STATE-OF-THE-ART PAPER
Left Ventricular Structure and Function
Basic Science for Cardiac Imaging
Partho P. Sengupta, MBBS, MD, DM*,
Josef Korinek, MD*,
Marek Belohlavek, MD, PhD, FACC, FESC*,
Jagat Narula, MBBS, MD, DM, PhD, FACC, FAHA
,
Mani A. Vannan, MBBS, FACC
,
Arshad Jahangir, MD, FACC* and
Bijoy K. Khandheria, MD, FESC, FASE, FACC
,*
* Division of Cardiovascular Diseases, Mayo Clinic, Rochester, Minnesota
Division of Cardiology, University of California at Irvine, Irvine, California
Division of Cardiovascular Diseases, Mayo Clinic, Scottsdale, Arizona.
Manuscript received June 1, 2006;
revised manuscript received August 29, 2006,
accepted August 30, 2006.
* Reprint requests and correspondence: Dr. Bijoy K. Khandheria, Division of Cardiovascular Diseases, Mayo Clinic, 13400 East Shea Boulevard, Scottsdale, Arizona 85259. (Email: khandheria{at}mayo.edu).
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Abstract
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The myofiber geometry of the left ventricle (LV) changes gradually from a right-handed helix in the subendocardium to a left-handed helix in the subepicardium. In this review, we associate the LV myofiber architecture with emerging concepts of the electromechanical sequence in a beating heart. We discuss: 1) the morphogenesis and anatomical arrangement of muscle fibers in the adult LV; 2) the sequence of depolarization and repolarization; 3) the physiological inhomogeneity of transmural myocardial mechanics and the apex-to-base sequence of longitudinal and circumferential deformation; 4) the sequence of LV rotation; and 5) the link between LV deformation and the intracavitary flow direction observed during each phase of the cardiac cycle. Integrating the LV structure with electrical activation and motion sequences observed in vivo provides an understanding about the spatiotemporal sequence of regional myocardial performance that is essential for noninvasive cardiac imaging.
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Abbreviations and Acronyms
| | IVC = isovolumic contraction | | IVR = isovolumic relaxation | | LV = left ventricle/ventricular | | MRI = magnetic resonance imaging |
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Heart failure is a growing problem worldwide (1). Almost 5 million Americans have heart failure, and a further 550,000 are diagnosed with heart failure annually (2). The current biological models used for understanding the syndrome of heart failure are insufficient in explaining the benefits of several newer emerging therapies (3). These limitations may result from inaccuracies in modeling the structure and physiology of the left ventricle (LV), which becomes maladaptive and disorganized. A report from a recent National Institutes of Health meeting drew attention to the existing gaps in the understanding of the normal structure and function of a beating heart (4). In particular, the regional inhomogeneity of mechanical shortening and lengthening sequences in the LV wall, which result in a highly efficient global function of the normal heart, despite presence of structural anisotropy, remain contentious and incompletely characterized (58).
Normal ventricular function requires coordinated electrical activation and contraction. Given the 3-dimensional pattern of ventricular activation and contraction, the assessment of mechanical activation using conventional imaging methods is a complex task. Although electrical depolarization follows an anatomically predefined sequence in healthy individuals, physiological mechanical activity is characterized by a higher degree of nonuniformity (9). The impact of cardiac resynchronization therapy on global systolic and diastolic performance in dyssynchronous hearts particularly has renewed an interest in understanding the physiological nonuniformities of regional LV performance (10,11). Because QRS duration alone fails to predict reverse remodeling, imaging techniques with high temporal resolution have been actively sought for more accurate characterization of regional LV deformation (10,11). Simultaneous integration of LV muscle fiber geometry and function at a regional level with global sequence of cardiac deformation in different phases of the cardiac cycle remains an area of intense investigation.
In this review, we first summarize the parameters that are required for describing LV geometry and deformation. Further, we describe the emerging concepts regarding the sequence of electromechanical activation and LV intracavitary flow within the anatomical context of the helical myofiber arrangement of the LV wall.
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Left ventricular geometry
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Normal LV geometry has been conceptualized as a prolate ellipsoid shape (12) with its long-axis directed from apex to base. Therefore, short-axis cross sections of the LV should reveal a circular geometry. However, because of a curved posterolateral wall and a flat anterior wall (13), the short-axis cross sections obtained by cardiac imaging techniques do not appear circular. In addition, the endocardial surface is extremely irregular because of the presence of papillary muscles and trabeculae (12). Significant nonuniformities also exist in the LV wall, particularly with regard to the thickness. The posterolateral wall is significantly thicker than the septum. A gradual thinning of the LV wall is observed toward the apical segments (13).
