(Circulation. 1995;92:219-230.)
© 1995 American Heart Association, Inc.
Articles |
From the Division of Pediatric Cardiology, Department of Pediatrics (M.A.F., P.M.W.), and the Department of Radiology (K.E.F., E.A.H.), The Children's Hospital of Philadelphia, Philadelphia, Pa.
Correspondence to Mark A. Fogel, MD, The Children's Hospital of Philadelphia, The Division of Cardiology, 34th St and Civic Center Blvd, Philadelphia, PA 19104. E-mail mark@arielle.cardio.chop.edu.
| Abstract |
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Methods and Results A noninvasive magnetic resonance tagging technique (spatial modulation of magnetization [SPAMM]) that lays intersecting stripes down on the myocardium was used to examine 18 patients with systemic right ventricles: 7 with a single right ventricle who have undergone the Fontan procedure (age, 38.8±8.9 months) and 11 with transposition of the great arteries who have undergone an atrial inversion operation (age, 16.3±3.9 years). The motion of the intersection points was tracked through systole to determine regional twist and radial shortening. Shortening rates also were evaluated. Finite strain analysis was applied to the grid lines using Delaunay triangulation, and the two-dimensional strain tensor and principal E1 strains were derived for the various anatomic regions. Basal and apical short-axis planes through the ventricular wall were categorized into four distinct regions spaced equally around the circumference of the slice. We observed the following results. (1) Strain was greatest and heterogeneity of strain was least in patients with transposition of the great arteries who were status post atrial inversion operation (six of eight regions). Marked differences were noted in the distribution of strain within a given region, from endocardium to epicardium, and from atrioventricular valve to apical plane between patient subtypes and those with a normal left ventricle. (2) Contrary to the normal subject studied by the use of the same method, for both patient subtypes, there was counterclockwise twist in one region, clockwise twist in the posterior or inferior wall, and a transition zone of no twist at which the two regions of twist met. Normal human adult left ventricles studied in short-axis twist uniformly counterclockwise as viewed from apex to base. (3) Radial inward motion was greatest in the superior wall of both types of systemic right ventricle. The inferior walls of Fontan patients and the posterior (ie, septal) walls of patients with transposition of the great arteries, status post atrial inversion, moved paradoxically in systole. The shortening rate at the atrioventricular valve of patients with transposition of the great arteries, status post atrial inversion, was significantly lower than at the apex or in Fontan patients.
Conclusions Marked differences in regional wall motion and strain were demonstrated in systemic right ventricles, depending on whether a left ventricle was present to augment its function. Ventricularventricular interaction appears to play an important role in affecting the biomechanics of systemic right ventricles. These observations were markedly different from those in the normal systemic left ventricle. These techniques demonstrate tools with which we can begin to evaluate surgical outcomes using regional myocardial mechanics and may provide a clue to single right ventricle failure.
Key Words: contraction ventricles Fontan procedure transposition of the great arteries
| Introduction |
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Patients with single RVs presently undergo a staged surgical reconstruction culminating in the Fontan procedure.6 7 8 9 Long-term success and viability of the single ventricle have been evaluated after surgery by the use of hemodynamic and anatomic parameters only.9 10 We have observed that a subgroup of these patients present with RV failure of unknown cause (eg, clinical congestive heart failure, poor systolic shortening, high end-diastolic pressure, significant tricuspid regurgitation, and so on). Because by definition single RVs do not have a second ventricle to augment function, the question arises of whether the lack of interaction with an LV contributes to failure in some single RVs.
We had an opportunity to study patients with systemic RVs with and without an associated LV to determine V-V interaction by comparing single RVs in patients who have undergone the Fontan procedure (Fontan patients)6 7 8 9 10 with those who have transposition of the great arteries (TGA) and have undergone an atrial inversion procedure (ie, Senning or Mustard operation) (status post [S/P] TGA patients).11 12 13 Both patient groups have postoperative intra-atrial baffles, making them even more comparable.
Using a noninvasive magnetic resonance tagging technique, we previously demonstrated that significant alterations exist in the myocardial mechanics across surgical stages of the Fontan procedure and between myocardial regions at each stage.14 15 In the present study, we evaluated regional myocardial strain and wall motion of the single RV after Fontan repair and S/P TGA by using a newly developed magnetic resonance imaging technique to determine regional myocardial twist, radial contraction, and strain. The normal human LV studied in our laboratory is used for reference.16
Regarding twist, as early as 1669, Richard Lower observed that cardiac motion was like the "wringing of a linen cloth to squeeze out the water."17 Subsequent investigators have demonstrated and quantified LV twisting along its long axis, although there is debate about direction.17 18 19 20 21 22 23 24 25 26 27 28 29 We and others26 28 29 believe there is an initial LV counterclockwise twist (viewed apex to base) in early systole and that when the apex stops twisting, the base begins to untwist with wringing of the myocardium.
