Vol. 274, Issue 3, H829-H845, March 1998
Optical mapping of atrioventricular node reveals a conduction
barrier between atrial and nodal cells
Bum-Rak
Choi and
Guy
Salama
Department of Cell Biology and Physiology, School of Medicine,
University of Pittsburgh, Pittsburgh, Pennsylvania 15261
 |
ABSTRACT |
The mechanisms responsible for atrioventricular
(AV) delay remain unclear, in part due to the inability to map
electrical activity by conventional microelectrode techniques. In this
study, voltage-sensitive dyes and imaging techniques were refined to detect action potentials (APs) from the small cells comprising the AV
node and to map activation from the "compact" node. Optical APs
(124) were recorded from 5 × 5 mm (~0.5-mm depth) AV zones of
perfused rabbit hearts stained with a voltage-sensitive dye. Signals
from the node exhibited a set of three spikes; the first and third
(peaks I and
III) were coincident with atrial (A)
and ventricular (V) electrograms, respectively. The second spike
(peak II) represented the firing of
midnodal (N) and/or lower nodal (NH) cell APs as indicated by
their small amplitude, propagation pattern, location determined from
superimposition of activation maps and histological sections of the
node region, dependence on depth of focus, and insensitivity to
tetrodotoxin (TTX). AV delays consisted of
1 (49.5 ± 6.59 ms, 300-ms
cycle length), the interval between peaks
I and II (perhaps AN
to N cells), and
2 (57.57 ± 5.15 ms), the interval between peaks
II and III (N to V
cells). The conductance time across the node was 10.33 ± 3.21 ms,
indicating an apparent conduction velocity
(
N) of 0.162 ± 0.02 m/s
(n = 9) that was insensitive to TTX.
In contrast,
1 correlated with
changes in AV node delays (measured with surface electrodes) caused by
changes in heart rate or perfusion with acetylcholine. The data provide
the first maps of activation across the AV node and demonstrate that
N is faster than previously presumed. These findings are inconsistent with theories of decremental conduction and prove the existence of a conduction barrier between the
atrium and the AV node that is an important determinant of AV node
delay.
rabbit atrioventricular node; compact node; atrioventricular nodal
delay; decremental conduction; atrioventricular node conduction; photodiode array; voltage-sensitive dyes; 4-[
-[2-(di-n-butylamino)-6-naphthyl]vinyl]pyridinium
 |
INTRODUCTION |
THE ATRIOVENTRICULAR (AV) node was first described by
Tawara (25) in 1906 as the only electrical connection between the atria
and the ventricles in mammalian hearts. The node is located between the
interatrial septum (IAS) and interventricular septum (IVS) in a region
called the triangle of Koch. It is composed of a spindle-shaped compact
network of small cells that was found to be essentially the same in
various species. The main function of the AV node is to delay
depolarization (e.g., activation) between the atria and the ventricles
and thereby coordinate their contraction. Histological analysis of the
AV node indicated that the node consists of five morphologically
distinct cell types: 1) transitional cells commingled with 2) atrial
cells; 3) midnodal cells, 4) lower nodal cells, and 5) cells of the
penetrating AV bundle embedded within the central fibrous body (17).
Transitional cells are distinguished from atrial cells by their smaller
size, pale staining reaction, and extensive connective tissue. Midnodal
cells are closely packed, have little intervening connective tissue,
and form the "compact" node. Lower nodal cells are elongated,
smaller than atrial cells, and form a bundle parallel to the AV ring.
The AV node of the rabbit heart (~1.5 mm in length) has been
extensively studied to characterize action potentials (APs) and activation delays in various regions of the AV node. AV nodal cells
were divided into three zones on the basis of their electrophysiology (18): atrionodal (AN), nodal (N), and nodal-His (NH) cells. The N zone
is an area of slow conduction and slow AP upstrokes, the AN zone is a
transitional region between fast-conducting atrial muscle and the N
zone, and the NH zone is a transitional zone between the N zone and the
His bundle. This classification was not strict and was further extended
on the basis of the AP response following a premature atrial
stimulation (3). AN cells were further subdivided into AN and ANCO
cells because, at fast pacing rates, APs of ANCO cells exhibited two
components, or a notch, on the AP upstroke. Premature stimulation and
pacing at faster rates also served to distinguish N from NH cells. To
correlate a particular AP response to the morphology of the cell, APs
were recorded with microelectrodes filled with potassium ferricyanide (24) or cobalt-containing KCl (1) to selectively stain cells that fired
a particular type of AP. Such studies suggested that AN potentials
emanate from transitional cells and NH potentials emanate from the
lower nodal cells. It should be noted that the diffusion of the stain
to neighboring cells made it difficult to demonstrate unequivocally
that N-cell APs originate from anatomically defined midnodal cells (1).
Activation delays across the AV node were measured with intracellular
microelectrodes (3, 4); however, a detailed spread of activation within
the midnodal and lower nodal zone could not be determined because
markedly different AP characteristics and activation times could be
measured at any location (but at unknown depths), with some cells
activating early and others late in the same region. As a result, it
was not possible to detect a wave of depolarization within the node and
thereby measure a conduction velocity in the AV node.
Hoffman and Cranefield (9) introduced the concept of decremental
conduction to explain propagation delays at the AV node. AV node cells
and, in particular, N cells have high intracellular resistance and
reduced intercellular coupling compared with atrial and ventricular
cells. The high coupling resistance could explain the basic conduction
delay of the AV node. Such decremental conduction would also predict a
gradual delay across the N zone so that delay is distributed across the
cell network. However, Billette (3) demonstrated that the conduction
delay is not decremental in space following a premature stimulus but
seems more localized in N cells, where conduction stagnates. Studies
from several investigators (1, 3, 4, 8) have led to the realization
that slow conduction in the AV node cannot be solely explained by
active properties of N cells, such as the maximum rate of rise of the AP upstroke
(dV/dtmax),
and that both passive and active properties are responsible for the
inhomogeneous potential spread in the N zone.
In the present report, we applied voltage-sensitive dyes and optical
imaging techniques to map electrical activity across the AV node in
attempts to elucidate the mechanisms responsible for the AV node delay.
Voltage-sensitive dyes have been extensively used by various
investigators (7, 20, 22, 23) to measure optical APs in a variety of
cardiac muscle preparations. Simultaneous recordings of transmembrane
potential by optical and microelectrode techniques have validated the
high fidelity of optical APs compared with microelectrode recordings
and demonstrated that optical APs detected the classic features of
atrial, pacemaker, and ventricular APs (14, 23). Optical
techniques also face important limitations because the absolute value
of membrane resting potential cannot be obtained unless calibrated with
a microelectrode, the downstroke of the AP can be distorted by movement
artifacts, and the optical AP represents the sum of APs from cells
within a region of tissue and not the AP of a single cell. Despite
these limitations, the technique offers important advantages in mapping
the inputs to the node, detecting the activation sequence in the
compact node, and identifying zone(s) of conduction delay.
 |
MATERIALS AND METHODS |
Experimental protocol.
This study describes data from nine experimental groups of rabbit AV
node preparations for a total of 44 hearts. In
group 1 (n = 3) hearts, the atrial-His bundle
(AH) interval and AV delays were measured before and after the hearts
were stained with the voltage-sensitive dye to examine possible
pharmacological effects of the dye. In group
2 (n = 4) hearts, APs
were simultaneously recorded with microelectrodes and optical mapping
techniques to help identify the origin of peak
II (see Isochronal maps and movies of
activation). In group
3 (n = 9) hearts,
activation across the IAS and the crista terminalis, conduction
velocity across the compact node, and AV delay were measured. In
group 4 (n = 4) hearts, AP signals were
analyzed as a function of depth of focus. In group 5 (n = 4) hearts,
optical recordings of APs were carried out, and then the tissue was
labeled with fiducial marks to superimpose activation maps on
histological sections of the tissue. In group 6 (n = 3) hearts, AV
node preparations were used to test the effects of tetrodotoxin (TTX).
In group 7 (n = 3) hearts, the effects of cutting
the His bundle were investigated, and in group
8 (n = 5) hearts, the
effects of exposure to acetylcholine (ACh) were tested. In
groups 1-8, the hearts were
allowed to beat at their intrinsic rates, which were controlled by the
sinoatrial (SA) node or primary pacemaker; a crush of the SA node
interrupted the normal heart rate and, after a few minutes, the AV node
became the primary pacemaker. In group
9 (n = 9) hearts, the
SA node was intentionally dissected and the heart was paced on the
right atrium (1-2 mm below the SA node) to measure changes in AV
delay and optical APs as a function of heart rate. Alternatively, the SA node was dissected to measure activation patterns with the AV node
as the primary pacemaker. This investigation conformed with the
Guide for the Care and Use of Laboratory
Animals published by the National Institutes of Health
[DHHS Publication No. (NIH) 85-23, Revised 1985, Office of
Science and Health Reports, Bethesda, MD 20892].
AV node preparation.