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Quantitative terms in LV mechanics
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During a cardiac cycle, the LV wall shortens, thickens, and twists along the long axis. Shortening and thickening can be quantified by measuring regional strain. Strain or myocardial deformation from developing forces is expressed as either the fractional or the percent change from the original dimension (14). Positive radial strains represent wall thickening (radial deformation), whereas negative strains represent segment shortening (e.g., circumferential shortening, longitudinal shortening, and fiber shortening). These strains can be expressed either in a local cardiac coordinate system or a local fiber coordinate system (13). Three perpendicular axes orienting the global geometry of the LV define the local cardiac coordinate system: radial, circumferential, and longitudinal. The local fiber coordinate system is defined by the following: 1) the radial axis similar to the local cardiac coordinate system, 2) the fiber axis tangent to the surface and parallel to the local fiber orientation, and 3) the cross-fiber axis, tangent to the surface and perpendicular to the fiber.
Echocardiographic techniques like tissue Doppler imaging have excellent temporal resolution (<4 ms) and provide the instantaneous velocity of myocardial motion. The velocity data can be postprocessed for calculating parameters such as displacement, strain rate, and strain. Numerical integration of velocity over time results in displacement curves. Strain rate, which is the rate of change of deformation, is derived as a spatial derivative of velocity, whereas temporal integration of strain rate is used for calculating regional strain (14).
Left ventricular rotation, twist, and torsion are terms often used interchangeably in published reports for explaining the wringing motion of the LV. For this review, the term "rotation" will refer to the rotation of a short-axis sections of LV as viewed from the apical end and defined as the angle between radial lines connecting the center of mass of that specific cross-sectional plain to a specific point in the myocardial wall at end diastole and at any other time during systole (15). The unit of rotation is degrees or radians. The base and apex of the LV rotate in opposite directions. Twist defines the base to apex gradient in the rotation angle along the longitudinal axis of the LV and is expressed in degrees per centimeter or radians per meter (16). Torsion and twist are equivalent terms. Torsion also can be expressed as the axial gradient in the rotation angle multiplied by the average of the outer radii in apical and basal cross-sectional planes, thereby representing the shear deformation angle on the epicardial surface (unit degrees or radians) (17). This normalization can be used as a method for comparing torsion for different sizes of LV. When the apex-to-base difference in LV rotation is not normalized, the absolute difference (also in degrees or radians) is stated as the net LV twist angle (16).
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Developmental changes
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The heart increases in size by 2 orders of magnitude during development but, unlike the mature heart, the embryonic heart grows by hyperplasia (18). The helical arrangement of myofibers is evident at a very early stage of cardiac development and can be accelerated or delayed by manipulating the loading conditions (19). At the stage of an embryo, the primitive tubular heart develops from two layers of epithelial cells (20) (Fig. 1). The inner layer proliferates and grows toward the ventricular cavity as sheets and chords that develop into trabeculae. Cells in the outer layer proliferate and undergo progressive compaction in response to the functional needs of a growing embryo. The early embryonic heart responds to changes in its mechanical environment. Pressure overload, for example, leads to increased thickness of the trabeculae and to precocious spiraling of the trabecular architecture (18,20).

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Figure 1 Embryonic development of the left ventricular wall in a chick. (A) The tubular myocardium (My) (2 to 3 cell layers thick) is separated from the endocardium (En) by acellular cardiac jelly (CJ). (B) The inner layers proliferate to form trabeculations (Tr), which are nourished by the blood circulating through the intertrabecular spaces (ITS). The outer layers proliferate and undergo compaction (Co) and are covered by epicardium (arrowhead). (C) By the sixth embryonic day, the compact layer has thickened and is invaded by developing coronaries from the epicardial surface. (D) In the neonatal (day 10) heart, the multilayered compact architecture of the left ventricular wall is clearly appreciated with the innermost layer merging with the papillary muscle (mp). On the right side of each picture is a schematic drawing illustrating the major steps in development of ventricular myoarchitecture. Scale bars = A, B, C, 100 µm; D, 500 µm. Reproduced from Sedmera et al. (20) with permission.