Strain, a unitless measure of deformation, is believed to be coupled with rotational dynamics17 19 and relates myocardial wall distortion during systole to end diastole (ie, the fractional change in dimension or size of the myocardium from the unstressed dimension that results from the application of a stress, which is defined as force divided by cross-sectional area18 30 ). It is a component of the regional tensionarea diagram, which measures regional work, and has been shown to correlate with regional oxygen consumption in certain instances.31 Numerous studies have evaluated stress and strain in the normal LV,16 29 32 33 34 35 36 37 including the use of magnetic resonance tagging,16 29 37 38 39 40 which has recently been validated.38 These studies have suggested that due to the interplay between torsion and contraction, LV strain and shortening are distributed in a specific manner across the ventricular wall.
We hypothesize that single RV mechanics (twist, regional radial motion, and associated regional strain) differ from that of the RV of S/P TGA patients and from the normal LV because of a lack of V-V interaction. New image-acquisition techniques (magnetic resonance imaging and spatial modulation of magnetization [SPAMM]38 39 40 ) coupled with a broad-based image-analysis capability have made this in vivo evaluation possible.
| Methods |
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Magnetic Resonance Imaging
All Fontan patients and 4 of 10
S/P TGA patients were sedated
before imaging. If less than 2 years old, the patient was administered
either chloral hydrate (75 to 120 mg/kg PO) or Nembutal (2 to 6 mg/kg
IV). If more than 2 years old, either Nembutal (4 mg/kg PO) and Demerol
(3 mg/kg PO), Nembutal (2 to 6 mg/kg IV), or Ativan (5 mg PO) was
administered. All patients were monitored with pulse oximetry, nasal
end-tidal CO2, ECG, and direct visualization via
television. All patients tolerated sedation without incident.
Studies were performed with a Siemens 1.5-T Magnetom. The scanning protocol was as follows. First, a stack of coronal localizers were acquired to locate the heart in the chest. T1-weighted transverse images that spanned the region of the heart were then acquired to evaluate cardiovascular anatomy and were used as a localizer for subsequent magnetic resonance tagging. The effective repetition time (TR) equaled RR interval (range, 350 to 800 milliseconds); echo time (TE) equaled 15 milliseconds; and the number of excitations was three.
Second, the method designed to standardize
the RV short axis is shown
in Fig 1
. The short-axis plane was defined as being
perpendicular to the long-axis plane, and the long-axis plane was
defined as being perpendicular to the atrioventricular
valve plane and intersecting both the atrioventricular
valve and the apex. Short-axis images were acquired by the use of the
following localizers (Fig 1
). (1) Four to six
T1-weighted
images were obtained through the plane of the
atrioventricular valve by the use of the transverse
images as a localizer (one signal average). This ensured that there
were images in the plane of the atrioventricular valve
(Fig 1
, images I and II). (2) On an image that contained both
atrioventricular valves or their remnants (in cases of
atresia or stenosis), an imaginary estimated line was drawn
between the two valves (images III and IV). Four to six
T1-weighted images were obtained perpendicular to this
imaginary line to provide an image of both the
atrioventricular valve and the apex in a
ventricular long-axis view (Fig 1
, image IV). (3) With the
ventricular long-axis view (image V), an imaginary line was
drawn that was the length of the ventricle through both
atrioventricular valve and apex. This line was divided
into thirds, and two images (one is one third of the way from the
atrioventricular valve to the apex [designated
"atrioventricular valve"] and one is two thirds
of the way from the atrioventricular valve to the apex
[designated "apex"]) were obtained orthogonal to this
(image
VI) to provide short-axis SPAMM images. End diastole was
determined by the R wave on ECG.
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Third, regarding myocardial tagging,
the SPAMM
sequence38 39 40 uses multiple
radiofrequency pulses of
130° separated in time and a series of gradient radiofrequency pulses
to produce saturated spins in two sets of parallel stripes that are
perpendicular to each other (black on the image) followed by a standard
gradient echo sequence dividing the wall into "cubes of
magnetization" (Fig 2A
and 2B
). Images 4
to 7 mm
thick are acquired every 25 milliseconds for 12 phases from end
diastole, and in plane tissue motion moves and distorts
these cubes of magnetization. Tracking of this movement and distortion
allows assessment of motion and deformation. TR equaled RR interval
(range, 350 to 800 milliseconds); inversion time (TI) equaled 16
milliseconds; flip angle equaled 30°; the number of excitations was
three; and the matrix size was 256x256. Grid lines were spaced to
allow three or four lines to be laid down between endocardial and
epicardial surfaces (ie, three or four rows of cubes; Fig 2A
and 2B
).