New Zealand White rabbits (2.0-3.0 kg) were anesthetized with
pentobarbital sodium (Nembutal; 35 mg/kg) by intravenous injection in
an ear vein. The chest was opened, and heparin (200 U) was injected in
the inferior vena cava. After a few minutes, the heart was removed and
perfused through the aorta in a modified Langendorff perfusion. The
perfusate contained (in mM) 130 NaCl, 12.5 NaHCO3, 1.2 MgSO4, 4.75 KCl, 1.0 CaCl2, and 20 dextrose. Solutions
were continuously gassed with 95%
O2-5%
CO2. The pH was adjusted to 7.4 with NaHCO3. Input of perfusate at
the aorta was controlled with a peristaltic pump (Minipuls 2, Gilson,
Middleton, WI) and was connected to a graduated manometer to obtain a
physiological mean aortic pressure of 80 mmHg. Aortic pressure was
monitored with a manometer and/or a pressure transducer (P10,
Statham, Waltham, MA). The flow rate of the pump determined the flow of
perfusate delivered to the coronary vessels and was adjusted to 7 ml · min
1 · g
wet wt
1 at the beginning of
each experiment and kept constant thereafter. A perfusion system with
"constant coronary flow rate" instead of the more typical
"constant aortic pressure" ensured that the flow of perfusate
through the myocardium remained constant and homogeneous during changes
of the contractile state and/or coronary resistance. The
perfusate was not recycled through the heart, and only preparations
with stable aortic pressures were selected for the study; initial
pressures were in the range of 80-100
cmH2O, and final pressures at the
end of the experiments changed by
5% of initial pressure. The free
walls of the right ventricle and atrium were dissected open to expose
the IAS and IVS and were pinned down on a Sylgard-coated horizontal
chamber. The chamber was water-jacketed to control temperature, which
was continuously monitored with a thermistor placed near the optical
field of view. A heating coil in the chamber was used to continuously
adjust the temperature of the bath via a feedback system. Surface
electrograms were recorded with bipolar electrodes (Teflon-coated
platinum wires, 250 µm and 1 mm apart) placed at key sites on the
preparation: 1) near the SA node,
2) on the IAS near the AV ring,
3) close to the His bundle,
and/or 4) on the IVS.
Staining procedure.
The heart was stained with the voltage-sensitive dye
4-[
-[2-(di-n-butylamino)-6-naphthyl]vinyl]pyridinium
(di-4-ANEPPS; Molecular Probes, Eugene, OR) by gradual injection of 200 µl of a stock solution of dye [2 mM in dimethyl sulfoxide
(DMSO)] into the bubble trap over a period of 5-10 min.
Other voltage-sensitive dyes, RH-421, di-8-ANEPPQ, and di-12-ANEPPQ
(Molecular Probes, Eugene, OR), were also tested in attempts to obtain
the highest possible signal-to-noise ratio for APs from the AV node.
All four dyes were tested by preparing stock solutions in DMSO or 1:1
mixtures of DMSO and Pluronic acid. Each stock solution of dye was
tested by either injecting the dye in the coronary perfusate or adding
dye to the bathing solution (1-2 mM) for 30-45 min. For all
four dyes, staining the hearts by injections in the coronary
circulation was markedly more effective than bathing the preparation in
dye solution such that greater amplitudes of optical AP upstrokes,
signal-to-noise ratios, and more homogeneous staining were obtained.
Di-4-ANEPPS gave the best signal-to-noise ratio and was used for the
experiments described in this study. In one experimental group
(n = 3), AH intervals were measured with bipolar surface electrograms before, during, and after perfusion of the hearts with dye solution to examine the possible pharmacological effects of DMSO with or without dye on AV conduction delays. Figure 1
shows the AH measurements from an AV node preparation. AH intervals averaged over a period of 5 min before hearts were stained were 42.7 ± 2.4 ms (Fig.
1A);
after hearts were stained, AH intervals were 43.3 ± 2.5 ms when
averaged over 5 min of dye washout (Fig. 1B; n = 3 hearts). Thus the present staining conditions with the use of a
DMSO stock solution of di-4-ANEPPS caused no detectable changes in AV
node conduction.

View larger version (19K):
[in this window]
[in a new window]
|
Fig. 1.
Bipolar surface electrodes were used to measure
atrial-His (AH) intervals before
(A), during, and after
(B) perfusion with
4-[ -[2-di-n-butylamino)-6-naphthyl]vinyl]pyridinium
(di-4-ANEPPS). One bipolar electrode was placed on the interatrial
septum (IAS) halfway between the sinoatrial (SA) and atrioventricular
(AV) nodes to detect atrial depolarization [atrial bipolar
electrogram (BE)]. A 2nd electrode was placed at junction of
tendon of Todaro (TT) and crista terminalis (CT) to detect His bundle
and ventricular depolarizations (His BE).
|
|
To avoid motion artifact to optical recordings, 10 mM diacetyl monoxime
(DAM) solution was used to block contraction during data acquisition.
Hearts were perfused in Tyrode solution containing DAM for 10-12
min and then perfused with standard Tyrode to avoid prolonged exposure
to DAM, which produced time-dependent changes in AP characteristics.
Exposure to DAM (10 mM) did not appear to alter AV conduction during
brief periods of DAM perfusion as used in these experiments, but
prolonged perfusion (>45 min) produced a gradual increase in coronary
resistance in total AV delays followed by inexcitable atrial and
ventricular tissue.
Optical apparatus.
Details of the optical and recording apparatus have been described
elsewhere (22). The horizontal chamber was mounted on an X-Y-Z
micromanipulator to accurately select the zone of tissue viewed by the
photodiode array and to control the location of the focal plane of the
optical apparatus as a function of depth in the tissue. Light from two
100-W tungsten-halogen lamps was collimated, passed through a 520 ± 20-nm interference filter, and focused on the triangle of Koch.
Fluorescence emission from the stained tissue was collected with a
camera lens (50 mm, f1:1.4, Nikon), projected through a 630-nm cut-off
filter (RG-645, Schott Glass), and focused to form an image of the
preparation on the surface of a 12 × 12 photodiode array
(Centronic, Newbury Park, CA). Five diodes from each corner of the
array were ignored such that optical signals were monitored from 124 of
144 diodes. The image of the AV node was focused on the array at a
magnification of ×0.36 such that each diode detected fluorescence
APs from a 0.46 × 0.46 mm area of epicardium. The depth of field
of the collecting lens restricted the fluorescence measurements to a
layer of cells ~100 µm from the surface. The depth of field of AP
recordings was estimated by varying the staining protocol and by
empirical calculations based on the magnification of the image, the
numerical aperture of the lens, and the wavelength of the emitted light (19). The image of the heart focused on the array was reflected by a
mirror onto a custom-made graticule with the exact dimensions of the
array (Graticules, Tonbridge, UK) located on a plane parafocal with the
plane of the array. Precise focusing and aligning of the heart with
respect to the array was accomplished by focusing and aligning the
image of the heart on the graticule. The photocurrents from 124 diodes
were fed to a current-to-voltage converter, amplified, digitized (1.56 kHz per channel, 12-bit resolution per sample), and stored in a memory
buffer of an IBM PC 486DX/4 100-MHz computer. The sampling rate (1.56 kHz per channel) was set to the maximum rate of the data acquisition
processor (DAP 1200e, Microstar Laboratories, Bellevue, WA). A data
acquisition scan consisted of 128 simultaneously recorded traces: 124 optical plus 4 instrumentation channels. A scan consisted of a
continuous recording of these 128 channels for 1.2-3 s.
Simultaneous AP recordings with microelectrodes and
voltage-sensitive dyes.
In some experiments, conventional 3 M KCl-filled microelectrodes with a
resistance of 20-40 M
were used to record APs from the AV node
to identify the APs that fired in synchrony with the second spike of
the optical recordings. Optical APs were recorded from the
AV node zone, and then the diodes on the array that detected three
spikes were used to identify the mid- and lower nodal zone, which was
then impaled with a microelectrode to simultaneously record APs by the
two techniques. These measurements were challenging because the short
working distance between the lens and the preparation made it difficult
to obtain stable microelectrode impalements at a shallow angle of
penetration.
Data analysis.
Several criteria were used to assess the "health" of AV node
preparations: 1) the rapid rise time
of atrial and ventricular AP upstrokes,
2) the short AH intervals
[<80 ms at 500 ms cycle length (28)],
3) the rapid propagation of APs in
the atrium (<0.1 m/s), and 4) the
duration of ventricular APs, because short AP durations are indicative
of ischemic injury. The activation time point at each diode was taken
as the time point of the maximum rate of rise of the
fluorescence (F) AP upstroke
(dF/dtmax),
which represents the time when most of the cells depolarized (21, 22).
Optical recordings from each channel were normalized and passed through
a Butterworth filter, and the first derivative of each fluorescence
signal (dF/dt) was calculated by a
numerical differentiation method using a three-point Lagrangian
interpolation. The
dF/dtmax time
point was accepted as an activation time if dF/dtmax was
greater than the standard deviation (SD) of background noise. The
analysis of optical APs was automated using in-house software written
with IDL 3.6.1b (Interactive Data Language, Research Systems, Boulder,
CO) and Borland C++ 4.0.
Isochronal maps and movies of activation.
Optical signals from atrial and ventricular muscles exhibited the
expected shapes and characteristics of atrial and ventricular APs. In
contrast, signals from the AV node region (the region delineated by the
tendon of Todaro and the crista terminalis) exhibited a set of three
sequential spikes indicative of three distinct depolarization events
separated by marked time delays (see Figs. 2-4). The first and
third spikes (peaks I and
III) were coincident with atrial and
ventricular depolarizations, respectively. The second spike
(peak II) was only detected in the
AV node region and was the smallest in amplitude. Thus three cell types
were found to overlap in the same zone of AV node tissue, and
activation patterns were independently generated for the three spikes.
