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1Department of Cardiothoracic Surgery, Stanford University School of Medicine, Stanford; 2Department of Medicine, University of California San Diego, La Jolla; and 3Laboratory of Cardiovascular Physiology and Biophysics, Research Institute of the Palo Alto Medical Foundation, Palo Alto, California; and 4Department of Biomedical Engineering, Texas A&M University, College Station, Texas
Submitted 9 August 2004 ; accepted in final form 10 November 2004
| ABSTRACT |
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) were measured and averaged. Mean fiber angles progressed nearly linearly from 41° (SD 11) at the epicardium to +42° (SD 16) at the endocardium. Two families of sheets were identified at approximately +45° (
+) and 45° (
). In the lateral region (n = 5), near the epicardium, sheets belonged to the
+ family; in the midwall, to the
family; and near the endocardium, to the
+ family. This pattern was reversed in the basal anterior region (n = 4). Sheets were uniformly
over the anterior papillary muscle (n = 2). These direct measurements of sheet angles reveal, for the first time, alternating transmural families of predominant sheet angles. This may have important implications in understanding wall mechanics in the normal and the failing heart.
cardiac microstructure; sheets
The three-dimensional geometry of fibers and sheets is critical. Maximum contraction of fibers that lie in planes tangent to the epicardial surface is only 15% along their long axis (21); yet LV ejection fractions of 60% and systolic radial wall thickening of 40% are typically observed. The helical arrangement of the fibers may account for some of this disparity (20), but an additional important mechanism appears to be sheet deformation (19, 22). Laminar shear, extension, and thinning or thickening are thought to contribute to wall thickness changes (6, 7, 24).
Fiber orientation, which can be measured directly, has been found in several species to vary from approximately 60° at the epicardium to +60° at the endocardium (4, 10, 12, 14, 23, 28). Until recently, however, sheet orientation could only be inferred indirectly from the directions of fiber and cleavage planes from three orthogonal views (6). Recently, our group and Ashikaga et al. (2) employed a method (developed by J. C. Criscione) to measure directly sheet orientations across the LV wall. Studying the anterior wall of the canine heart, Ashikaga et al. found a relatively uniform transmural distribution of negative sheet angles (
). The present work, studying the anterolateral region of the ovine heart, revealed a hitherto unknown alternating transmural angular distribution of two separate sheet families. The presence of these families provides a new interpretation of myocardial mechanics.
| MATERIALS AND METHODS |
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Surgical preparation. Ten adult, Dorsett-hybrid, male sheep [68 kg (SD 7)] were intubated and ventilated (Servo Anesthesia Ventilator, Siemens-Elema, Stockholm, Sweden), and general anesthesia was maintained with inhalational isoflurane (12.2%). The heart was exposed via a left fifth intercostal space thoracotomy and suspended in a pericardial cradle. A micromanometer-tipped catheter (model SPC-500, Millar Instruments, Houston, TX), zeroed in a 37°C water bath, was placed in the ventricle through the apex to measure LV pressure. End-diastolic pressure was defined at the time immediately preceding the upstroke of the LV pressure curve. An intravenous bolus of thiopental sodium (1 g) was given, and the heart was depolarized and arrested at end diastole with an intravenous bolus of potassium chloride (80 meq).
LV pressure was adjusted to match in vivo LV end-diastolic pressure by venous exsanguinations (volume infusion was never required) and was maintained constant throughout the in situ fixation process. An 8-F coronary guiding catheter (PowerGlide, Advanced Cardiovascular Systems, Temecula, CA) was then advanced into the left main coronary artery under fluoroscopic guidance over a 0.014-in. floppy guide wire (HI-TORQUE, Advanced Cardiovascular Systems, Santa Clara, CA) through a sheath placed in the carotid artery. A conventional 3.0-mm perfusion balloon dilatation catheter was advanced into the proximal circumflex coronary artery through the guiding catheter. The balloon was inflated to prevent retrograde flow, and 300 ml of buffered glutaraldehyde (5%) were infused to fix the circumflex coronary artery distribution. Immediately thereafter, the balloon catheter was repositioned into the proximal left anterior descending coronary artery, and an additional 300 ml of buffered glutaraldehyde were infused to fix the left anterior descending coronary artery distribution. The hearts were then excised and stored in 10% formalin for later histological examination.