Tag thickness ranged from 1.5 to 2 mm.
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Data Analysis
Images were downloaded from the Magnetom onto a
Sun SPARC 10
workstation (Sun Microsystems). VIDA (Volumetric Image
Display and Analysis)41 was used to manipulate the
images; this system uses a UNIX/X Windows graphic
interface with a shared memory structure designed to hold
multiple-volume image sets. Images were displayed with the use of a
color scale that was linear over the dynamic range of the Sun video
monitor. The window and level display parameters were held
constant throughout the analysis of a complete cardiac cycle
for a given patient, and the contrast and brightness controls of the
Sun monitor always were set to their maximum gain.
To determine wall
motion and strain, we tracked manually each SPAMM
line intersection point (Fig 2A
, image I) through systole
(typically
for at least six phases) with a computer-based image with the use of a
video cursor and mouse (Fig 2A
, image II). Next, the
intersection
points were connected automatically to form uniform, nonoverlapping
triangles using the mathematical technique of Delaunay
triangulation42 43 (Fig 2A
, image
III). Using the centroid
of each triangle (Fig 2A
, image IV) and wall motion software,
we
computed the regional wall motion across the short-axis plane of the
ventricle (Fig 2A
, image V). Furthermore, complete
two-dimensional finite strains (a measure of the amount of deformation
experienced locally by the myocardium18 30 )
within each triangle were computed at the measured phases (Fig
2B
) with
the use of strain software. The SPAMM technique has been validated for
these measurements.38
Wall Motion
Regional
wall motion was determined by mathematically computing
the centroid of all triangles during each phase of systole that was
imaged. Twist and radial shortening were measured relative to the
ventricular center of mass (Fig 2A
, image VI). The
coordinates (x and y) of the centroid of the
ventricular cavity were obtained at end
diastole through computer-based user-interactive tracing of
the endocardial border and then computation of the center based on the
border location. With a global Cartesian coordinate system, the
difference between the distance of the centroid of
triangleA on the myocardial wall created by Delaunay
triangulation42 43 to the centroid of the
ventricular cavity at phase n and n+1 (ie, how far the
muscle marked by the triangle was displaced away from the centroid of
the ventricular cavity from phase n to phase n+1) is
represented by the following
equation:
![]() |
where
(xn,
yn), and (xn+1,
yn+1) are the coordinates of the centroid of
triangleA at phase n and n+1, respectively;
(xc, yc) are
coordinates of the centroid of the ventricular cavity; and
Pn and Pn+1 are vectors from the centroid of
the cavity to the centroid of triangleA at phase n and n+1,
respectively. The angle
(made by the two vectors drawn from the
centroid of the ventricular cavity to the centroid of
triangleA at phases n and n+1 (ie, twist around the
centroid of the ventricular cavity) is
represented by the following
equation:
![]() |
where
Pn and Pn+1 are vectors
(IPnI and IPn+1I are the lengths of those
vectors) from the centroid of the cavity to the centroid of
triangleA at phase n and n+1, respectively, and
Pn · Pn+1 is the vector dot product.
Wall motion data were displayed as depicted in Fig 2A
, image V.
"Dots" represent end-diastolic triangle
centroid location, and "tails" represent the subsequent
motion. By convention, clockwise motion was negative and
counterclockwise was positive, when viewing the heart apex to base.
Parameters that were quantified were the magnitude and
direction of net twisting; motion throughout systole (sampling at six
to eight time points) also was observed graphically (Fig 2A
).
Radial motion was measured as the net inward motion of each
triangle's
centroid toward the centroid of the ventricular cavity
relative to the end-diastolic distance (measured in pixels
of distance moved divided by initial radial length to normalize for
heart size [Fig 2A
, images V and VI]) and was
displayed to depict
each triangle's centroidal motion. By convention, radial motion inward
was positive, and radial motion outward was negative.
Analysis necessitated dividing the myocardial wall into various standard regions (anterior, posterior, superior, and inferior walls).