The combined activation patterns represented atrial, nodal, and
ventricular activation that corresponded anatomically to the atrial,
nodal, and ventricular regions of the preparation. Isochronal maps were generated for the three wave fronts using a linear triangulation method
(Tecplot-3DV, Amtec Engineering, Bellevue, WA). To map activation in
the AV node zone, the region that exhibited peak II was extracted first and was typically delineated by
12-18 photodiodes, or areas of 4 × 3 or 6 × 3 diodes,
on the array. Activation time points for all peak
II were triangulated, isochronal lines were calculated
for every 1-ms interval using the values of the three edges of the
triangles by linear interpolation, and then points were connected by
lines. With linear triangulation, 10-12 isochronal lines were
typically generated in a zone delineating 2-3 mm of nodal tissue.
Conduction velocity was determined from the time delays between
isochronal lines and the distance traveled by the wave front detected
in the two-dimensional (2-D) field of view of the array. These
measurements represent "apparent" conduction velocities given
that the precise pathways of the wave fronts are approximate, because
the node is a three-dimensional (3-D) structure (0.75-1.25 mm
thick according to histological analysis) and the pathway is determined
from 2-D maps. As a result, conduction velocities may be underestimated
if the pathway propagation spreads in depth across the thickness of the
node as well as in the 2-D field of view.
The spread of depolarization was animated to visualize the spread of
excitation waves. The animation program was written with g++ 2.7.2 and
YORICK 1.2 by scaling the amplitudes of the optical recordings into a
range of 8-bit, 256-color levels. The signal-to-noise ratio was
sufficiently high so that filtering of the normalized signals was not
necessary. One frame of the byte-scaled data from the 12 × 12 array was converted to a 120 × 120 pixel image that consisted of
12 × 12 squares (the level of depolarization was color coded and
filled an array of 10 × 10 pixels). The sequence of excitation
images was displayed on the monitor using X Windows System (X
Consortium) "pixmaps." The typical animation runs at 20 frames/s.
Mapping and animation were performed on a Pentium (100 MHz) running
Linux (kernel version 2.0) or an Indy workstation (Silicon Graphics,
Mountain View, CA) running Irix 5.3. Movies of AP propagation across
the AV node can be seen at our web site (Salama, Guy. Lab and current
research: AV node conduction. [On-line] Dept. of Cell
Biology and Physiology, Univ. of Pittsburgh.
http://www.cbp.pitt.edu/
gs.htm);
QuickTime movie player is required.
The activation time point for each fluorescence AP was
taken at
dF/dtmax, when
most of the cells viewed by a diode are depolarizing. Activation time
points for all 124 APs were labeled with "tick marks" that could
be verified and corrected by the operator using an interactive program.
The detection of activation time points using
dF/dtmax was
highly reliable and rarely required correction by the investigator
(<1% of activation events). The upstrokes of optical APs from the AV
node were distorted by movement artifacts from vigorously contracting
hearts because atrial contractions interfered with the small signals
from the AV node zone such that the use of DAM (as described in
Staining procedure) was essential to
abate movement artifacts.
Histology.
Optical electrophysiological recordings were made to identify the zone
of tissue that fired three sequential spikes, and then the tissue was
marked with fiducial points at sites that corresponded to the edges of
the array. The fiducial marks were made by impaling the tissue with a
microelectrode and then placing a silk surgical thread suture at those
sites to ensure that the fiducial mark was clearly identifiable even
after the histological processing. The tissue containing the AV node
region was excised and fixed in Bouin's solution overnight. The fixed
tissue was embedded in paraffin, and serial sections 5 µm thick were
taken starting from the endocardial surface, and every tenth section
was mounted on a glass slide. Mounted sections were progressively
stained with Mayer's hematoxylin, counterstained with eosin, and
placed under a glass coverslip (15). Stained sections were examined
under a microscope and captured in TIFF images (in 24-bit true color) using a charge-coupled device camera. Shrinkage caused by fixation (~35%) was automatically taken into account by aligning the fiducial marks on the sections with their respective locations on the edges of
the array. The isochronal maps derived from optical APs were superimposed on images of the tissue derived from histological sections
using CorelDraw 7.0.
 |
RESULTS |
Optical recordings from AV node.
Figure 2A
shows an anatomic sketch of the AV node region delineated by the tendon
of Todaro and the crista terminalis forming the triangle of Koch and
the central fibrous body. A symbolic map of the array is
superimposed on the AV node to identify the region of tissue mapped by
the array. The orientation of the array relative to the AV node was
arbitrary but was kept constant in the present study. Figure
2B shows a set of 124 optical signals recorded from the AV node region as well as simultaneously recorded atrial and ventricular bipolar electrogram (BE) recordings. Figure 3,
A-D, shows the four types of
signals recorded from the AV node region and the temporal relationship
between these signals and the surface electrograms. Each panel of Fig.
3 represents a more detailed tracing of recordings from
diodes a-d in Fig.
2A. Each panel contains three traces,
the atrial and ventricular BEs plus an optical recording from one of
the diodes (a-d) viewing
different sites on the preparation. Diode
a (see Fig. 2A)
viewed the IAS and detected atrial APs with negligible contribution
from other cell types such as nodal or ventricular cells (Fig.
3A). Diode b (see Fig. 2A)
viewed the IVS and detected ventricular APs (Fig. 3B). At border zones between the IAS
and IVS, diode c (see Fig. 2A) detected voltage-dependent
optical responses with two upstrokes per cardiac beat (Fig.
3C). In these zones, the IAS
overlapped ventricular tissue such that both cell types contributed to
the signal recorded by the same diode, resulting in the sequential firing of atrial, and then ventricular, APs. The interpretation of the
cell types responsible for these optical signals was validated by the
electrogram recordings in that the upstrokes of atrial and ventricular
optical APs were coincident with the atrial and ventricular
electrograms, respectively (Fig. 3,
A-C). In addition, atrial and
ventricular APs were recorded optically at sites consistent with the
anatomy of the preparation: they had the expected shape and time course
of atrial and ventricular APs, and the delay between the firing of the
two upstrokes was consistent with the expected AV delay. More
interesting was a unique feature of optical signals from the AV node
region shown in Fig. 3D. Signals
recorded from a narrow zone between the tendon of Todaro and the crista
terminalis (diode d; see Fig.
2A) exhibited a set of three
sequential depolarizations per cardiac beat, peaks
I, II, and
III (Fig.
3D). By superimposing signals
detected by other diodes and surface electrodes, peak I was again coincident with atrial depolarization and
peak III was coincident with
ventricular depolarization. Peak II
consistently fired at intermediate time points and was only observed in
a narrow (1 × 2 mm) region of the preparation.

View larger version (53K):
[in this window]
[in a new window]
|
Fig. 2.
A: sketch of AV node
preparation superimposed on a symbolic map of photodiode array to
delineate AV node region being viewed. Anatomic landmarks of AV node
region are identified to correlate optical signals obtained from each
site with origins of signals. Compact node, or midnodal region, is
delineated by a speckled outline and is bounded by TT and CT,
surrounded by IAS above and inter- ventricular septum (IVS) below, and
adjacent to central fibrous body (CFB). Orientation of array relative
to AV node zone was arbitrary but was kept the same for all experiments
shown. B: simultaneously recorded
optical action potentials (APs) from 124 sites on AV node zone. A
symbolic map of array is shown as 124 square boxes, each identifying
the location of individual diodes. The region of tissue viewed by each
diode corresponds to map in A. The
optical trace recorded by each diode is shown in its respective
location in a compressed time base (400 ms).
Inset: BE recordings, 1 located on IAS
2 mm above TT (A; outside field of
view of array; atrial BE) and 1 on IVS near apex of ventricle
(ventricular BE), were simultaneously recorded along with 124 optical
signals. Optical APs recorded by diodes at locations
a-d
(A) are shown in Fig. 3.
|
|

View larger version (21K):
[in this window]
[in a new window]
|
Fig. 3.
Classification of optical signals from AV node region. Optical APs from
AV node region shown in Fig. 2B
exhibited 1 of 4 possible characteristics depending on location of
recording. Each class of optical AP was temporally correlated with
atrial and ventricular BEs to show firing sequence of APs.
A-D each show a set of 3 traces,
the atrial (top) and ventricular
(bottom) BEs plus an optical
recording (middle), from diodes
labeled a-d, respectively, in
Fig. 2A.
A: optical AP recorded from atrial
cells located on IAS by diode a.
B: ventricular AP recorded from IVS by
diode b.
C: optical APs from AV boundary were
recorded by diode c. At such sites,
atrial and ventricular cells overlapped, resulting in optical signals
with 2 spikes, synchronous with atrial and ventricular BEs,
respectively. D: optical recordings
from AV node at diode d invariably
consisted of 3 sequential depolarizations (peaks
I-III). Peaks I
and III were coincident with atrial
and ventricular BEs, and peak II fired
at an intermediate time point, indicating that AV node was origin of
signals that exhibited 3 sequential spikes. F/F, fractional
fluorescence change.
|
|
AP propagation within AV node.