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The propulsion of blood flow in an embryonic tubular heart parallels an initial isotropic electrical activation sequence that spreads from the most caudal portion of the tubular heart toward the cranially located outflow (21). Using a model of embryonic zebrafish heart tube, it has recently been suggested that this blood propulsion is not because of peristalsis but the result of dynamic suction of the tubular heart (22). Soon after the initial contractions, the process of cardiac looping begins to transform the heart into a curved tube (18). During looping, the heart tube undergoes ventral bending and torsion to create the basic pattern of the mature heart (23). Formation of torsional component of the looping promotes a change from the propulsive movements of the tubular heart to the twisting pattern seen in adult life. Further maturation of the LV wall is accompanied with emergence of a specialized His-Purkinje conduction system that progressively alters the immature base-to-apex sequence of electromechanical activation into a mature apex-to-base pattern (21).
With regard to mechanical performance, an interesting feature of an early trabeculated heart is the pattern of ventricular filling. Filling of an early embryonic looped heart occurs predominantly in late diastole, primarily because of atrial contraction, and shifts into early diastole after the addition of outer ventricular layers (24). A good correlation is seen to exist between the thickness of outer compact myocardium and the suction performance of a developing heart. A mutant mouse model with underdeveloped outer layers of myocardium shows diastolic dysfunction with diminished suction gradient and reduced force development during ejection (24). Thus, the progressive addition of outer compact spiral layers contributes to the efficient ejection and suction performance of the developing heart.
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Left ventricular architecture in adult life
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Early historic descriptions of the relation between myocardial structure and function were based on the belief that the heart comprised distinct muscle bundles that worked like skeletal muscles, with the long axis spiraling around the heart chambers (25,26). Subsequent descriptions of myocardial architecture have ranged from laminated sheets, layered fibers, and complex nested syncytium to a unique band-like arrangement (2531). Torrent-Guasp et al. (28,29) attracted major attention in recent years to their proposed model in which the continuum of myocardial architecture was depicted in the form of a muscle band that was spatially organized into 2 distinct helicoids. Although the model emphasized the importance of counter-directional helical anatomy in the LV, the embryological origin and existence of a unique band-like arrangement in the LV has been debated by other investigators (7,8,31).
The myocardial cells are single-nucleated and are themselves supported loosely within a continuous matrix of fibrous tissue. Groups of myocytes are surrounded by condensations of the endomysial weave, thus forming the perimysium, which aggregates a meshwork of myocytes into the so-called myofibers (31). The attachments between neighboring cells and matrix accommodates shearing between cardiac muscle fibers (32) and dynamic alterations in myocardial fiber direction during different phases of cardiac cycle (33).
Most studies have analyzed the architecture of the myocardium in transmural plugs of ventricular tissue that permit a detailed examination within a given region of myocardium (3436). Myofiber morphology has either been described based on orientation of individual fibers or as multiple myocyte "sheet" arrangements separated by extensive "sheet-cleavage" planes. For describing the global arrangement, most studies and computational models have depicted LV myocardial architecture as a transmural continuum between 2 helical fiber geometries, where right-handed helical geometry in the subendocardial region gradually changes into left-handed geometry in the subepicardial region (33,37,38) (Fig. 2). Mathematical models have shown that this counterdirectional helical arrangement of muscle fibers in the heart is energetically efficient and is important for equal redistribution of stresses and strain in the heart (37). Incidentally, a counterdirectional arrangement of muscle fibers in the LV mirrors the structural theme that exists for propulsion in other organ systems, such as the alimentary tract, in which smooth muscles in 2 opposite directions generate peristaltic waves (39). Similarly, biophysical studies in various animals have shown the use of synergistic though inversely oriented pairs of skeletal muscles for propulsion, locomotion, or flying (40). The counterdirectional arrangement of muscle fibers helps maintain stability and minimizes energy expenditure (40).

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Figure 2 Helical arrangement of muscle fibers in the left ventricle of an explanted adult porcine heart. The arrangement of muscle fibers as seen in the circumferential-longitudinal plane changes from a left-handed helix in the subepicardium (A) to a right-handed helix in the subendocardium (B). The helical arrangement of the endocardial region is also reflected in the arrangement of trabeculae near the apex (C). A = anterior; P = posterior.