Strain Analysis
As mentioned,
finite strain analysis relates myocardial
deformation during systole and uses end diastole as a reference (Fig
2B
).18 30 This parameter of cardiac
mechanics
is unitless and, in its simplest form in two dimensions, is defined as
initial shape and size minus final shape and size divided by initial
shape and size. From two-dimensional datasets, even the most complex
finite deformation can be decomposed into two length changes and two
associated angle changes. These measurements can easily be converted to
finite strains of continuum mechanics (consisting of two normal strain
vectors and two shear strain vectors). Based on previous
work,36 two-dimensional finite strains were computed and
are reported in the present study as their associated principal E1
strains.
Strain calculations used the two-dimensional strain tensor and
the
method of eigen system solutions to solve for principal strains, which
are the maximum and minimum strains experienced by each triangle.
Principal strain E1, reported in the present study,
represents the most negative strain value (myocardial
compression) (Fig 2B
). Strain in a given region at a given
phase was
obtained by averaging the strain of all the triangles within the region
and reporting it as mean±SD. Our research focused on the maximum
strain observed in the region throughout systole. An underlying
assumption of our analysis is that cardiac muscle deformation
is homogeneous within each triangle. The data were
quantified and displayed in a color-coded format superimposed onto the
anatomic images (Fig 2B
).
Shortening Rates
Because of regional wall motion abnormalities and because
standardization of velocity of circumferential fiber shortening is
lacking in the morphological right ventricle, fractional area
shortening per unit time was used for shortening rate calculations. To
determine systolic and end-diastolic cavity areas at the
atrioventricular valve and apical short-axis levels,
the endocardial borders at end diastole and in mid to late
systole were traced manually (Fig 2A
, image VI) with the aid of
a
mouse. Computerized counting of the pixels enclosed by this border
yielded the area; the following formula was used:
![]() |
![]() |
where
ED is end-diastolic, area is measured in
square millimeters, and time is measured in seconds. Time between
images was
150 milliseconds.
Statistical Analysis
Comparisons between two mean values were
made with the use of
the unpaired, two-way, Student's t test and the Wilcoxon
ranked sum test. Differences between various groups of patients and
location (regional wall location, short-axis slice of either apex or
base) were analyzed with the use of two-factor ANOVA with
repeated measures used when appropriate. Comparison between multiple
mean values within groups was made with the use of one-way ANOVA, with
pairwise comparisons made with the use of Scheffé's F test or
Fisher's protected least squares test. All measurements are given as
mean±SD. Intraobserver variability was determined by replicate
measures using the coefficient of variability. One trained observer
performed all image-analysis steps. Significance was defined as
P<.05. Statistical analysis was performed with a
Macintosh II computer using STATVIEW II version 1.03
software (Abacus Concepts).
To obtain the homogeneity of strain within the region, the coefficient of variation was used and derived as follows:
![]() |
To compare endocardial strains with epicardial strains and to compare strains between atrioventricular valve and apical short-axis planes, the natural logarithm (ln) of the ratio of the endocardial to epicardial strain (eg, ln [endocardial strain/epicardial strain]) was used. This was advantageous in that significant differences implied significant differences in the geometric mean values of the two groups being compared.
| Results |
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Strain
Fig 3A
through 3C
displays strain data
in a
color-coded format superimposed over the anatomic image. Fig 4A
and 4B
displays principle compressive strain (E1 multiplied
by -1) for both Fontan and S/P TGA patients in the four anatomic
quadrants (anterior, inferior, posterior, and superior
walls) evaluated in two short-axis planes (one near the
atrioventricular valve and one near the apex).
Coefficient of variation for strain measurements was 6.2±1.6%. At the
atrioventricular valve level (Fig 4A
), S/P TGA patients
demonstrated greater compressive strain in the anterior and posterior
walls (negative strain value furthest from zero) than Fontan patients
(P<.05). Among Fontan patients, significantly less strain
was found in the anterior wall than other wall regions
(P<.05), whereas among S/P TGA patients, greater strain was
found in the posterior wall (P<.05). At the apical level
(Fig 4B
), S/P TGA patients had greater strain than Fontan
patients in
all regions except the posterior wall (P<.05).
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Distribution of Strain
Heterogeneity of Strain Within a
Given Anatomic
Region
At the atrioventricular valve level (Fig 5A
),
Fontan patients had the greater
heterogeneity of strain in all regions except the
superior wall (P<.05). Anterior and superior walls among
S/P TGA patients and the anterior wall among Fontan patients displayed
the greatest heterogeneity of strain
(P<.05). At the apical level (Fig 5B
), Fontan
patients had
greater heterogeneity of strain than S/P TGA patients
in only two regions (anterior and inferior), whereas S/P
TGA patients had a greater heterogeneity of strain in
the posterior wall (P<.05). It was the anterior and
inferior walls among Fontan patients and the posterior wall
among S/P TGA patients that had greater heterogeneity
of strain than other regions (P<.05).