To elucidate the origins of peak II,
intracellular microelectrodes and optical APs were simultaneously
recorded from the zone that exhibited the sequence of three
depolarizations. As shown in Fig.
4A, the
firing of peak II was coincident with
APs with the characteristic shape of N and/or NH cells because
of the slow diastolic depolarization and slow upstroke
(n = 4 hearts). In contrast,
microelectrode recordings of atrial, AN, His, and ventricular APs were
not coincident with peak II
depolarization (not shown). More detailed analysis of the
spatiotemporal characteristics of peak
II was carried out to reinforce the interpretation that
peak II originated from the midnode
and/or lower node region and to map electrical conduction
across the AV node. Figure 4B shows the approach used to calculate the time delays
1 and
2 from the time points of
dF/dtmax for
peaks I-III.

View larger version (17K):
[in this window]
[in a new window]
|
Fig. 4.
Detection of activation time points in AV node.
A: simultaneous optical and
microelectrode recordings from AV node. Optical signals detected a
sequence of 3 depolarizations, and peak
II was coincident with an AP recorded from a
microelectrode impaled in a midnodal or distal node cell, either an N
or NH cell. The shape and time course of the microelectrode AP show
that peak II fired in synchrony with
an N and/or an NH cell. B: 1st
derivatives of all 4 classes of signals
(dF/dt) were taken to analyze spread
of activation across AV node and to determine time point of activation
at each site. For signals from AV node,
dF/dt identified 3 separate activation
time points. Top: F/F recorded from
a diode viewing AV node exhibited a set of 3 upstrokes (arrows)
per cardiac beat (peaks
I-III). Bottom:
delays between peaks I and
II
( 1) and between
peaks II and
III
( 2) were determined from time
points of maximum dF/dt
(dF/dtmax) of
voltage-sensitive fluorescent signals.
dF/dt of peak
II allowed identification of activation time points for
cells comprising AV node that were used to map activation patterns
across node.
|
|
Maps of electrical activation generated from activation time points (as
in Fig. 4A) were highly reproducible
from beat to beat of the same heart and from heart to heart. Figure
5 shows an experiment from a spontaneously
beating heart with a cycle length of 417.92 ± 0.96 ms (mean ± SD). The mean AV delay (±SD) measured with surface electrograms was
88.75 ± 0.37 (n = 5 beats). As
shown in Fig. 5, the time points of
dF/dtmax for
peaks I-III were detected
separately and used to map the spread of activation in the IAS (Fig.
5A), the AV node (e.g., the zone of
tissue detecting peak II) (Fig.
5B), and the IVS (Fig.
5C). Figure
5D depicts the superimposition of all
three activation patterns, showing that the three maps overlap in a
small region identified as the compact node. Activation across the IAS
occurred in 15 ms (Fig. 5A), and, after a substantial delay, the AV node signal appeared at 43 ms (Fig.
5B) and spread across the node in 8 ms. After another delay (e.g., the time to propagate from the His
bundle to the apex and back to the base of the ventricle), the IVS
fired APs at 93 ms and spread in the field of view in 4 ms (Fig.
5C). Such maps of conduction across
the AV node were highly reproducible in both their patterns and
temporal relationships. Table 1 lists the composite analysis of nine rabbit preparations. The means ± SD for
1 and
2 were calculated for rabbit AV
nodes (n = 9) under sinus rhythm, with
an intrinsic cycle length of 301.64 ± 8.41 ms. The time for
peak II to propagate across the
compact node (i.e., midnode) was 10.33 ± 3.21 ms, which predicts a
conduction velocity of 0.162 ± 0.024 m/s. The conduction velocity
measured by optical techniques is faster than that inferred from
intracellular microelectrode recordings because the latter measurements
were not based on multiple recordings within the node and included a
substantial component of
1 or
AN delays.

View larger version (34K):
[in this window]
[in a new window]
|
Fig. 5.
Isochronal maps of activation across AV node. From activation time
points obtained as described in Fig. 4, activation sequences of atrial
(peak I), nodal
(peak II), and ventricular
(peak III) regions were triangulated
individually and isochronal lines of activation were drawn 1 ms apart.
Gray scale from bright to dark represents "early" to "late"
activation times. Axes are length in millimeters.
A: depolarization sequence of IAS
generated from peak I.
B: activation sequence of the AV node
generated from peak II.
C: activation sequence of IVS
generated from peak III.
D: composite isochronal map of AV node
region generated from superimposition of activation maps in
A-C reveals details about
supraventricular activation and spread of activation across AV node and
IVS. Note that from last depolarization of peak
I to first depolarization detected through
peak II, there is a 30- to 33-ms
interval during which firing of APs is not detected anywhere in the
preparation.
|
|
In Fig. 6, an activation pattern across the
AV node is shown as a sequence of activation maps captured at different
time points during a single cardiac beat. Each map is a pseudocolor map
of the array for which the extent of depolarization at each site is
color coded from violet to red (from least to most depolarized potential). The first map (at time t = 0.0 ms) is violet or blue (i.e., the tissue is at resting potential).
The next map, at 3.2 ms, shows the initial firing of the atrium that
spreads along the IAS in the subsequent maps (from 3.2 to 25.6 ms).
After a partial repolarization of the IAS (from 25.6 to 41.6 ms), the firing of nodal APs begins in the lower left zone of the array (44.8 ms) and spreads along a narrow zone (1-2 diodes wide), at first
slowly and then faster, into the His bundle (from 44.8 to 54.4). After
a delay (from 60.8 to 80.0 ms), the IVS depolarizes and ventricular
signals overlap the AV node zone (from 80.0 to 86.4 ms). Video
animation of these maps is more effective for visualization of the
propagation pathway and can be accessed from our web page (see
Isochronal maps and movies of activation).

View larger version (75K):
[in this window]
[in a new window]
|
Fig. 6.
Pseudocolor maps of activation across AV node region. A sequence of
array images recorded at different time points during a single cardiac
beat was generated as an alternative approach to display activation
maps. Levels of local depolarization were linearly converted to rainbow
color map (color scale 0-255), where least to most depolarized
levels produced a color shift from blue to red, respectively.
Successive images taken every 3.2 ms were generated from optical
recordings as described in MATERIALS AND
METHODS. Inset:
orientation of images.
|
|
Depth resolution and amplitude of AV node APs.
The AV node is a 3-D structure located near the surface of the IAS,
with the majority of cells comprising the compact node found
~0.06-0.5 mm below the surface of the IAS (6). Microelectrode studies have identified zones of AN that overlap zones of N and NH
cells on the basis of their AP characteristics (6). The 3-D nature of
this structure implies that the focal plane of the imaging system
should be located below the surface of the preparation to obtain
maximum signal amplitudes for AV nodal APs. As shown in Fig.
7, a given diode will detect light from
different volumetric zones of tissue as the focal plane of the optical
apparatus is shifted below the surface. This is a natural consequence
of optical detection because light from cells located on the plane of
focus is transferred to the diode with the highest efficiency, whereas light from cells above and below the focal plane is transferred to the
diode with decreasing efficiency. The efficiency of light transfer as a
function of depth (at any given wavelength of light) depends on the
"energy transfer function" of the collecting lens, measured at a
particular optical magnification (21). The AV node was optically
sectioned by recording APs from the surface and then from deeper
optical sections by shifting the plane of focus into the tissue in
250-µm steps. Changes in the relative amplitude from
peak I to peak
II were used to estimate the depths of the cells
responsible for the generation of peak
II.

View larger version (37K):
[in this window]
[in a new window]
|
Fig. 7.
Ratio of peak II to
peak I as a function of depth.
Schematic of a transverse histological section of rabbit AV node
indicates different layers of cell types found as a function of depth
in tissue [adapted from Janse et al. (10a)]. Volumetric
elements (shaded cubes) superimposed on section represent volume of
cells that are primary sources of fluorescence signals (F) detected by
a diode when focal plane is shifted below surface in a stepwise manner.
At different focal planes, different layers of cells become primary
sources of signal. h , Excitation
light.
|
|
As shown in Table 2, the relative amplitude
from peak II to peak
I increased with increasing depth of the focal plane
for 0, 0.25, and 0.5 mm and then decreased for 0.75 and 1.0 mm. The most likely explanation for these depth-dependent changes is that peak I emanated from the surface and
peak II emanated from cells ~0.5 mm
below the surface. In all experiments, the focal plane was first
adjusted to maximize peak II relative
to peak I at the beginning of each
experiment. This approach made it possible to maximize the
signal-to-noise ratio for peak II,
delineate the 2-D distribution of the cells that fire
peak II, and map the spread of
activation of peak II.
Activation sequence of pacing AV node.
A key feature of the AV node is that, in the absence of SA node
activity, N or NH cells can become primary pacemakers. To investigate
the spread of activation in hearts, we removed the SA node so that the
AV node became the primary pacemaker
(n = 4). Figure
8A shows
the optical signals detected from the AV node zone when pacemaker
activity was initiated at the AV node. In this case, the initiation of
the heart beat begins in the node [AV node (midnodal)] at a
time delineated by the time line labeled a (Fig.