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For quantification of fiber orientation, the helix and transverse angles were introduced by Streeter et al. (27). The helix angle represents the angle between the circumferential axis and the projection of the myofiber onto the circumferential-longitudinal plane. The myofiber helix angle changes continuously from the subendocardium to the subepicardium, from a right- to a left-handed helix (Fig. 2), typically ranging from +60° at the subendocardium to 60° at the subepicardium (41). The tranverse angle represents the angle between the circumferential axis and the projection of myofiber orientation onto the radial-circumferential plane (41) and ranges between 20° to +20° (33). Le Grice et al. (42) found that collagen binds adjacent myocytes together forming layers known as lamina or sheets, which typically are 4 cells thick and separated by cleavage planes. On the basis of this finding, other investigators incorporated the helix angle (
) and the sheet angles in longitudinal radial plane (ß') and circumferential radial plane (ß'') in descriptions of the myofiber and sheet arrangements (43).
Figure 3
shows the arrangement of sheets and cleavage plane in the longitudinal cross-sectional plane (ß'). A radial arrangement of fiber sheets and cleavage planes produces a distinct layered appearance (33). Figure 4
shows the arrangement of fiber sheets and cleavage plane in a radial cross-sectional plane (ß'') taken through the mid LV and viewed from the LV base. The cross sections of the sheets within the short-axis sections diverge from the midwall. Such a characteristic appearance of myofiber arrangement can also be identified in the human LV when viewed in its short axis and was first described by Greenbaum et al. (44) and recently also reviewed by Anderson et al. (31,45). These transmural differences in orientation of muscle fibers and cleavage planes within the myocardial wall can be appreciated noninvasively using diffusion tensor magnetic resonance imaging (MRI) (Fig. 5) (46) and high-resolution ultrasonography ( and . [see ]). When a high-resolution ultrasound transducer is moved over an explanted porcine heart specimen from the apex toward the base, the panning cross-sectional view as seen from the basal end of the LV shows an outer clockwise and inner counterclockwise movement of speckles due to the counterdirectional arrangement of the fiber sheets in the subendocardial and the subepicardial regions ( [see ]). The predominant left-handed helical arrangement of myofibers at the LV apex can be identified by cardiac ultrasound even in a beating heart ( [see ]).

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Figure 3 Arrangement of left ventricular fiber sheets and cleavage planes in long-axis slices. (A) Longitudinal cross section of the left ventricle fixed in diastole (hematoxylin and eosin stain). (B) Radial orientation of the cleavage planes and the quantification of diastolic and systolic angles of the sheets and the cleavage planes from the boxed area in A. Reproduced from Chen et al. (33) with permission.
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Figure 4 Cross-sectional view of a rats left ventricle (LV) when viewed along the short axis. The cross section obtained from the midsegment of the interventricular septum has been viewed from the basal end of the LV. The fiber sheets (dashed arrows) are seen to diverge away from midwall (hematoxylin and eosin stain) (A). The cleavage planes (arrow) separating the myofiber sheets are distinctly appreciated using high-resolution confocal laser scanning micrograph (B) magnification. Scale bar in B = 200 µm. RV = right ventricle.
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Figure 5 Assessment of cardiac muscle fiber orientation by diffusion tensor magnetic resonance imaging. In these examples (A and B), scalar and tensor glyph visualization methods have been used to investigate the helical structure of the heart muscle in an explanted fixed canine heart. Right-handed helical orientation (subendocardium) is shown in shades of purple, and left-handed helical muscle fiber orientation (subepicardium) is shown in shades of blue. The cross-sectional view (B) has been viewed from the basal end of the left ventricle. Reproduced from Zhukov and Barr (46) with permission. LV = left ventricle; RV = right ventricle.
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Electrical sequence in the adult heart
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The fascicles of the His-Purkinje system are insulated from the surrounding muscle during their course from the crest of the septum toward the ventricular apex (21). The LV myocardial wall is, therefore, first activated at the LV endocardium in septal and anterior free wall regions, close to the LV apical endocardium (47). From these exits of the Purkinje system, the LV activation sequence travels from apex to base with small differences in activation between the septum and LV free wall (47). Pacing from the LV apex has been shown to provide a more physiologic sequence of activation and LV function than that produced with right ventricular or LV free wall stimulation (48,49).