Histological preparation. To avoid the distortional effects of dehydration and shrinkage associated with embedding, histological measurements were obtained with freshly fixed heart tissue.
To define the myocardial geometry, a right-handed "cardiac" Cartesian coordinate system was defined with positive X1 (circumferential) pointing toward the posterior LV, positive X2 (longitudinal) pointing toward the LV base, and positive X3 (radial) pointing from endocardium to epicardium (Fig. 1) (26). X3 was defined normal to the epicardial tangent plane at the centroid (origin) of the equatorial wall tissue block to be studied. X2 was defined by the intersection of this epicardial tangent plane with a plane containing X3 and a line from the apex of the heart through the centroid. X1 was defined mutually perpendicular to X2 and X3.
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10 mm) was then carefully removed from the lateral equatorial wall, with edges of the block cut parallel to the local X1, X2, and X3 axes (Fig. 1, A and B). To examine some nearby regions, tissue blocks from five additional hearts were similarly analyzed, four blocks from the midanterior free wall and two from the region directly overlying the base of the anterior papillary muscle.
With a Plexiglas template to guide the blade, each block of tissue was sliced into 1-mm-thick sections parallel to the (X1,X2) plane, providing a series of slices from epicardium to endocardium for measurement of fiber angle (
) across the wall. The
was defined as the angle subtended by Xf and X1, with
being negative for a left-handed helix (Fig. 1B) (16, 23). To maintain the orientation of the coordinate system for all subsequent measurements, each slice was affixed (with cyanoacrylate) to note cards, with positive X1 pointing to the right, positive X2 pointing up, and positive X3 facing away from the paper (Fig. 2A). Digital photomicrographs of each section were taken (Nikon 4500 Coolpix, Nikon, Melville, NY). The angle between the local myofiber axis and the circumferential edge of the tissue section was measured at five sites on each image using image-processing software (SPOT Advanced version 3.5.6, Diagnostic Instruments, Sterling Heights, MI), and mean
was calculated at each transmural depth. Positive X1 defined 0°, with negative
defined as clockwise rotation about X3 (Fig. 1C).
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1 mm were then made along the cross-fiber (Xcf) axis, i.e., normal to the fiber (Xf) axis (Fig. 2A). The resulting blocks of myocardial tissue were rotated 90° about Xcf, so that Xf pointed out of the page (i.e., fibers now viewed "end-on") and the sheet (Xs) axis lay in the plane of observation (Fig. 2B). This allowed direct measurement of
at each transmural depth. To avoid distortions due to dehydration, the samples were kept moist with a 30% sucrose solution, which also served as a cryoprotectant to minimize freezing artifact during the subsequent frozen section process.
The rotated cross-fiber blocks were placed in 15 x 15 x 5-mm plastic molds (Tissue-Tek, Cryomold Intermediate, Miles, Elkhart, IN), embedded in OCT compound (Tissue-Tek, Sakura Finetek, Torrance, CA), and frozen over dry ice. Care was taken to preserve the coordinate orientations, and the specimens were stored in an 80°C freezer. The specimens were then cut into 8- to 10-µm-thick sections using a cryostat (Jung Frigocut 2800 N, Leica) and carefully transferred to a glass slide. During the sectioning process, a predominant
could be appreciated visually on each frozen specimen mounted on the cryostat. Once transferred to the glass slide, the specimens were imaged immediately with use of a digital camera (RT Color, x1 HRD 100-NIK, Diagnostic Instruments) mounted on a light microscope (type 301-371.010, Leica) at low-power (x25) magnification (Fig. 2C). Myolaminae coursing in the direction noted during sectioning of the frozen specimen were then observed. Over a 3-min period, gaps appeared between the myolaminae, defining the cleavage planes, and additional cracks and dehydration artifact appeared as the section dried. For each slice, angles representative of predominant sheet population(s) were defined as the first gaps to appear between the myolaminae as the section dried, corresponding to the predominant angles observed grossly in the frozen specimen. Values of
were determined from the cleavage planes that extended the majority of the width of the 1-mm section to minimize the likelihood of measuring dehydration artifact. Occasionally, two different sheet families were observed in a single section. Image-processing software was used to measure five angles representative of the predominant sheet orientation(s) over the length of the specimen, and the mean
was calculated for each transmural depth. The
was defined as the angle subtended by Xs and X3, with
being negative if the sheet moves away from the LV base as one follows the sheet radially toward the epicardium (Figs. 1C and 2C) (6). Values are means (SD).
| RESULTS |
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values ranged roughly linearly from 41° (SD 11) to 42° (SD 16) from epicardium to endocardium, being circumferentially oriented at the midwall level (Fig. 3A).