8A). As a primary pacemaker, the AV
node trace (or peak II) fired first,
and the atrial and ventricular BE are delayed (~28 ms) and are
coincident with the time line labeled
c (Fig. 8A). Note that, as expected, the
optical recording of ventricular AP was coincident with the ventricular
BE. On the other hand, the recovery of atrial AP was coincident with
the time line labeled b (Fig.
8A) and precedes the atrial BE
because the optical signal recorded APs near the AV node at an early
time of activation, whereas the BE was located on the IAS, near the SA
node. When the AV node is the dominant pacemaker, the amplitude and
slope of the first depolarization was markedly decreased as expected because peak II is now the leading
wave of depolarization originating from the AV node. In Fig.
8B, activation maps indicate that
impulses were initiated in a narrow zone within the triangle of Koch,
and the first site to activate fired in the node as indicated by the asterisk. The signal spread in 10 ms within the node, and after a
substantial delay (27.96 ms; see arrow in Fig.
8B), activation spread across the
IAS. The zone of activation delineated by peak II during sinus rhythm (not shown) was the same as that
delineated by the leading wave of AP upstrokes when the AV node became
the pacemaker (Fig. 8B). The marked
conduction delay from the AV node zone to the IAS (Fig.
8B) indicates that propagation is
not smooth but is discontinuous in both the anterograde and retrograde
directions. This barrier to conduction (arrow) between the compact node
and the IAS is dramatically evident in all the activation maps (Fig. 8B). The activation pattern within
the ventricular tissue was intentionally omitted from the activation
maps of Fig. 8B so that AV nodal
activation would not be obscured.

View larger version (25K):
[in this window]
[in a new window]
|
Fig. 8.
Optical recordings from a pacing AV node. SA node was removed so that
AV node became primary pacemaker. A:
atrial and ventricular BEs were used to monitor firing of IAS and IVS
and were temporally correlated with optical APs recorded from various
regions of AV zone preparation: IAS (atrial AP),
posterior boundary of AV node (transitional cells), AV node (midnodal
cells), and IVS (ventricular AP). Earliest activation occurred at AV
node (time line a) and propagated to
atrium (time line b), His bundle,
and ventricle (time line c).
B: activation maps of AV node and IAS
generated from atrial and nodal APs (axes are length in millimeters).
Activation sequence in IVS was intentionally omitted to allow
visualization of conduction through node and delay between nodal and
IAS activation. Impulses initiated in node (*) and propagated across
node in 10 ms and to IAS after a 17.96-ms delay. Step delay in
excitation wave occurred across a conduction barrier delineated by
closely packed isochronal lines (arrow). Isochronal lines were 2 ms apart. For web site access to QuickTime movie of propagation
sequence, see MATERIALS AND METHODS.
|
|
Superimposition of activation maps and histological sections of AV
node.
In four hearts, optical maps of APs were recorded from the AV node
region and the tissue was labeled with fiducial marks, fixed, embedded
in paraffin, serially sectioned, and mounted on microscope slides for
histological analysis. Figure
9A shows
the anatomic landmarks of the AV node seen from longitudinal cross sections taken from the endothelial surface at increasing depths in the
tissue. The conventional anatomic landmarks of the AV node are all
resolved at a depth of 100 µm (Fig.
9A,
left), namely, the IAS, the pale
cells of the compact node, the IVS, and the His bundle. As shown in
Fig. 9, A and
C, zones of fat cells are found
adjacent to the AV node region. These zones of adipose cells are
typical of mammalian AV nodes and extend continuously at all depths of
the preparation. In this heart, the dimensions of the AV node zone were
largest at a depth of 150 µm (Fig.
9A,
middle) and decreased at a depth of
200 µm (1-mm scale at right applies to A-C). Activation maps
recorded from the same preparation are shown in Fig.
9B as a set of maps taken every 3.2 ms. In this case, the SA node was removed and the AV node became the
primary pacemaker. The superimposition of isochronal maps derived from optical recordings and the histological section taken at a 150-µm depth showed that the compact node is the tissue underlying the optical
map-identified activation patterns across the AV node. Moreover, the
earliest sites to fire APs in these maps were located in the proximal
region of the compact node (i.e., posterior), and subsequent APs fired
in the distal zone of the AV node (i.e., anterior), followed by the His
region, with increasingly faster propagation velocity. The
superimposition of optical isochrones and histological images (Fig.
9C) provides compelling evidence that these optical signals originate from the firing of APs in the AV
node and delineate the shape and boundaries of the AV node. Figure
10 shows another example of activation
isochrones across the AV node toward the His bundle and depicts the
marked increase in conduction velocity from the proximal to the distal
portion of the node. The traces (Fig.
10A) show the kinetics of optical signals recorded from these two regions. The top trace (Fig.
10A), recorded from the proximal
region of the AV node trace, exhibited the typical sequence of three
depolarizations. Here, peak II
originated from the midnodal region, which initiated waves of
depolarization (Fig. 10A, top arrow).
The bottom trace, recorded from a more distal region, exhibited a
sequence of two depolarizations, a His followed by a ventricular
depolarization.

View larger version (110K):
[in this window]
[in a new window]
|
Fig. 9.
Superimposition of activation maps and histological landmarks of AV
node. A: charge-coupled device images
of 3 longitudinal sections of same AV node taken at different depths.
Anatomic landmarks are IAS, IVS, CT, fat deposits (F), midnodal region
(N), and His bundle. B: activation
maps recorded from same AV node showing sequence of depolarization at
3.2-ms intervals, as in Fig. 6. Within a single cardiac beat,
progression from earliest (top left)
to latest (bottom right) activation
map shows sequence of depolarization.
C: superimposition of activation map
derived from peak II depolarization on
a longitudinal cross section of same AV node preparation. Optical and
histological maps were aligned as described in
MATERIALS AND METHODS and indicate
that a barrier to electrical propagation forms a collar at posterior
edge of AV node (may include zones of adipose tissue) and that a bridge
with a high electrical resistance appears to separate IAS from midnodal
region.
|
|

View larger version (31K):
[in this window]
[in a new window]
|
Fig. 10.
Effect of TTX (10 µM) on activation across AV node and His bundle.
Excitation maps across AV node were generated from activation time
points of peak II, as in Fig. 3, and
isochronal lines were drawn 1 ms apart.
A: in some preparations, activation
maps generated from intermediate (peak
II) depolarization revealed a pattern of
depolarization across midnodal, lower nodal, and His bundle regions
(left). Optical signals
(right) measured from midnodal
region (AV node) exhibited typical response characteristics of
peak II. Signals from lower node
region (not shown) were similar to midnodal signals. Signals from His
bundle were typically recorded from zones exhibiting 2 sequential
depolarizations: upstrokes generated by His firing followed by firing
of ventricular cells. Time lines labeled A, N, and H represent the
depolarization time of the IAS, node, and His bundle, respectively.
B: to confirm interpretation of these
signals, TTX was used to identify nature of cells producing optical
signals. Activation maps were drawn in absence of TTX
(left) and then recorded after 20 min of perfusion with 10 µM TTX. Note that conduction across
posterior segment of node was TTX insensitive, whereas conduction
through anterior segment slowed markedly, supporting interpretation
that these responses originated from His bundle.
|
|
Effect of TTX on AV node signals and conduction.
The major depolarizing current of N and NH cells is a slow inward
current (most likely Ca2+ current)
that is insensitive to the voltage-gated
Na+-channel blocker TTX (12). In
contrast, atrial, AN, His, and ventricular cells are somewhat sensitive
to TTX, which, at 5-10 µM, decreases
dV/dtmax.
We investigated the effect of TTX (10 µM) on the propagation times
across the AV node, that is, of peak II and His bundle depolarization, in the same manner as
in Fig. 10A
(n = 3). Figure
10B shows an example of activation
maps measured from the node before
(left) and after
(right) 20 min of TTX perfusion. TTX
reduced the rise time of atrial and ventricular APs (not shown) but did
not alter the spatiotemporal characteristics of peak
II (compare the proximal zone of the AV node in Fig.
10, A and
B). On the other hand, TTX produced
a marked decrease in apparent conduction velocity in the distal zone of
the activation map (Fig. 10B,
right, TTX-sensitive zone). The
sensitivity of the distal zone to TTX supports its identification as a
His bundle region from the histological analysis (Fig. 9) and the
spatiotemporal distribution of the signals (Fig.
10A). Thus the posterior zone consists of TTX-insensitive cells (most likely N and/or NH
cells), and the anterior zone contains TTX-sensitive cells (most likely His and perhaps NH cells), in line with intracellular microelectrode recordings.
Effect of His bundle cut.
Figure
11A
shows the atrial and ventricular BEs and optical recordings from the
IAS, the AV node, and the IVS following a cut of the His bundle. The
His bundle forms the only electrical connection between the AV node and
the ventricle such that cutting fibers below the AV node effectively
disconnected electrical coupling between the ventricular myocardium and
inputs from the AV node. As shown in Fig.
11A, severing the His bundle
eliminated the synchronous firing of ventricular BE and the detection
of ventricular APs. This finding reinforced our interpretation that APs
from the lower left zone of the preparation originate from ventricular
cells. Under our experimental conditions, the His bundle cut produced a
2:1 block between atrial and nodal activation (Fig.