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EndocardialtoEpicardial Strain Ratio Within a
Given Anatomic
Region
Fig 5C
and 5D
displays the ln of
the endocardialtoepicardial
strain ratio (a positive value implies endocardial>epicardial strain;
a negative value implies endocardial<epicardial strain). At the
atrioventricular valve level (Fig 5C
), Fontan patients
differed from S/P TGA patients in all regions (P<.05).
Among Fontan patients, inferior and posterior walls had
positive values (ie, endocardial>epicardial strain as in the normal
human LV16 ), whereas the anterior and superior walls had
negative values. Among S/P TGA patients, the superior wall had a
significantly positive value (P<.05), whereas all other
regions were not significantly different from 0 (ie,
endocardial=epicardial strain). At the apical level (Fig
5D
), S/P TGA
patients demonstrated endocardial<epicardial strain (negative
values, opposite of the normal LV pattern16 ) in all four
regions, which differed significantly from Fontan patients, who had
only two of four regions with that profile (more negative than S/P TGA
patients at the inferior wall, less negative at the
posterior wall) (P<.05). Among S/P TGA patients, the
posterior wall had the most negative value of all regions (ie,
endocardial<<epicardial strain) (P<.05).
Atrioventricular ValvetoApical Plane Strain
Ratio (Distribution of Strain Along the Long Axis of the
Ventricle)
Fig 5E
displays the ln of the
atrioventricular
valvetoapical plane strain ratio (a positive value implies
atrioventricular valve>apical plane strain; a negative
value implies atrioventricular valve<apical plane
strain). S/P TGA patients differed significantly from Fontan patients
in all four regions (P<.05). Among Fontan patients, all
regions had positive values (ie, atrioventricular valve
plane>apical plane strain, the pattern followed by normal
LVs23 ). Among S/P TGA patients, the posterior wall had the
highest positive value of all wall regions in either patient subtype,
whereas the superior wall showed a significantly negative value (ie,
atrioventricular valve plane<apical plane strain)
(P<.05). Both anterior and inferior walls did
not differ significantly from 0 (ie, atrioventricular
valve plane=apical plane strain).
Wall Motion
Twist
Fig 3A
through
3C
(left) depicts in graphic format the twisting
motion in short axis of Fontan patients, S/P TGA patients, and the
normal LV as studied in our laboratory, whereas Fig 6A
and
6B
quantitatively displays the data. Intraobserver
variability was 5.6±1.9%. At the atrioventricular
valve level (Fig 6A
), Fontan and S/P TGA patients twisted
significantly
differently in the inferior and posterior walls (S/P TGA
patients had counterclockwise [ie, +] movement and Fontan
patients
had clockwise movement at the inferior wall, whereas at the
posterior wall, S/P TGA patients had significantly more clockwise twist
than Fontan patients [P<.05]). Among Fontan patients,
both inferior and posterior walls twisted clockwise,
whereas the superior wall did not twist and the anterior wall twisted
counterclockwise. Among S/P TGA patients, only the posterior wall moved
clockwise, whereas the other walls moved counterclockwise. At the
apical level, however (Fig 6B
), it was only the posterior wall
in both
patient types that demonstrated twist in the clockwise direction,
whereas all other walls moved counterclockwise (P<.05). The
superior wall of Fontan patients demonstrated the most counterclockwise
movement of all regions (P<.05).
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Note the uniform
counterclockwise motion of the normal LV (Fig 3A
)
across both short-axis planes. Compare this motion with that of the
single RV, S/P the Fontan procedure (Fig 3B
) and the systemic
RV of S/P
TGA patients (Fig 3C
). Note the similarity of twisting motion
in both
types of RVs, with regions of clockwise and counterclockwise twists
that meet in a region of no twist that we call the "transition
zone," which had any one of three types of radial motion (inward,
outward, or paradoxical).
Radial Motion
Fig
3A
through 3C
displays in graphic format and Fig
6C
and 6D
displays in quantitative format the net radial motion along the short
axis of the ventricle. Intraobserver variability was 5.4±1.7%. At the
atrioventricular valve level (Fig 6C
), S/P TGA patients
and Fontan patients had movement in opposite directions at the
inferior and posterior walls (P<.05). Both
patient types at this short-axis level had paradoxical systolic wall
motion and differed only in the region in which it occurred (the
posterior [septal wall] for S/P TGA patients and the
inferior wall for Fontan patients). Both patient types had
the greatest inward radial motion at the superior wall at both the
atrioventricular valve and apical levels
(P<.05). Similar to the atrioventricular
valve level, at the apex (Fig 6D
) both patient types had
paradoxical
systolic wall motion, differing only in the region in which it occurred
(the posterior [septal wall] for S/P TGA patients and
inferior wall for Fontan patients), and the superior wall
had the greatest inward radial motion.