Although electrical gradients produced by the matching sequence of ventricular depolarization results in QRS complex on surface ECG, the gradients underlying repolarization has been widely debated. Roughly, 3 types of repolarization inhomogeneities play a role: 1) differences between the right and left ventricle; 2) differences between apex-base and anterior-posterior; and 3) transmural differences (50). In previous investigations, the presence of a repolarization gradient between the "mid-myocardial region" (M-cells) and subendocardial and subepicardial regions has been correlated with the genesis of upright T waves in ventricular wedge preparations (51). However, studies of intact hearts have failed to provide evidence for transmural differences in repolarization (52). Thus the genesis of T wave on surface electrocardiogram (ECG) may be largely due to the base-to-apex gradient with minimum contribution from the transmural gradient (50,53).
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Mechanical sequence of an adult heart
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Isovolumic contraction.
Cardiac isovolumic phases are characterized by transient changes in LV shape that produce rapid variations in regional velocities. Rushmer (54) had shown that LV geometric changes during the initial phases of systole were not isometric but were characterized by abrupt expansion of the external circumference. An advent of tissue Doppler imaging further facilitated quantification of rapid variations in regional velocities (55) during isovolumic intervals. Both open-chest experimental animal models and human studies (5557) have reported a bidirectional movement of the LV wall during isovolumic contraction (IVC) ( [see ]). Recent investigations from our laboratory and by others have shown that the biphasic longitudinal myocardial velocities and strain rate waveforms are consistently seen during IVC on tissue Doppler imaging (5557) and result from a physiological asynchrony of shortening between the subendocardial and subepicardial regions (57,58).
In earlier descriptions of myocardial band hypothesis, Torrent-Guasp et al. (29) proposed that isometric contraction of the posterior basal epicardial region of the LV would result in a rigid external buttress, which could explain the inner bidirectional movement of the subendocardial region. However, recent investigations in the intact human heart have shown that electrical activation of the posterior basal epicardial region occurs around the down-sloping of the R wave or S wave on surface ECG (59). Mitral valve closure, on the other hand, occurs approximately at the peak of R wave (60,61), implying that mechanisms for closing the mitral valve are initiated within the LV even before the posterior basal epicardial region is electrically activated. Newer observations indicate that cardiac muscle activity during IVC is not isometric, and early shortening occurs within the subendocardial myofibers in the anterior wall of the LV (57,62). The shortening of the inner subendocardial fibers (right-handed helix) is accompanied with stretching of the outer subepicardial fibers (left-handed helix) (57). Stretching of activated cardiac muscle fibers produces rapid increase in myocardial stiffness (63,64). The "rigid external cylinder" of the basal epicardial loop as hypothesized by Torrent-Guasp et al. (29) may correspond to this early stiffening of the subepicardial fibers produced by transient stretching; however, this requires further confirmation in vivo. Shortening and stretching are reciprocal deformations that satisfy isovolumic mechanics, that is, shortening in one direction is accompanied with stretching of the orthogonal direction (57). Stretching of myofibers during IVC is also important in initiating "stretch activation response," an intrinsic length-sensing mechanism that allows muscle to adjust the force and duration of subsequent shortening (6567). This has recently been proposed as the main basis of the Frank-Starling mechanism of the heart (68). Stretching a myocyte that has been electrically activated increases the force of subsequent shortening due to strain of attached cross bridges and acceleration of cross-bridge cycling kinetics (69).
The papillary muscles are among the earliest portions of the ventricle that are electrically stimulated. However, during IVC, despite the electrical signal to contract, the papillary muscles also are stretched during IVC and early period of systole while other portions of the ventricle are contracting (62,67,70). This motion has been attributed to the increasing intraventricular pressure in early systole that leads to closure of the mitral valve leaflets with increasing tension on the chordae, which causes stretching of the papillary muscles (67,70).
Ejection phase.
Myocardial deformation during ejection demonstrates extensive transmural tethering (71) such that subendocardial and subepicardial regions undergo simultaneous shortening along the fiber and cross-fiber direction during ejection (57,72). Subendocardial strains are higher in magnitude than subepicardial strains (Fig. 6) (53). Within subendocardium, the magnitude of circumferential strains during ejection exceeds that of longitudinal strains (13) (Figs. 6 and 7).
