from pacing
stimulus. The distance between the calculated site of earliest
activation and the needle site (ie, spatial error) was 9.8 mm in
Fig 7A
, 8
.2 mm in Fig 7B
, 0 mm in Fig 7C
, and 6
.6 mm in
Fig 7D
. Average error, for all pacing protocols, in determining the
site of origin of the pacing stimulus was 9.2 mm, as summarized in
Table 1
.

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[in a new window]
Figure 7. Three-dimensional isochrone maps constructed
from computed electrograms at 194 nodes. The maps correspond to the
same apical pacing protocols in Fig 6
. The pacing site is indicated by
x. The maps are plotted at the same scale.

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Figure 8. Simultaneous surface ECGs (leads I,
II, and III) in the open-chest dog during a spontaneous
ventricular premature depolarization (VPD). The sinus
rhythm beat (*) and the premature beat are analyzed in Fig 9
.
Corresponding isopotential maps are displayed in Figs 10
and 11
,
respectively.
For the first time, cavitary probe electrograms were recorded
simultaneously during ischemia-induced spontaneous
ventricular premature depolarizations (5 nonconsecutive
beats). Surface ECGs (leads I, II, and III) during sinus rhythm
interrupted by a ventricular premature depolarization are
shown in Fig 8
.
, electrograms computed during sinus rhythm resulted in an average
correlation coefficient of .86 and an average error in activation time
of 4.9 ms (Fig 9A
). Electrograms computed
during ventricular premature depolarization resulted in an
average correlation coefficient of .81 and an average error in
activation time of 4.5 ms (Fig 9B
). Earliest activation was clearly at
site 1 in Fig 9B
. Furthermore, electrogram fractionation and change in
morphology were observed at sites 1, 2, and 3, which is characteristic
of ischemia-related conduction.

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[in a new window]
Figure 9. Computed (thick tracings) and measured (thin
tracings) endocardial electrograms, plotted over 100 ms, during sinus
rhythm (A) and ventricular premature depolarization (VPD)
(B). Electrogram number corresponds to recording site (Fig 5
).
T indicates absolute difference between activation times determined
from computed and measured electrograms.
. A
primary potential minimum (potential <-5 mV) appeared initially in an
area on the posterior paraseptal wall in the lower half of the LV (Fig 10A
). Within 4 ms, another primary potential minimum (potential <-5
mV) appeared in the anterior apex extending toward the septum in the
anterior paraseptal area (Fig 10B
). Depolarization wave fronts spread
rapidly from these two areas, as they merged after 6 ms from the onset
of the initial primary minimum. Most of the LV endocardium was
depolarized within 11 ms, except for a posterobasal area, an
anterolateral area, and an anteroapical area (Fig 10C
). The last part
to depolarize on the endocardium was the posterobasal area, 20 ms from
the initial depolarization.
). The depolarization wave
front propagated downward along the septum and throughout the anterior
and posterior LV as shown in Fig 11B
after 25 ms. Most of the LV
endocardium was depolarized 40 ms after the initial depolarization and
completed after 55 ms. The alignment of the initial maximum and minimum
potentials was similar to the direction of fibers between epicardial
and midwall layers depicted in Fig 11C
.