Shortening Rates
Shortening rates differed significantly between Fontan and S/P TGA
patients at the atrioventricular valve short-axis level
(2.02±0.23 and 1.51±0.18 s-1, respectively,
P<.05) but not at the apical short-axis level (1.99±0.12
and 2.22±0.34 s-1, respectively). Although there
was no significant difference between atrioventricular
valve and apical short-axis levels in the Fontan group, a significant
difference did exist in the S/P TGA group (see above;
P<.05).
| Discussion |
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We observed a number of patients with single RVs who have undergone the Fontan procedure to present with failing ventricles. To supplement hemodynamic and anatomic information, we evaluated regional wall mechanics in the hope of gaining a broader understanding of heart function and to determine the effects of V-V interaction. We previously evaluated the hearts of patients at various stages of Fontan reconstruction with the use of magnetic resonance tagging.14 15 44 Based on standard anatomic regions, we have demonstrated that distinct mechanical differences, based on strain measures, can be demonstrated between surgical subgroups.14 15 We have also shown that wall motion of the single ventricle is distinct and significantly different from that of the normal LV and that when the myocardium is divided according to patterns of motion, a region of significantly increased strain (the transition zone) is found.14
By defining the altered twist, shortening, and strain relations observed in the present study, it is our hope to have added to the groundwork needed to follow individual patients on a long-term basis and to begin to understand circumstances leading to and/or predicting failure. We further hope to define the role that V-V interaction, or the lack of, plays in the functioning of the single RV and whether V-V interaction is necessary for the long-term health of the heart.
In the Fontan procedure,6 7 8 9 10 all systemic venous return is channeled into the pulmonary arteries and bypasses the ventricle through direct anastomosis of superior vena(e) cava(e) to the pulmonary artery and through a hemicylindrical polytetrafluoroethylene baffle in the atria to direct inferior vena caval flow to the pulmonary artery. In the atrial inversion operation,11 12 13 a baffle is also placed in the atria to baffle systemic venous blood to the mitral valve and pulmonary venous blood to the tricuspid valve. Hoffman28 and Cristesue et al45 noted that atrial fibrillation and perhaps reduced atrial compliance or loss of atrial systole can cause an important ventricular afterload. The atrial baffles of both patient types that we studied may act similarly to cause an increased stress on the ventricle and may affect its long-term function. This may be why both types of systemic RVs differ functionally from the normal human LV.
Our analysis broke down ventricular biomechanical properties not only between Fontan and S/P TGA patients but also between regions within each patient subtype. Results from the present study indicate that strain in certain regions differed depending on whether a second ventricle was present to augment its function. Furthermore, strain was not distributed uniformly around the ventricular short axis in a given patient subtype, but rather certain walls appeared to deform to a greater degree than others, again, depending on whether an LV was present. Strain was greater in six of the eight regions studied (four regions at two short-axis levels) in S/P TGA patients than in Fontan patients and, although it did not reach statistical significance, was greater in a seventh. It is interesting to note that in S/P TGA patients, the posterior wall (ie, septal wall) is shared by both ventricles and is under the greatest strain. As a reference, in the normal human LV16 studied in our laboratory, the posterior free wall demonstrated the highest strain at the atrioventricular valve and apex levels. It may be that the geometric changes induced in the septum (ie, concave on the RV side and convex on the LV side, whereas the normal heart is the reverse) by such factors as fiber angle orientation and transmural pressure gradients play a role in this finding.
As noted, due to the interplay between torsion and contraction, normal LV stress and strain are distributed in a specific manner across the wall.29 32 33 34 35 36 37 Heterogeneity of strain is a measure of this nonuniformity. Within a given region, this distribution of strain depended on whether an LV was present to augment function. Five of eight regions demonstrated that not only were S/P TGA patients under greater strain but also the heterogeneity of this strain within a given region was less than that for Fontan patients, and in two of eight regions, there was no difference between patient subtypes. Also of note is that in general, regardless of whether the patient was S/P TGA or Fontan, the greater the strain, the more homogeneous was the strain within that region.