With regard to the timing, longitudinal shortening strains for both regions show an apex-to-base gradient, so that successive shortenings are reached earlier at apex and midsegments compared to the LV base (57,72). Thus, the direction of LV mechanical shortening parallels the apex-to-base direction of electrical activation (47). Studies of canine (73) and childrens (48) hearts also have shown that an apex-to-base direction of LV pacing yields a more physiologic sequence of activation and LV function.

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Figure 6 Longitudinal deformation of the anterior wall of the left ventricle by 2-dimensional speckle tracking of B-mode ultrasound images (2-dimensional strain). Longitudinal shortening starts during isovolumic contraction period and occurs earlier in the apex as compared with the base. Shortening-lengthening crossover of the basal anteroseptal segment is delayed until the end of isovolumic relaxation. Phase 1, isovolumic contraction; 2, ejection; 3, isovolumic relaxation; 4, early diastole; 5, late diastole. ECG = electrocardiogram.
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Figure 7 Circumferential deformation of the subendocardial and subepicardial regions of left ventricular apex by 2-dimensional speckle tracking of B-mode ultrasound images (2-dimensional strain). Note the presence of positive strains (lengthening) during the phase of isovolumic contraction. Note the higher circumferential strains of the subendocardial regions as compared with the subepicardial region. Peak shortening in some segments of the subepicardial region extends beyond the timing of aortic valve closure (postsystolic shortening, arrow). Phases 1 to 5 are described in the legend to Figure 6. ECG = electrocardiogram.
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Previous tissue Doppler image analyses in the apex-to-base direction reported a velocity gradient but nearly uniform strain and strain-rate gradients. Recent investigations using either direct sonomicrometry (53) or indirect measurement by MRI tagging (13) have reported higher shortening strains within the LV apex. Results of Doppler strain measurements are dependent on the angle between the scan axis and tissue and may have inherent limitations in accurately measuring deformation from curved regions of LV, particularly near the apex. Measurements with a recently developed technique of measuring 2-dimenstional strains by speckle tracking of B-mode ultrasound images (74) also suggest that radial and longitudinal strains and strain rates are higher in the apex compared to the base (Fig. 6, [see ]) (75,76).
Isovolumic relaxation and postsystolic shortening.
Two types of mechanical gradients operate during isovolumic relaxation (IVR): apex-to-base and transmural gradients (Figs. 6 and 7). Near the LV apex, shortening of the subepicardium (left-handed helix) continues beyond aortic valve closure and is accompanied with lengthening of the subendocardial layer (right-handed helix) (53,72). Near the LV base, lengthening of myocardial wall occurs along the left-handed helical subepicardial fiber direction and is accompanied with shortening and shear along the subendocardial fiber sheets (i.e., right-handed fibers) (36,53). Changes in LV cavity volume follow the deformation pattern of the subendocardium, with enlargement of the LV cavity at the apex.
Longitudinal and circumferential shortening of the myocardial wall during the IVR period has been reported in normal human subjects (77,78). Zwanenburg et al. (77) timed cardiac contraction in healthy subjects with high-temporal-resolution MRI myocardial tagging and reported that several segments in the lateral wall and in the basal regions contracted circumferentially beyond aortic valve closure (Fig. 8). The occurrence of longitudinal postsystolic shortening in healthy subjects was reported also by Voigt et al. (78). Postsystolic shortening as a physiological phenomenon may be explained on the basis of synergistic movements that occur during IVR, that is, lengthening of the LV segment in one direction is accompanied with shortening in the other direction. Recent observations in beating porcine hearts indicate that a component of this reciprocal shortening occurs circumferentially near the apex and is linked with longer repolarization intervals. Normal postsystolic contraction of the LV provides an apex-to-base and transmural gradient of deformation that may help in rapidly restoring the geometry of LV cavity in early diastole (53,72). Delayed force development is predominantly seen in regions that undergo prestretching during IVC, that is, stretch activation, and results from recruitment of additional cross bridges to sustain a state of prolonged force generation (69).

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Figure 8 Time sequence of circumferential shortening in a healthy subject by tagged magnetic resonance imaging. Several segments contract beyond aortic valve closure. + = measured data points; = fitted line model to data for estimating T
onset; circled + = end point of data used in the fit; upside-down triangles = estimated T
onset; triangles = T
peak. The vertical lines denote, from left to right, the moment of aortic valve opening (dashed), aortic valve closure (solid), and mitral valve opening (dashed). AL = anterolateral; AN = anterior; AS = antero-septal; IL = inferolateral; IN = inferior; IS = inferoseptal. Reproduced from Zwanenburg et al. (77) with permission.