View larger version (83K):
[in a new window]
Figure 11. Isopotential maps constructed from computed
electrograms at 194 left ventricular nodes during
spontaneous ventricular premature depolarization (indicated
in Fig 8
). A, Map showing the earliest primary potential minimum in the
high septal area, under the occlusion site of the left anterior
descending coronary artery (LAD). Locations of the potential
minimum and maximum are indicated by - and +, respectively.
Dashed line is a relative indication of orientation between both
extrema. B, Map, plotted 25 ms after A, showing progression of the
depolarization wave front. All aspects of the left ventricle (LV) are
shown as viewed from the epicardial side. C,
Histological sections obtained from a myocardial block
in the region of premature depolarization as viewed from the
epicardium.
Using the same cavitary electrograms, endocardial electrograms
were computed assuming an idealized probe-cavity geometric model (Fig 4
). Fig 12
shows
representative computed electrograms that correspond to
the same pacing protocol in Fig 5
(pacing at site 7). Computed
electrograms were degraded, and site 5 incorrectly reflected an earlier
activation time compared with the actual pacing site. Results of pacing
are summarized in Table 2
. Compared with
measured electrograms, computed endocardial electrograms resulted in an
overall correlation coefficient of .75 and an error in activation time
of 9.9 ms. Compared with the realistic geometry, the average error for
all pacing protocols in determining the site of origin of the pacing
stimulus was 17.0 mm.
View this table:
[in a new window]
Table 2. Computed Endocardial Electrograms With Idealized
Geometry
![]()
Discussion
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
New methods were developed and tested in the present study,
and new findings were achieved beyond that accomplished in previous
reports.12 13 14 In the present study, a
noncontact multielectrode probe was used to measure cavitary
electrograms from multiple directions in the blood-filled canine LV. A
three-dimensional model of the probe-cavity geometry was determined in
situ in the beating heart using two-dimensional epicardial
echocardiography. These cavitary electrogram and
geometry data were then used to mathematically compute the
corresponding electrograms on a high-resolution, three-dimensional
endocardial surface. Similar to previous studies, the methods were
tested during artificially paced control rhythms and further extended,
for the first time, to construct
electrophysiological images during sinus
rhythm and spontaneous ventricular premature
depolarization.
Our study has limitations. First, the probe used in the
present study was not yet suited for percutaneous
insertion. However, this prototype design provided us with new data
that permitted us to further test and advance our imaging methods.
Second, global validation of activation patterns with measurements
obtained from an extensive array of contact endocardial electrograms
was not performed. This was limited in the present study to
qualitative correlation with underlying fiber direction. Third, the
ability to resolve two simultaneous adjacent ectopic events
was not tested in the present study. Fourth, endocardial
electrograms were computed assuming a single probe-cavity geometry (ie,
end diastole), which was determined at the beginning of the
experiment, without accounting for possible variability throughout the
experiment. This was feasible as long as the electrical event (ie,
depolarization) preceded the mechanical event (ie, contraction). Fifth,
endocardial electrograms were computed using a fundamental numeric
regularization method, namely, Tikhonov zero-order, and the electrical
potentials at each time sample were treated independently (quasistatic)
using a single regularization parameter throughout the
entire image. However, the use of temporal and spatial numeric methods
has recently been demonstrated to be
advantageous.33 34 35
The study used a multielectrode cavitary probe that can be easily
miniaturized into a catheter-based probe, allowing for
percutaneous insertion into the blood cavity in a way
that is similar to electrode-catheters used in routine
electrophysiology studies. This noncontact mapping approach
reconstructs surface electrograms and activation sequences from
measured cavitary probe electrograms, providing high-resolution,
three-dimensional isopotential and isochrone maps. This mapping
technique is carried out over a single cardiac cycle. Therefore,
mapping can be conducted on a beat-by-beat basis, allowing for the
study of brief, rare, or even hemodynamically
compromising rhythm disorders that are difficult to evaluate with
existing techniques. Moreover, with the advent of catheter ablation,
the noncontact mapping approach can be preeminent in advancing ablation
for managing heart rhythm disorders by localizing arrhythmogenic sites
and directing ablation without the need for surgery.
![]()
Conclusions
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
We further extended our mathematical and experimental methods to
compute endocardial surface electrograms and activation sequences at
multiple simultaneous sites using electrograms measured
with a custom-made, cavitary, noncontact, multielectrode probe. While
measuring the probe-cavity geometric model in situ, we were able to
successfully construct high-resolution three-dimensional
electrophysiological images of the intact
canine LV endocardium during sinus, artificially paced, and spontaneous
premature beats. Further testing of the methods using a miniaturized,
catheter-based system is warranted.
![]()
Acknowledgments
This work was supported by grants-in-aid 94G-171 and 96R-171
from the American Heart Association, Texas Affiliate. Dr Khoury is a
recipient of the 1996 Lyndon Baines Johnson Research Award from the
American Heart Association, Texas Affiliate. The authors are indebted
to Dr Lloyd Michael and Peggy Jackson for their expertise and
assistance in conducting the experiments and to Dr Keith Youker and
Alida Evans for their generous efforts in performing the histology
studies.
![]()
References
Top
Abstract
Introduction
Methods
Results
Discussion
Conclusions
References
1.
The Cardiac Arrhythmia Suppression Trial
(CAST) Investigators. Effect of encainide and flecainide on mortality
in a randomized trial of arrhythmia suppression after
myocardial infarction. N Engl J Med. 1989;321:406412.[Abstract]
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