11A, node). As a result, some atrial
activation waves (Fig. 11A, I)
failed to entrain an AV node activation (Fig.
11B; note the lack of AV node
activation), whereas the next beat (Fig.
11A, II) was coupled to an AV node
activation (Fig. 11C). Not all
activity ceased in the ventricular tissue because ectopic beats were
occasionally observed, but these were out of phase with atrial and
nodal APs. An advantage of His bundle cuts is the absence of
ventricular APs, which interfered with our ability to detect the
repolarization phase of N-cell APs.

View larger version (44K):
[in this window]
[in a new window]
|
Fig. 11.
Effect of cutting His bundle on electrical activity was investigated in
4 rabbit AV node preparations. A:
simultaneous recordings of atrial and ventricular BEs and optical APs
from IAS (atrium), AV node, and IVS (ventricle) are shown after His
bundle was cut. As expected, His bundle cut blocked excitation to IVS,
abolishing ventricular BEs and APs. In absence of coupled ventricular
depolarization, AV node signals fired 2 sequential spikes, an atrial
and a nodal spike; the latter was not followed by a ventricular AP,
revealing plateau and repolarization phases of AV node AP. Atrial APs
were synchronous with atrial BE, but nodal APs were markedly reduced at
every other beat, suggesting a 2:1 block of AV conduction. Activation
maps of 2 successive beats (beats I
and II on nodal AP) are shown,
respectively, in B and
C. Activation map produced by
beat I produced an IAS excitation
pattern (B), whereas
beat II mapped IAS and nodal
activation. Note that IAS activation patterns were similar for
beats I and
II. Isochronal lines were 1 ms apart;
axes are length in millimeters.
|
|
A conduction barrier between atrial and nodal cells regulates AV
delay.
AV delay is physiologically regulated by heart rate, parasympathetic,
and sympathetic activity. To investigate the mechanisms responsible for
the physiological regulation of the AV node delay, activation maps
across the node were analyzed as a function of cycle length. The heart
rate was controlled by removing the SA node and pacing the right atrium
with bipolar electrodes placed near the SA node. In this experimental
group (n = 9), cycle length was varied
from 270 to 350 ms; shorter cycle lengths made it difficult to
temporally separate the overlapping peaks
I-III for analysis, and longer cycle lengths were
possible except that extra beats occasionally interfered with the
measurements. In this range of cycle lengths, activation maps across
the IAS, AV node, and IVS maintained the same pattern. AV delay
measured with atrial and ventricular electrograms changed with cycle
length, as shown in Fig. 12, and was
highly correlated with changes in
1, with a correlation coefficient of 0.98, but correlated poorly with changes in
2, with a correlation
coefficient of 0.42 (each data
point corresponds to the mean ± SD).

View larger version (18K):
[in this window]
[in a new window]
|
Fig. 12.
Correlation of 1 and AV delay
at various cycle lengths. A heart was paced from 270 to 350 ms with
bipolar electrodes placed near SA node;
1 and
2 were measured as described in
Fig. 4. Total AV delay (measured with surface electrograms),
1, and
2 were plotted as a function of
cycle length. Each set of data points was fitted with a line drawn
using polynomial curve fit. Step delay in conduction between A
(and/or AN) and N cells
( 1) changed with rate,
whereas 2 was within
experimental error and rate independent. Correlation coefficient
between AV and 1 delay as a
function of cycle length was 0.98, and that between AV and
2 was 0.39.
|
|
Heart rate and AV delay are regulated physiologically by sympathetic
and parasympathetic innervation to the heart. Although much is known
regarding the mode of action of neurotransmitter at the SA node, the
mechanisms responsible for AV node regulation are less well understood.
In a separate experimental group (n = 5), we altered AV delay by perfusing the heart with ACh (0.1 µM). In
all five experiments, the major change in the optical map was an
experimentally significant increase in
1 by 19 ± 2.3 ms and a
slight increase in the time to activate the node [e.g., a
decrease in apparent conduction velocity in the node region (
N)]. Figure
13, A
and B, depicts the maps of activation
of the IAS before and after perfusion with ACh, respectively. Note the similarities in activation patterns across the IAS and the node; the
only marked change caused by ACh is an increase in the delay between
atrial and nodal activation, with
1 increasing by 39.4% from
44.2 to 61.6 ms (Fig. 13, A and
B). The prolongation of
1 with a slight decrease in
N suggests that ACh
hyperpolarizes N cells such that the atrial current injected across a
high-resistance barrier is less effective at reaching suprathreshold
potential in the AV node. Thus a longer interval of current injection
is required to reach threshold and elicit AV node activation. The increased AV delay caused by an ACh-induced hyperpolarization can be
attributed to an injection of current across a high-resistance barrier
with passive electrical properties.

View larger version (36K):
[in this window]
[in a new window]
|
Fig. 13.
Effect of neurotransmitter ACh on AV node delay was investigated by
perfusing heart with 0.1 µM ACh. AV delay increased within seconds
after ACh perfusion, and data were acquired 2-5 min after ACh
injection (n = 5). Isochronal lines
were 2 ms apart; axes are length in millimeters.
A: control activation map recorded
immediately before ACh injection. B:
activation map recorded after 3 min of perfusion with ACh. First nodal
activation occurred at 44.2 ms in control
(A) and at 61.6 ms in presence of
ACh (B).
|
|
 |
DISCUSSION |
The study presents the first measurements of electrical propagation
across the AV node using voltage-sensitive dyes and imaging techniques.
A number of technical difficulties were overcome, including
signal-to-noise ratio, depth of focus, detection and analysis of three
sequential optical upstrokes, and display of activation maps. Several
lines of evidence were presented to support the interpretation that
peak II represented AV nodal AP and
could be used to map activation within the node.
1) The occurrence of peak II was anatomically correlated
with the location of the midnodal and lower nodal regions (Fig. 9).
2) The temporal relationship between
peak II and electrograms recorded from
the IAS and IVS indicated that peak II
originated from cells firing in the correct time frame for AV nodal
APs. 3) The spread of activation
analyzed from peak II reproducibly (in
>28 hearts) produced a zone of slow conduction distinguishable from
either atrial or ventricular propagation. 4) Under conditions in which the AV
node was the primary pacemaker, peak
II became the first upstroke to fire during a cardiac
beat and produced the same spatiotemporal zone of activation as that observed when the AV node is driven by atrial inputs.
5) After the His bundle was cut,
ventricular activation was blocked, but the spatiotemporal
characteristics of peak II did not
significantly change. 6) The signal
amplitude of peak II as a function of
depth of focus was consistent with the interpretation that
peak II originated from the firing of
APs by cells ~0.2-0.5 mm below the surface of the preparation.
7) Peak
II signals (Fig. 3D)
recorded from the posterior zone of the activation map were insensitive
to TTX. Late signals (observed in ~50% of the preparations)
consisting of a small depolarization preceding a ventricular AP
represented the firing of His bundle APs and were TTX sensitive (Fig.
10).
Peak II is not movement artifact.
A major concern was the possibility that peak
II was primarily caused by movement artifact (MA)
rather than voltage-dependent fluorescence signals. Extensive
measurements were carried out to negate that possibility.
First, all measurements were obtained with the judicious use of DAM, an
uncoupler of excitation-contraction coupling. It was important to find
suitable conditions for the use of DAM (see Staining
procedure) because perfusion with DAM for >30 min
prolonged AV delays and reduced excitability of the preparation, and
continued DAM perfusion eventually blocked all electrical activity
(measured optically or with electrodes). On the other hand, DAM
effectively blocked contractions after 8-10 min and could be
washed out to reverse its effects. In this way, DAM perfusion for 10 min gave us 15-20 min to acquire data before washing out DAM.
Second, the dF/dt of
peak II produced a sharp, unique time
point, whereas analysis of MAs by the same signal-processing technique produced neither a sharp maximum dF/dt
(see Fig. 4) nor a single maximum time point so that an activation map
could not be generated from MAs.
Third, analysis of activation patterns from peak
II were highly reproducible (>27 hearts) in the
anatomic location, the direction of propagation, and the propagation
velocity. MAs are typically unpredictable, and such a coincidence is
statistically negligible.
Fourth, in a few experiments, the
Ca2+ concentration (0.2-5 mM)
was varied to produce vastly different levels of MAs, yet the spatiotemporal characteristics of peak
II did not vary significantly.
Fifth, when the AV node was the primary pacemaker,
peak II fired first and no
interference from MA from atrial and ventricular contractions was
possible. In the latter case, the signals produced maps of electrical
activity similar to those obtained when the AV node fired after the
atrial activation.
Finally, microelectrode impalements in the midnodal zone recorded N- or
NH-cell APs that were coincident with the rise of peak
II signals, which demonstrates that
peak II depolarization originated from
the firing of N and/or NH cells.
Taken together, these findings give a high degree of confidence that
peak II represented the electrical
activity of a group of cells that fired APs in the correct anatomic
location and at the right time.
Identification of various AV node cell types.
Previous electrophysiological and morphological studies have identified
at least five different cell types in the AV node zone. A major
limitation of the optical technique is the difficulty of resolving
single cell APs by optical mapping. However, drug interventions such as
TTX proved to be useful in identifying the cell types comprising the
activation zone delineated by peak II and His depolarization (Figs. 9 and 10). For example, TTX had no effect
on propagation in the proximal region (Fig.