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Coexistence of shortening and lengthening deformations within the LV wall during the isovolumic phases (57,58) makes "contraction" and "relaxation" terms misleading for defining the corresponding phases (IVC and IVR, respectively). Instead, the terms of "isovolumetric ventricular contraction" or "systolic ventricular filling" due to a muscular mechanism recently have been suggested (79). However, published reports are inconsistent with regard to the definition of "systole" and "diastole" (80). Even Wiggers, who originally defined the phases of cardiac cycle, found it most difficult to correlate end ejection with valve closure and to delineate exactly the moment when "systole" ceases and when relaxation of muscle and ventricle starts (80). He admitted that this intermediary interval belongs, strictly speaking, neither to the period of systole nor to that of diastole (80). To avoid this uncertainty, we propose using the term "pre- and postejection" isovolumic intervals for providing more succinct information because such definition can include existence of simultaneous myocardial shortening or lengthening within the LV wall.
Left ventricular thickening.
Continuum mechanics would suggest that continuity of wall materials is all that is required for LV wall thickening. Shortening in longitudinal and circumferential direction would result in thickeneing in the radial direction for conserving mass. However, LV wall thickening is not a resultant of simple shortening of individual myocytes in concert but an effect of shearing of groups of myocytes across each other ( [see ]). Transmural shearing results from sliding and rearrangement of myofiber sheets along cleavage planes during the cardiac cycle (33,42,81). Rademakers et al. (82) used MR myocardial tagging and showed that cross-fiber strain was near zero at the epicardium but was large at the endocardium and increased from base to apex. This study concluded that the primary source of myocardial wall thickening was the interaction between the different layers of the myocardium (82). The transmural variations in radial deformation depend upon the regional differences in activation and electromechanical coupling of myocardial layers. Anatomical M-mode echocardiography and Doppler can be used for timing the transmural differences in the onset and peaking of radial motion during different phases of cardiac cycle (Fig. 9).

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Figure 9 Direct in vivo imaging of anterior wall of a beating porcine left ventricle using high-resolution linear array transducer (10 MHz). (A) Anatomic M-mode imaging of the different layers of anterior segment of left ventricular apex at high temporal resolution (250 frames/s). During isovolumic contraction, the endocardium moves toward the cavity (blue arrows) and is accompanied with a reciprocal outward movement of the subepicardium (white arrows). A reverse pattern of movement is seen during isovolumic relaxation. These reciprocal movements of the subendocardial and subepicardial regions also are seen in tissue Doppler imaging, in the form of simultaneous red and blue colors within the inner and outer layers of the same segment of the myocardial wall during isovolumic contraction and vice versa during isovolumic relaxation (B). Phases 1 to 5 are described in the legend to Figure 6.
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Left ventricular twist.
In the past, dynamics of LV rotation were assessed by implanting multiple radioopaque markers and biplane cine angiography (83,84). Currently, LV twist can be assessed noninvasively by MRI and 2-dimensional echocardiography (85). Recently introduced 2-dimensional strain echocardiography allows rapid and accurate measurement of regional twist angles or rotation (86). Rotation is conventionally viewed from the apical end of the LV, with clockwise and counterclockwise rotations shown in negative and positive degrees respectively. During IVC, the LV apex shows brief clockwise rotation ( [see ]) (87,88). This is explained by the predominant mechanical activity that develops along the right-handed helical direction during IVC because of shortening of the subendocardial region (89). During ejection, the apical rotation reverses becoming counterclockwise and the direction corresponds with the orientation of the left-handed helical subepicardial myofibers. Beyar et al. (84) demonstrated for the first time in a canine model that a major component of untwisting (clockwise rotation) occurred during the IVR and early period of diastole. Subsequently, in another canine experimental study, it was shown that untwisting of LV apex was initiated within IVR following the first 20 ms of aortic valve closure and approximately 50% of untwisting occurred before mitral valve opening ( [see ]) (90).
Rotation of the LV base is opposite to that of the apex but is significantly lower in its magnitude. During IVC, there is a brief counter-clockwise rotation due to the mechanical activity of the subendocardial fibers, which is followed by clockwise rotation (twist) during ejection when the subepicardal myofibers dominate the direction of LV rotation. The counterdirectional rotation of the LV apex with respect to the base results in a "wringing" movement during ejection. The pattern of net LV twist in which the apex and the base rotate in different directions has been explained on the basis of varying spiral myofiber architecture of the apical and basal region and apex-to-base and transmural gradients in myosin phosphorylation (67,91).
