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The Journal of Physiology logoLink to The Journal of Physiology
. 2008 Aug 7;586(Pt 19):4721–4733. doi: 10.1113/jphysiol.2008.156323

Alteration in left ventricular normal and shear strains evaluated by 2D-strain echocardiography in the athlete's heart

S Nottin 1, G Doucende 1, I Schuster-Beck 2, M Dauzat 2, P Obert 1
PMCID: PMC2614036  PMID: 18687717

Abstract

The contraction of cardiomyocytes induces a systolic increase in left ventricular (LV) normal (radial, circumferential and longitudinal) and shear strains, whose functional consequences have not been evaluated, so far, in athletes. We used 2D ultrasound speckle tracking imaging (STI) to evaluate LV regional strain in high-level cyclists compared to sedentary controls. Sixteen male elite cyclists and 23 sedentary controls underwent conventional, tissue Doppler, and STI echocardiography at rest. We assessed LV long and short axis normal strains and shear strains. We evaluated circumferential–longitudinal shear strain from LV torsion, and circumferential–radial shear strain from the difference between subendocardial and subepicardial torsion. Apical radial strain (42.7 ± 10.5%versus 52.2 ± 14.3%, P < 0.05) and LV torsion (6.0 ± 1.8 deg versus 9.2 ± 3.2 deg, P < 0.01) were lower in cyclists than in controls, respectively. Rotations and torsion were higher in the subendocardial than in the subepicardial region in sedentary controls, but not in cyclists. Haemodynamic and tissue Doppler based indexes of global LV diastolic and systolic functions were not different between cyclists and controls. Athlete's heart is associated with specific LV adaptation including lower apical strain and lower myocardial shear strains, with no change in global LV diastolic and systolic function. These mechanical alterations could improve the cardiovascular adjustments to exercise by increasing the radial strain and torsional (and thus untwisting) response to exercise, a key element of diastolic filling and thus of cardiac performance in athletes.


During systole, contraction of cardiomyocytes induces myocardial normal strains, including longitudinal shortening (from base to apex), circumferential shortening (perpendicular to radial and to the longitudinal axis) and radial thinning (perpendicular to epicardium and to the longitudinal axis) (Moore et al. 2000). Each strain can be defined as the fractional change in length compared to its end-diastolic length. Moreover, due to the helically orientated myofibres (Torrent-Guasp et al. 2001), following right-handed and left-handed helical pathways in the subendocardial and subepicardial layers, respectively (Greenbaum et al. 1981), contraction also induces shear strains (i.e. transmural strains) within the myocardium (Rosen et al. 2004) including longitudinal–radial, circumferential–radial and circumferential–longitudinal components. Magnetic resonance imaging (MRI) studies have provided detailed insight into myocardial relaxation mechanisms and shown that, during diastole, shear strains decrease before normal strains (Rosen et al. 2004). This ‘elastic recoil’ (Notomi et al. 2006) causes the rapid reduction of left ventricular (LV) pressure that leads in turn to mitral valve opening and early filling (Dong et al. 2001; Notomi et al. 2008). Insight into myocardial normal and shear strains is therefore crucial for a better understanding of the complex LV mechanics that underlies LV function in the human heart.