Other measures of distribution of strain in the myocardium (endocardialtoepicardial and atrioventricular valvetoapical plane strain ratios) also showed significant differences between patient types and from the normal human LV.16 In a number of regions, both S/P TGA and Fontan patients displayed a reversal of the endocardialtoepicardial strain ratio (ie, endocardial strain<epicardial strain) as well as a reversal of atrioventricular valvetoapical plane strain ratio (ie, atrioventricular valve strain<apical strain) of those of the normal human LV.16 There also were significant differences between S/P TGA and Fontan patients in all regions, demonstrating that V-V interaction affects not only absolute amounts of strain but also its distribution.
Twist and radial motion also were affected. Twisting on a microscopic
level, is believed to be a combination of complex fiber architecture
coupled with electrical activation sequences, allowing sarcomere
shortening to be distributed in a specific manner throughout the thick
wall of the normal
LV17 18 19 20 21 22 23 24 25 26 27
(Fig 3C
; data from our
laboratory). This torsion is believed to allow sarcomere stress,
strain, and energy requirements to be minimized across the
myocardium independent of loading
conditions.18 19 20 Magnetic resonance
tagging38 39 40 has been used
successfully by many
researchers to demonstrate the normal pattern of twist, shortening, and
strain
distribution.16 26 27 29 37
Twisting in both patient types was noted to be markedly different from
normal at each slice level (Figs 3A
through 3C
). Regions of both
clockwise and counterclockwise twist were noted, with the abnormal
clockwise motion being most notable in the posterior wall of both
patient types and the inferior wall of Fontan patients. By
necessity, these regions must meet in an area of no twist, which we
call the transition zone. It is interesting that the regions of
clockwise twist (not found in the normal LV) were also the same regions
under the greatest strain in a given patient subtype (ie, the posterior
wall of S/P TGA patients at the atrioventricular valve level and the
posterior wall of Fontan patients at the apex). This abnormal twisting
may imply an altered orderly reciprocal emptying and filling of the
atrium and ventricle, possibly leading to inefficient energy use. This
altered systemic RV motion may be a consequence of geometry altering
foreign materials used to reconstruct the great vessels (affecting
blood flow and velocity profiles), the mechanics of baffle placement
within the atria affecting ventricular performance,
or complications of cardiopulmonary bypass and deep hypothermic
circulatory arrest.
Radial motion is also a measure of contraction and the ability of the heart to pump blood. It appears that depending on patient type, one wall moves paradoxically in systole (inferior wall in Fontan patients and the posterior wall in S/P TGA patients). Furthermore, radial contraction was not distributed uniformly around the short axis. At both the atrioventricular valve and the apex, regardless of whether the systemic RV had an LV attached, the superior wall underwent the largest radial inward motion. It is interesting that S/P TGA patients have their posterior wall (ie, septal wall) move paradoxically, as if the LV has not remodeled its fibers to convert from a systemic to a pulmonary pumping chamber. It is also interesting to note that the superior wall, which performed the greatest radial contraction in systemic RVs, also had the greatest counterclockwise twist, which implies that twist is coupled with shortening, consistent with published LV data.17
This difference from the normal motion of the LV myocardium
(Fig 3C
; data from our laboratory) may be due to remodeling of
fiber
angles, extra cardiac tethering of the ventricle, altered electrical
activation sequences, or ischemia of various muscle regions.
The altered twist may represent the lowest possible energy
state for the ventricle as a whole to assume.
It is interesting to hypothesize that the shortening rate for S/P TGA patients at the atrioventricular valve level was significantly different from the shortening rate at the apical short-axis level and from that for Fontan patients because the degree of paradoxical regional wall motion was greater for S/P TGA patients at the septal (posterior) wall than for Fontan patients at the inferior wall at that level (rate for S/P TGA is almost twice that for Fontan). At the apical level, the degrees of paradoxical regional wall motion were approximately equal. It is even more interesting to note that although strain was significantly greater in the S/P TGA group at the apical short axis, this difference was not translated into shortening rate because it was not statistically significant between the two groups at that short-axis level.
Comparison With Previous Studies of Normal LV Twist
Previous
studies have suggested that the normal and hypertrophied
LVs do not demonstrate the same twist and radial motion characteristics
that we have observed in both of our patient subtypes. Maier et
al27 found in both control and hypertrophic
cardiomyopathy groups a clockwise rotation at the
base (5.0±2.4° and 5.0±2.5°, respectively) and a
counterclockwise
rotation at the apex (-9.6±2.9° and
-7.3±5.2°, respectively).
These authors failed to track motion throughout systole. Although
Ingels et al,25 Arts et al,21 24 and
Chadwick20 did not describe the direction of twist in
either clockwise or counterclockwise directions in humans and intact
dog, they noted that the apical segment rotated in an opposite
direction to the basal segment, ie, there was a wringing motion of the
LV during contraction. Hansen et al23 found that this
torsion between basal and apical segments was decreased during
allograft rejection and myocyte necrosis and normalized once the
rejection episode was successfully treated. Beyer and
Sideman19 noted that LV twist and strain were coupled, and
later, Beyer et al17 noted that twist and shortening also
were coupled; however, the direction of twist was not defined.