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values tended to fall into two different families or populations:
+, clustered around +45°, and
, clustered around 45° (Fig. 4). In the lateral equatorial wall, near the epicardium, the sheets belonged to the
+ family [+31° (SD 9)], in the midwall to the
family [41° (SD 15)], and near the endocardium to the
+ family [+54° (SD 11); Fig. 3B]. In 5 of the 37 slices, mostly at transition layers between the subepicardium and midwall and between the midwall and subendocardium, two predominant
values from the
+ and
families,
7090° apart, were observed within the same section. In the anterior basal region, the opposite trend occurred. Near the epicardium the sheets belonged to the
family [47° (SD 6)], in the midwall to the
+ family [+44° (SD 8)] and near the endocardium to the
family [43° (SD 4)]. In blocks from the region over the anterior papillary muscle, there was no alternating distribution; rather, sheets belonged to the
family throughout the entire wall depth [44° (SD 4)].
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| DISCUSSION |
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is relatively straightforward in sections cut parallel to the circumferential-longitudinal (X1, X2) plane, because the myofibers run almost parallel to this plane, with an out-of-plane, or imbrication, angle of <10° (23). This transmural myofiber distribution has been described in many species, including humans (12), using histology (14, 18, 23, 28) or diffusion tensor magnetic resonance imaging (4, 10, 25). This helical myofiber orientation is relatively preserved among different species, ranging from approximately 60° to +60° from epicardium to endocardium, with circumferential fibers at midwall, although some studies have shown some variation from apex to base (6, 23, 24). The present study is the first to report transmural distribution of
in the ovine heart, but our data are consistent with these previously published reports from other species.
Measurement of
, however, is not nearly as straightforward. The Xs axis is defined as orthogonal to the Xf axis, and
is defined as the angle of rotation of Xs around Xf, with reference to the positive X3 axis (15, 16, 22) (Fig. 2B). This Xs axis lies in a plane skewed in relation to the cardiac coordinates. Therefore, previous studies have measured cleavage plane angles in two orthogonal planes tangent to the cardiac coordinates (X23 and X13) and
in the X12 plane, and these cleavage plane angles were mathematically transformed to correspond to those in the plane in which the Xs axis (Xcf-3) lies (1, 6, 17, 24). Therefore, indirect
measurements using such mathematical transformations must assume a continuous distribution of a predominant sheet family from the measurement plane (X2,X3 or X1,X3) to the extrapolated (Xcf,X3) plane.
Previous indirect measurements in canine hearts, mostly from the anterior wall, have shown a consistently negative
(approximately 30° to 40°) through the wall depth, (2, 5, 6, 17, 24) or a progression from negative to positive
or vice versa (within 90° and +90°) across the heart wall (6, 15, 16). These transmural patterns also vary substantially from apex to base (6, 16, 24) and in different regions of the LV (16, 17). Two of these studies (15, 17) noted areas containing sheets with markedly different orientations, implying two coexisting sets of intersecting sheets at these locations. Ashikaga et al. (2), using the direct measurement method similar to that reported here, demonstrated one sheet population, which was consistently negative, running throughout the wall, with a second population, lying approximately perpendicular to the first, occurring simultaneously in the subendocardium of the canine anterior LV wall.
The present study, applying this direct measurement approach to the ovine lateral equatorial LV wall, demonstrated
falling into two distinct families (Fig. 4):
+ clustered around +45° and
clustered around 45°. Although this is consistent with previous reports of two families of
(1, 2), it differs from previous reports, in that the orientation of a specific sheet population was found to depend on transmural depth. In the lateral wall, near the epicardium,
belonged to the
+ family; near the midwall, to the
family; and near the endocardium, again to the
+ family (Fig. 3B). In the anterior wall the reverse trend was observed. Near the epicardium,
belonged to the
family; near the midwall, to the
+ family; and near the endocardium, again to the
family. In the anterolateral region, overlying the anterior papillary muscle, a homogenous distribution was found, with
consistently belonging to the
family throughout the wall. Figure 5 presents a conceptual schematic model depicting how the results observed in these three regions could be synthesized into a more global picture of the cardiac microstructure.