The athlete's heart is a LV adaptation to long-term intensive endurance training characterized by an increase in chamber size, wall thickness and mass (Pelliccia et al. 1991). Most echocardiographic studies have evaluated ejection fraction and transmitral flow velocities to search for a relationship between cardiac hypertrophy and LV systolic and diastolic function (Pluim et al. 2000; Fagard, 2003). However, these haemodynamic variables do not provide any direct information about the myocardium motion and function. The tissue Doppler imaging (TDI) technique has been introduced to overcome this limitation (Caso et al. 2000; Schmidt-Trucksäss et al. 2001; Nottin et al. 2004; Saghir et al. 2007). However, as TDI measures velocities relative to the direction of the ultrasound beam, it yields only the longitudinal component of LV mechanics. To the best of our knowledge, and despite their relevance in the comprehension of LV function, normal and shear strains have never been investigated to date in the athlete's heart. Sympathetic activity (Maruo et al. 2007; Notomi et al. 2008), by its inotropic and lusitropic effects, and also LV dimensions and loading conditions (Moon et al. 1994; MacGowan et al. 1996) are important determinants of normal as well as shear strains. Since all these parameters differ at rest between athletes and sedentary individuals, alterations in normal and shear strains might be expected in the athlete's heart. The non-invasive evaluation of LV strains has been so far limited to tagged MRI, which is not widely available, and cannot be used in routine clinical practice. Recently, the development of 2D ultrasound speckle tracking imaging (STI) has allowed the angle dependence of TDI to be overcome and LV normal strains to be non-invasively evaluated (Amundsen et al. 2006). Moreover, STI has the capability to assess LV torsion (Helle-Valle et al. 2005), and to distinguish torsion of the subendocardial and subepicardial layers of the myocardium (Hui et al. 2007), thus providing information on the circumferential–longitudinal and circumferential–radial components of shear strains, respectively. In the present study, we used STI to evaluate LV normal and shear strains underlying the global LV function in the athlete's heart.

Methods

Study population

We evaluated 16 male elite cyclists and 23 age-matched sedentary controls. The elite cyclists participated in national cross-country cycling events and had been training 12.4 ± 3.6 hours per week for 11.0 ± 4.8 years, whereas none of the sedentary men reported regular training habits. All subjects underwent conventional and colour tissue Doppler echocardiography. None of them had any clinical or historical evidence of cardiovascular disease or arterial hypertension. A biometric evaluation including assessment of body fat mass by skin-fold thickness measurements was performed on all subjects (Durnin & Rahaman, 1967). This study received approval from the local ethics committee and written informed consent was obtained from all subjects. The study conformed with the Declaration of Helsinki.

Echocardiographic image acquisition

Images were obtained in the left lateral decubitus position after a 15 min resting period using a commercially available system (Vivid I, GE Healthcare, Horten, Norway) with a 3.5 MHz sector scanning electronic transducer. Gains and filters were adjusted carefully to eliminate background noise and allow for a clear tissue signal. Two-dimensional greyscale harmonic images were obtained at a rate of 60–75 frames s−1, and separate harmonic colour tissue velocity images were saved at a rate of 120–140 frames s−1, depending on both the depth and the sector width. Images were acquired in cine loops triggered to the QRS complex and saved digitally for subsequent off-line analysis with dedicated software (EchoPac 6.0, GE Healthcare, Horten, Norway). Measurements in athletes and in controls were obtained in a blind fashion.

Standard parameters

Standard echocardiograms consisted of two-dimensional, M-Mode and Doppler blood flow measurements. M-Mode measurements were obtained, according to the recommendations of the American Society of Echocardiography, in the parasternal long-axis view (Sahn et al. 1978). LV mass was calculated according to the Penn convention (Devereux et al. 1986). Pulsed Doppler LV inflow recordings, including early (E) and atual (A) waves, were performed in the apical four-chamber view, with the sample volume at the tip level of the mitral valves. Stroke volume was calculated as the product of the aortic root area and the integral of the aortic blood flow velocity recorded from a five-chamber view. Cardiac output was calculated as the product of stroke volume and heart rate and systemic vascular resistances as the ratio of mean arterial pressures and cardiac output.

Tissue Doppler imaging

Color cine loops were recorded in the apical two-, three- and four-chamber views for subsequent off-line tissue Doppler analysis. We assessed wall motion velocities at the mitral annulus level on the septal, lateral, inferior, anterior, antero-septal and posterior walls. Peak myocardial systolic velocity (Sm) and early (Em) and atial (Am) diastolic velocities were derived for each wall. The peak myocardial acceleration during isovolumic contraction (AIVC), recorded at the level of the lateral wall of the mitral annulus, was also used as an index of global LV contractility (Hashimoto et al. 2005). The E/Em ratio, recorded at the level of the lateral wall of the mitral annulus, was used as an index of LV filling pressure (Nagueh et al. 1997).