Other
investigators have found that rotation was consistently
counterclockwise. Buchalter et al26 separated endocardium
from epicardium and found that both twisted counterclockwise, with
short-axis slices near the base twisting less than those near the apex
and endocardial twist>epicardial twist. These authors also failed to
track motion throughout systole. Hansen et al22 also found
that "counterclockwise twisting about the left
ventricular long axis (as viewed from apex to base)
accompanied ventricular ejection in all patients" with
implanted radiopaque markers (7.6° to 10.7° at the
midventricular level and 13.3° to 23.4° at the apical
level). Young et al29 confirms that twisting is
"anticlockwise." Researchers at our laboratory also believe this
to be the case28 (Fig 3C
).
The present
study of systemic RVs differs markedly from both views
of ventricular twist, strain, and shortening of the normal
LVs (Fig 3C
). No studies of normal LVs describe
simultaneous counterclockwise and clockwise rotation in the
same short-axis plane or describe a transition zone. Systemic RVs were
found to twist the same way whether at apical or
atrioventricular valve (basal) short-axis levels,
similar to the findings of Buchalter et al26 (who found
the same twist at three short-axis levels). Furthermore, although Beyer
et al17 found a positive correlation between normal LV
systolic twist and radial shortening, our findings that a transition
zone of no twist is present with any one of three types of radial
motionnone, inward, or outward (paradoxical)show that single
ventricles uncouple the twistshortening relation. We did note,
however, that superior walls of systemic RVs, which have the greatest
counterclockwise motion, also have the greatest radial contraction.
Study Limitations
Because magnetic resonance imaging measures
fixed planes in space,
through-plane motion of the heart may add artifactual deformation, as
Moore et al46 pointed out. It should be noted that they
described a type of tagging that is different from ours (radial versus
orthogonal grid) and compare three-dimensional strains with
two-dimensional strains. However, they observed that axial strains in
the radial and circumferential dimensions are fairly close when
comparing corrected three-dimensional strain with uncorrected
two-dimensional strain (<.05 difference). Furthermore, in normal
subjects, Hoffman et al47 showed that twist and twist
reversal found when tracking through-plane motion are similar in
direction and actually enhanced in magnitude from those images that do
not track the through-plane motion. Because the present study deals
with thick slices relative to the amount of through-plane motion, this
is not believed to have an appreciable affect on the findings.
No data are available concerning normal RV twist and radial motion or normal pediatric LV mechanics. Even if these data were available, they might not add more information than a comparison to the normal LV since the normal RV pumps blood against pulmonary vascular resistance. Nevertheless, a comparison would strengthen our study results.
Ages and time from operation for S/P TGA and Fontan patients are significantly different. Because the S/P TGA repair is rarely done today and magnetic resonance imaging was unavailable years ago, patients matched for age and time from operation are hard to find. The present study provides preliminary observations, and we intend to follow these two groups of patients. Although quantitative changes may occur in Fontan patients as they grow, it is unlikely that the fundamental differences in regional strain, twist, and radial motion we have observed between S/P TGA patients, Fontan patients and subjects with a normal LV will change with time.
Finally, because we have no data regarding the compliance of the lungs of these patients during tidal breathing occurring during the scanning, we cannot fully determine the effect this could have on our observations.
Conclusions
V-V interaction, which has been known to occur in
the normal human
heart, plays a measurable role in the systemic RV. Regional wall motion
and strain may play an important role in the long-term energetics of
the heart and may be an important factor in the mechanics of
ventricular pressure generation. Results from the
present study suggest that regional strain, twist, and radial
motion are markedly different in the systemic RV, depending on whether
an LV is present to augment ventricular function, and
differ significantly from those of the normal human LV. Areas of
clockwise, counterclockwise, and no twist (transitional zone) occur,
and these regions differ between Fontan and S/P TGA patients. Radial
shortening was not uniformly distributed around the myocardial wall,
with some regions having a greater radial motion (ie, doing more work)
than others and some regions moving paradoxically during systole.
The present study of V-V interaction coupled with our previous observations14 15 of altered regional strain across surgical subgroups of the Fontan procedure lays the groundwork from which surgical outcomes may be evaluated in the future.
| Acknowledgments |
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Received October 10, 1994; revision received January 9, 1995; accepted January 17, 1995.
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