10A) but slowed propagation in the
distal region. This suggests that peak
II consists primarily of N and/or NH cells with
few TTX-sensitive AN or His cells, whereas the distal region contained
TTX-sensitive His cells. Another limitation of the optical techniques
was the inability to measure AP durations because signals from the
compact node consisted of superimposed atrial, nodal, and ventricular
APs. We attempted to resolve the complete time course of N-cell APs (including the repolarization phase) by increasing the optical magnification and varying the depth of focus. With the present optical
configuration, we failed to selectively measure N-cell APs, even at the
expense of decreased signal-to-noise ratio. An alternative approach
used here was to cut the His bundle to block ventricular APs and
measure N-cell AP durations. However, cutting the His bundle could
change the electrotonic coupling between NH and His fibers and thereby
alter N-cell AP durations. Despite these limitations, optical mapping
techniques offer a new approach for studying the organization and
coupling of A, AN, N, NH, and His cells in ways that cannot be resolved
by conventional electrode techniques.
Activation patterns across AV node region.
The depolarizations of peaks
I-III delineate the spread of AP propagation
across the atrial, nodal, and ventricular tissue, respectively. The
earliest depolarizations (peak I)
were synchronous with the atrial electrogram and mapped the sequence of
depolarization across the IAS, overlapping the AV node region. The time
course, distribution, and propagation velocity of these APs identified them as atrial in nature, with AN characteristics as they overlap the
AV node zone. After the last AN cell depolarization, there was a delay
of 30-40 ms (during which no other cell depolarizations could be
detected) followed by depolarizations within the node, detected by
peak II. This delay between
peak I and
II indicated that conduction was
discontinuous between AN and midnodal cells. The zone delineated by
peak II represented the firing of
midnodal cells in the posterior region of the node and lower nodal
cells in the more anterior region of the AV node (Fig. 9). In ~50%
of the preparations, His bundle APs were detected as small
depolarizations that preceded ventricular APs and delineated a narrow
track of electrically active tissue contiguous with the lower nodal
region. In line with this interpretation, there was a progressive
increase in conduction velocity from the posterior region (midnode) to the anterior track (His bundle) of the AV node. Thus, for the first
time, optical techniques provided detailed maps of the sequence of
activation across the AV node and described the organization of the
various cell types comprising the node. The data also indicated that
there was a discontinuity in conduction, with a well-defined anatomic
location between atrial and midnodal cell depolarization.
Mechanism(s) responsible for AH intervals.
A number of important conclusions can be extracted from the present
findings. One major finding is that the conduction through the AV node
is not decremental but discontinuous, and we conclude that a conduction
barrier exists between the atrial and midnodal cells. Features of this
barrier are consistent with the presence of an inexcitable gap across
which activation proceeds electrotonically through a high-resistance
pathway. Although a barrier consisting of resistance and capacitance
components is consistent with the data, we have not excluded the
possibility of a barrier with more complex electrical properties, with
possible modulation by neurotransmitters. The superimposition of
activation maps on longitudinal cross sections of the AV node suggests
that the electrical barrier surrounds the node and lies at the boundary
of the midnode and the IAS. Zones of fat deposits (adipose cells)
adjacent to the posterior and anterior zones of the AV node surround
the AV node in 3-D, according to serial longitudinal sections, and are
typically found in rabbit (6) and human AV nodes (personal
communication, Dr. L. C. Nichols, School of Medicine, University of
Pittsburgh, PA). These fat deposits likely form an effective electrical
barrier that insulates the AV node from the IAS. As a result,
electrical coupling to the AV node can only occur via narrow bridges:
one bridge connects to the IAS and the other to the cristae terminalis that are unobstructed by fat deposits.
A mathematical simulation of optical signals was developed to predict
the signal characteristics under different conditions such as
synchronous, decremental, or discontinuous conduction. The model
consisted of 15 cells of equal dimensions firing optical APs of equal
amplitude and time course, and all 15 are detected with one diode. When
all 15 cells fired APs synchronously, the resulting optical AP had a
sharp upstroke with a rise time similar to that of the single cell
upstroke (Fig.
14A).
When the cells fired with a smooth conduction delay (50 ms across 15 cells), as in decremental conduction, the resulting optical AP had a
slower rise time indicative of the time-averaged upstrokes of
asynchronous depolarizations (Fig.
14B). Only when there was an abrupt
delay (e.g., 45 ms) between APs from the first 10 cells and the last 5 cells did the resulting optical APs exhibit two distinguishable upstrokes (Fig. 14C, arrow). Thus
decremental conduction can be excluded as an AV node delay mechanism,
because the resulting optical APs from the atrium and the node would
blend into a single upstroke (not 3 temporally distinct spikes)
representing the time-averaged sum of APs (Fig.
14B). Decremental conduction is also
incompatible with our measurements of
N (Table 1). For instance, if
conduction through the node is decremental (with no "step"
changes in conduction) and accounts for AV delays, then
N should be at least 10 times slower than in the atrium. From the analysis of optical signals, the
total AV delay was the sum of
1)
the interval between A- and N-cell activation
(
1),
2) the time to propagate across the
node, and 3) the time between N- and
V-cell activation (
2; see Table 2). The conduction velocity in the node was 0.162 ± 0.024 m/s, approximately one-third that of atrial tissue (0.76 ± 0.062 m/s). However, the delay due to conduction through the node was
14 ms, an
insufficient interval to account for the AV delay. On the other hand,
delay due to discontinuous conduction between peaks I and II was 44.24 ms
or ~50% of AV delays. On the basis of these results, it can be
postulated that the major AV nodal delay is not due to the slow
conduction inside the node but to discontinuous conduction between
peaks I and
II. Moreover, when the AV node became
the primary pacemaker, the conduction barrier at the posterior margin
of the AV node was still responsible for the major component of AV
delay during retrograde as well as anterograde propagation (n = 3).

View larger version (6K):
[in this window]
[in a new window]
|
Fig. 14.
An experimentally recorded atrial AP was used to simulate optical AP
recordings during synchronous, decremental, and discontinuous
activation of 15 cells with equal dimensions and signal amplitudes.
A: synchronous activation of 15 cells.
Optical recording is a single spike representing sum of 15 APs.
B: decremental conduction of 15 cells.
Cells were coupled through a high-resistance barrier, resulting in
graded delays (50 ms) evenly distributed from first to last cell.
Optical AP is a single spike with a slow rise time caused by
asynchronous depolarization of the 15 cells.
C: discontinuous activation between
first 10 cells ("early activating cells") and last 5 cells
("late activating cells"). This model was based on a single step
delay due to a high-resistance, inexcitable barrier, resulting in
discontinuous conduction (10 early activating and 5 late activating
cells). Time to propagate across early and late activating cells was 5 ms, and there was a 45-ms delay between early and late cells. In
discontinuous conduction, optical AP will exhibit 2 distinct upstrokes
that are temporally separated according to step delay across
inexcitable gap.
|
|
The concept of an inexcitable gap in the node, resulting in
discontinuous conduction, was inferred from intracellular electrode studies (3) and simulations of AV node conduction (11, 13, 16).
Discontinuous conduction was also tested by applying a local
perturbation [i.e., current (27), high
K+ (5), freezing (26), or a
sucrose gap (2)] in otherwise uniform cardiac fibers (e.g.,
Purkinje or ventricular). In such experimental models, the perturbation
produced a step change in delay and "stagnation" similar to that
observed in the node. Step delays were caused by an interruption of
active transmission of an impulse as it arrived at the inexcitable gap.
The electrotonic transmission through the inexcitable gap slowly
charged distal cells until the resting potential of the distal cells
reached threshold and ignited active transmission in the distal cells. It is critically important that the step delay is determined by the
time needed to inject the electrotonic current necessary to induce
active transmission in the distal cells. James et al. (10) also argued
against decremental conduction because AV delays were not proportional
to the size of the AV node in various mammalian hearts. They proposed
that pacemaker cells are involved in the AV delay as coupled relaxation
oscillators modulated by electrotonic atrial inputs.
The location and nature of the inexcitable gap and of discontinuous
conduction are still controversial. Early studies (18) indicated that
the major component of AV delay occurred between the firing of late AN
and early N cells. Subsequent findings by Billette et al. (3, 4) showed
that, at short cycle lengths, the interval between an atrial
electrogram and the latest AN cell had not changed; the delay occurred
between the latest AN cell and the earliest NH cell. Moreover, at a
short cycle length (130 ms), N-cell AP dissociated into two components:
the first component coincided with the AP upstroke of late AN cells,
and the second component coincided with the AP upstroke of the earliest
NH cells. No AP upstrokes were found in between. The conclusion was
that, at a short cycle length, the N zone (approximately equivalent to
the compact node) became inexcitable and only transmitted electrotonic currents that slowly brought distal NH cells to threshold. This implied
that N cells were the actual barrier (3, 4). The present optical data
are in agreement with the early studies of AV propagation (18) and
showed that, under a wide range of physiological rates (250- to 500-ms
cycle lengths), the major component of delay resides between the latest
AN and earliest N cells. In our intact heart preparations, attempts to
drive the AV node at higher rates produced unstable AV coupling, making
it unsuitable to reexamine the observation of Billette et al. (4).