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Our transmural sheet characterization provides additional insights into these models of wall thickening. Figure 6 demonstrates a two-dimensional representation of how previously described mechanisms of laminar deformation, when combined with our lateral transmural distribution of alternating families, could create an "accordion-like" wall thickening mechanism. Indeed, a heterogeneous transmural laminar structure, such as the accordion configuration observed in the present study, may facilitate wall thickening via laminar shear in the cylindrical ventricle. If only one population of sheets existed throughout the wall from epicardium to endocardium, thickening due to laminar shear would only be possible if the endocardium moved parallel to the epicardium as much as they move away from each other; i.e., thickening and shearlike translocation would have to be on the same order. Conversely, an accordion laminar distribution allows alternating shear displacement to occur within the wall, such that minimal shear displacement of the epicardium relative to the endocardium can occur. With this mechanism, the shear deformation can be the same throughout the wall, but the direction of sheet sliding alternates. The reverse-accordion distribution observed in the basal anterior region would operate in a similar fashion. This mechanism would not be available in the region over the anterior papillary muscle, however, in which we found a homogenous transmural sheet distribution. Interestingly, this region has been shown to have depressed wall thickening relative to the adjacent anterior free wall (13).
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In summary, this study directly measured
throughout the anterolateral ovine LV wall. Using this method, we demonstrated two families of
approximately perpendicular to each other, the orientation of which was a function of transmural depth. This heterogeneous transmural microstructure, characterized by discrete, alternating families of sheets, with opposite alternating sign patterns in the lateral and anterior regions, may provide new insight into LV wall thickening mechanisms. The importance of laminar transverse shear, thinning or thickening, and extension on wall thickening has previously been known, yet precisely quantifying global myolaminar architecture has remained elusive. This study is a step toward precise characterization of the distribution of sheets throughout many regions of the LV, which is crucial to a full understanding of the structure-function relation of the heart in physiological and pathological states.
Study limitations.
This analysis assumes an average
for each 1-mm slice, a method that has been used in previous studies (6, 17, 24). In the present study, there was a <10° variation in the five angles measured for a given population within a slice. In the slices where we measured all possible angles (including possible dehydration artifacts), there was greater dispersion. Although it is likely that such dispersion of
could significantly affect local sheet mechanics, we chose to average the predominant
for each slice, assuming that the predominant orientation would have the major effect on LV wall thickening.
Because
values were measured in frozen sections, it is possible that
may have become altered during the freezing and dehydration processes. All samples were soaked in 30% sucrose to minimize the freezing artifact. To minimize dehydration artifact, samples were photographed immediately after sectioning, and care was taken to match the measured angles to the observed predominant trend in the frozen tissue block.
Our observations are limited only to the equatorial and basal anterolateral ovine LV wall. The results of the present study encourage a thorough and systematic study of the entire LV, but this is beyond the scope of the present study. Variation in sheet distribution has been shown from apex to base (6, 16, 24), and it is possible that there is variation among different species as well. The site and species variation may account for the differences in the magnitudes and signs of
reported from previous experiments, which have largely focused on the basal and apical anterior LV walls of canine hearts. Therefore, caution is necessary in extrapolating these results to other regions and other species, including humans.
We have provided no functional data to support our accordion-like wall-thickening mechanism and acknowledge that many different possible heterogeneous distributions can create local shearing and wall thickening without requiring a concomitant large shear displacement of the epicardium relative to the endocardium. The blocks of tissue from the anterior and lateral walls were taken directly contiguous to transmural bead sets implanted in vivo for the purpose of strain analysis, and we plan further studies using data from these bead sets to more concretely test this proposed transmural wall-thickening mechanism.
| GRANTS |
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Present addresses: H. Ashikaga, University of California, San Diego, BSB 2004, 9500 Gilman Dr. 0613J, La Jolla, CA 92093; J. C. Criscione, Dept. of Biomedical Engineering, Texas A & M University, 3120 TAMU, College Station, TX 77843-3120.
| ACKNOWLEDGMENTS |
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This study was presented in part at the American Heart Association, Western States Affiliate, Young Investigator's Forum, 2003, San Francisco, CA.
| FOOTNOTES |
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The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
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