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Left ventricular mechanical sequence synchronizes the direction of blood flow
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Magnetic resonance imaging (92) and echocardiography (61,93) can be used for deciphering the 2-dimensional features of LV intracavitary flow during different phases of cardiac cycle. During high temporal resolution contrast echocardiography ( [see ]), bubbles are tracked in time and space for creating trajectories of blood flow in 2 dimensions (61,93). Figure 10
shows the direction of blood flow during each phase of the cardiac cycle analyzed by echo contrast particle imaging velocimetry. After the onset of a Q-wave on the surface ECG, just before the mitral valve closure, the blood flow accelerates in the apex-to-base direction, paralleling the apex-to-base direction of electromechanical activation. This accelerated stream unites with a large vortex that is formed across the anterior edge of a closing anterior mitral leaflet ( [see ]). The forced acceleration of blood in the direction of LV outflow before the opening of the aortic valve correlates temporally with the reshaping movement of the LV wall seen during IVC. Contraction in one direction (right-handed helix) displaces blood, stretching the orthogonal direction (left-handed helix) during the isovolumic period. Because the left handed helix direction faces the outflow, blood is displaced towards the LV outflow before the aortic valve opening ( [see ]). Further propulsion of blood from the LV cavity results into ejection. IVR is characterized with rapid base-to-apex reversal of blood flow (61,94) ( [see ]). This explains the physiologic significance of early endocardial relaxation and opening of the LV cavity near the apex during IVR. This base-to-apex suction of blood during IVR helps to accommodate a greater base-to-apex surge of blood flow once the mitral valve opens during early diastolic filling. Both early and late diastolic flows are characterized with formation of a large anterior vortex across the anterior mitral leaflet and a small posterior vortex across the posterior mitral leaflet (61,95). Intracavitary blood flow seen during the different phases of the cardiac cycle thus provides enhanced understanding about the significance of the apex-to-base sequence of mechanical activation. Since inflow and outflow of the LV are found closely aligned at the "top" of the ventricle, apex-to-base activation and contraction of the subendocardial fibers contributes to acceleration of blood flow in the direction of the aortic outlet for optimal ejection (7,61).

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Figure 10 Digital particle image velocimetry profiles of left ventricular flow during each phase of the cardiac cycle. Under specific conditions of dilution and administration to blood circulation, the echo contrast particles (microbubbles) can be tracked for calculating vectors and trajectories of flow within a 2-dimensional ultrasound scan plane. The ensemble-averaged velocity magnitudes are superimposed on the vector fields during isovolumic contraction (a), ejection (b), isovolumic relaxation (c), early diastole (d), diastasis (e), and late diastole (f). Note the apex-to-base redirection of blood flow during isovolumic contraction with formation of a dynamic vortex across the inflow-outflow region and the base-to-apex reversal of blood flow during isovolumic relaxation. LA = left atrium; LV = left ventricle. Reproduced from Sengupta et al. (61).
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Final comments
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We have reviewed the LV myofiber architecture with the eletromechanical activation and intracavitary blood flow sequence and provided the reasoning for complex deformation of a beating heart observed in vivo. The short-lasting highly localized deformations and the physiologic asynchrony of cardiac deformation can be deciphered accurately only when analyzed in reference to the structural anisotropy of the underlying myocardial architecture. This information became available with the advent of high temporal resolution imaging methods and is fundamental for understanding cardiac physiology, optimization of cardiac therapies and planning of surgical procedures used for restoring the LV geometry (96). Another important objective in attempting to discern the link between the structure and function of a beating heart is to develop accurate computational models that can assimilate all imaging information for planning of proper therapeutic strategies for a given individual patient (97). Understanding the cardiac structurefunction relationship will also be essential for generating true anatomical constructs and scaffolds that would guide the emerging field of cardiac tissue engineering in time for designing future components of a "bioartificial heart" (98).
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Appendix
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To view videos and supplementary figures, please see the online version of this article.
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Footnotes
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This work was supported by grant HL68573 and, in parts, grants HL68555 and HL70363 from the National Institutes of Health and a Grant-in-Aid from the American Society of Echocardiography.
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