The present study provides robust evidence for a step jump in
conduction across a well-defined anatomic gap. The regulation of the
time delay across this gap as a function of cycle length and ACh
indicates that delays across this gap play a major mechanistic role in
the physiological control of AV delay. Prolongation of AV delay by ACh
is consistent with the notion proposed by James et al. (10) that the AV
node is a pacemaker modulated by electrotonic inputs. The latter
interpretation is based on a hyperpolarization of AV nodal cells by ACh
such that a greater input of current is required across the inexcitable
gap to obtain a suprathreshold depolarization that can activate the AV
node. Thus the present data are incompatible with a decremental
conduction mechanism and provide direct evidence for the existence of a
conduction barrier, its specific anatomic location, and a measurement
of the step delay (
1)
involved in the physiological regulation of AV delay. This study raises
new questions regarding the mechanisms underlying
1 and AV delays and
demonstrates the potential of optical techniques to elucidate basic
problems in AV node physiology and salient clinical problems.
 |
ACKNOWLEDGEMENTS |
The authors are grateful for the inspiration of the late Richard A. Lombardi. The authors thank Dr. Gregory Kloehn for technical assistance
and William Hughes, departmental machinist, for construction of the
heart chamber and manipulators to adjust the focal plane of the optical
apparatus and to position stimulating and surface recording electrodes.
Thanks are also due Drs. Ronald L. Hamilton and Lawrence C. Nichols
(Dept. of Pathology, University of Pittsburgh, PA) for technical
support and guidance regarding analysis and interpretation of the AV
node histology.
 |
FOOTNOTES |
Address for reprint requests: G. Salama, Dept. of Physiology, School of
Medicine, Univ. of Pittsburgh, 3500 Terrace St., Room 2, 314 Biomedical
Science Tower, Pittsburgh, PA 15261.
Received 7 February 1997; accepted in final form 22 August 1997.
 |
REFERENCES |
1.
Anderson, R. H.,
M. J. Janse,
F. J. L. Van Capelle,
J. Billette,
A. E. Becker,
and
D. Durrer.
A combined morphological and electrophysiological study of the atrioventricular node of the rabbit heart.
Circ. Res.
35:
909-922,
1974[Abstract/Free Full Text].
2.
Antzelevitch, C.,
and
G. K. Moe.
Electrotonically mediated delayed conduction and reentry in relation to "slow response" in mammalian ventricular conduction tissue.
Circ. Res.
49:
1129-1139,
1981[Abstract/Free Full Text].
3.
Billette, J.
Atrioventricular nodal activation during premature stimulation of the atrium.
Am. J. Physiol.
252 (Heart Circ. Physiol. 21):
H163-H177,
1987[Abstract/Free Full Text].
4.
Billette, J.,
M. J. Janse,
F. J. L. van Capelle,
R. H. Anderson,
P. Touboul,
and
D. Durrer.
Cycle-length-dependent properties of AV nodal activation in rabbit hearts.
Am. J. Physiol.
231:
1129-1139,
1976.
5.
Cranefield, P. F.,
H. O. Klein,
and
B. F. Hoffman.
Conduction of the cardiac impulses. 1. Delay, block, and one-way block in depressed Purkinje fibers.
Circ. Res.
28:
199-219,
1971[Abstract/Free Full Text].
6.
DeFelice, L. J.,
and
C. E. Challice.
Anatomical and ultrastructural study of the electrophysiological atrioventricular region of the rabbit.
Circ. Res.
24:
457-474,
1969[Abstract/Free Full Text].
7.
Efimov, I. R.,
D. T. Huang,
J. M. Rendt,
and
G. Salama.
Optical mapping of repolarization and refractoriness from intact hearts.
Circulation
90:
1469-1480,
1994[Abstract/Free Full Text].
8.
Gettes, L. S.,
J. W. Buchanan, Jr.,
T. Saito,
Y. Kagiyama,
S. Oshita,
and
T. Fujino.
Studies concerned with slow conduction.
In: Electrophysiology and Arrhythmias, edited by D. P. Zipes,
and J. Jalife. Orlando, FL: Grune and Stratton, 1985, p. 81-87.
9.
Hoffman, B. F.,
and
P. F. Cranefield.
Electrophysiology of the Heart. New York: McGraw-Hill, 1960.
10.
James, T. N.,
K. Kawamura,
F. L. Meijler,
S. Yamamoto,
F. Terasaki,
and
T. Hyashi.
Anatomy of the sinus node, AV node, and His bundle of the heart of the sperm whale (Physeter macrocephalus), with a note on the absence of an os cordis.
Anat. Rec.
242:
355-373,
1995[Medline].
10a.
Janse, M. J.,
F. J. L. van Capelle,
R. H. Anderson,
P. Touboul,
and
J. Billette.
Electrophysiology and structure of the atrioventricular node of the isolated rabbit heart.
In: The Conduction System of the Heart: Structure, Function and Clinical Implications, edited by H. J. J. Wellens,
K. I. Lie,
and M. J. Janse. Leiden, The Netherlands: Stenfert Kroese, 1976, p. 296-315.
11.
Kinoshita, S.,
and
G. Konishi.
Mechanisms of atypical atrioventricular Wenchebach periodicity. A theoretical model derived from the concepts of inhomogeneous excitability and electrotonically mediated conduction.
J. Electrocardiol.
22:
227-233,
1989[Medline].
12.
Kokubu, S.,
M. Nishimura,
A. Noma,
and
H. Irisawa.
Membrane currents in the rabbit atrioventricular node cell.
Pflügers Arch.
393:
15-22,
1982[Medline].
13.
LeBlanc, A. R.,
and
B. Dube.
Propagation in the AV node: a model based on a simplified two-dimensional structure and a bidomain tissue representation.
Med. Biol. Eng. Comput.
31:
545-565,
1993[Medline].
14.
Loew, L.,
L. Cohen,
J. Dix,
E. Fluhler,
V. Montana,
G. Salama,
and
W. Jian-Young.
A naphthyl analog of the aminostyryl pyridinium class of potentiometric membrane dyes shows consistent sensitivity in a variety of tissue, cell and model membrane preparation.
J. Membr. Biol.
130:
1-10,
1992[Medline].
15.
Luna, L. G.
Manual of Histological Staining Methods of the Armed Forces Institute of Pathology (3rd ed.). New York: McGraw-Hill, 1968, p. 36-38.
16.
Malik, M.,
D. Ward,
and
A. J. Camm.
Theoretical evaluation of the Rosenblueth hypothesis.
Pacing Clin. Electrophysiol.
11:
1250-1261,
1988[Medline].
17.
Meijler, F. L.,
and
M. J. Janse.
Morphology and electrophysiology of the mammalian atrioventricular node.
Physiol. Rev.
68:
608-647,
1988[Abstract/Free Full Text].
18.
Paes de Carvalho, A.,
and
D. F. De Almeida.
Spread of activity through the atrioventricular node.
Circ. Res.
8:
801-809,
1960[Abstract/Free Full Text].
19.
Piller, H.
Microscope Photometry. New York: Springer-Verlag, 1977, p. 16.
20.
Salama, G.
Optical measurements of transmembrane potentials in heart.
In: Spectroscopic Probes of Membrane Potential, edited by L. Lowe. Boca Raton, FL: CRC Uniscience, 1988, p. 132-199.
21.
Salama, G.,
A. Kanai,
and
I. R. Efimov.
Subthreshold stimulation of Purkinje fibers interrupts ventricular tachycardia in intact hearts.
Circ. Res.
74:
604-619,
1994[Abstract/Free Full Text].
22.
Salama, G.,
R. Lombardi,
and
J. Elson.
Maps of action potential and NADH fluorescence in intact working hearts.
Am. J. Physiol.
252 (Heart Circ. Physiol. 21):
H384-H394,
1987[Abstract/Free Full Text].
23.
Salama, G.,
and
M. Morad.
Merocyanine-540 as an optical probe of transmembrane electrical activity of the heart.
Science
191:
485-487,
1976[Abstract/Free Full Text].
24.
Sano, T.,
M. Tasaki,
and
T. Shimamoto.
Histologic examination of the origin of the action potential characteristically obtained from the region bordering the atrioventricular node.
Circ. Res.
7:
700-704,
1959[Abstract/Free Full Text].
25.
Tawara, S.
Das Reizleitungs System des Herzens. Jena, Germany: Fisher, 1906.
26.
Waxman, M. B.,
E. Downar,
and
R. W. Wald.
Unidirectional block in Purkinje fibers.
Can. J. Physiol. Pharmacol.
58:
925-933,
1980[Medline].
27.
Wennemark, J. R.,
V. J. Ruesta,
and
D. A. Brody.
Microelectrode study of delayed conduction in the canine right bundle branch.
Circ. Res.
23:
753-769,
1968[Abstract/Free Full Text].
28.
Young, M.-L.,
B. M. Ramaza,
R. C. Tan,
and
R. W. Joyner.
Adenosine and hypoxia effects on atrioventricular node of adult and neonatal rabbit hearts.
Am. J. Physiol.
253 (Heart Circ. Physiol. 22):
H1192-H1198,
1987[Abstract/Free Full Text].
AJP Heart Circ Physiol 274(3):H829-H845
0363-6135/98 $5.00
Copyright © 1998 the American Physiological Society