Speckle tracking imaging

The computer automatically selected suitable stable objects for tracking and then searched for them in the next frame using the sum of absolute difference algorithm (Leitman et al. 2004). After manually tracing the endocardial border on the end-systolic frame of the 2-D sequence, the software automatically tracked myocardial motion, creating six equidistant speckle tracking regions of interest in each image. Whenever the software signalled poor tracking efficiency, the observer readjusted the endocardial trace line and/or the region of interest width until a better tracking score could be obtained.

We evaluated three normal strains (Fig. 1), namely longitudinal and circumferential shortening/elongation and radial thickening/thinning, and two shear strains, namely shear in the circumferential and longitudinal plane and in the circumferential and radial plane. LV longitudinal strain and strain rate (SR) analysis was performed using an apical four-chamber view. Peak global longitudinal SR during the isovolumic relaxation period (SRIVR), a preload independent index of LV relaxation, was calculated as proposed by Wang et al. (2007). Radial and circumferential strain and SR analysis was performed on short-axis views. LV rotations, resulting from circumferential–longitudinal shear strains inside the myocardium, were calculated from basal and apical short axis views. Care was taken to ensure that the basal short-axis plane contained the mitral valve, and that the apical plane was acquired distally to the papillary muscle. The width of the region of interest was adjusted first, to include the entire myocardium. To obtain information on circumferential–radial strains, the region of interest was then set to include only the subendocardial and subepicardial layers in order to evaluate the difference in torsion between the inner and outer layers (Hui et al. 2007). Basal and apical rotation of the entire myocardium and subendocardial and subepicardial layers were analysed in 12 subjects blindly on two separate days by an experienced cardiologist in order to assess intraobserver reproducibility. Since the reproducibility was good, only data on the first assessment were presented in the present study (myocardium –c.v.: 5.4–11.9%; R2: 0.97–0.99; subendocardial layer –c.v.: 8.1–9.1%; R2: 0.92–0.99; subepicardial layer –c.v.: 13.3–13.9%; R2: 0.89–0.92).

Figure 1. Directions of normal and shear strains.

Figure 1

A, illustration of the systolic strains evaluated in the study: longitudinal (L), radial and circumferential (C) strains; circumferential–radial (C-R) and circumferential–longitudinal (C-L) shear strains. B, adjustment of the region of interest on both subendocardial and subepicardial layers in order to evaluate the difference of torsion between the inner and outer layers. C, adjustment of the region of interest on the entire myocardium to assess both LV basal and apical rotations.

In order to assess the dynamics of global LV twist and its relation to radial displacement throughout the cardiac cycle, we constructed twist-displacement loops (Nakai et al. 2006). Averaged radial displacement data from six segments in basal and in apical short-axis planes were summed and divided by 2 to obtain the mean value of radial displacement throughout the cardiac cycle. Twist-displacement loops were constructed for each subject. To create average twist-displacement loop in each group, the time sequence was normalized to the percentage of systolic duration.

All data were exported to a spreadsheet program (Microsoft Excel) to calculate LV torsion and torsion rate. To adjust all strain parameters for intersubject differences in heart rate, the time sequence was also normalized to the percentage of systolic duration (i.e. t was 100% at end systole). Spreadsheet calculation allowed the detection of peak systolic and diastolic SR, the peak of LV twist and untwist rates, and the time to these peaks.

Statistical analysis

The statistical analysis was performed with Statview 5.0 (SAS Institute, Cary, NC, USA). Data were expressed as means ±s.d. Analysis of variance was used to compare each variable between the two groups. The significance of variation in torsion at different locations was determined by a two-way analysis of variance (group × location). Simple linear regression analyses between HR and LV radial strain, strain rate, torsion, twisting and untwisting rate were performed. Statistical significance was assessed when P < 0.05.

Results

Biometric data

There were no differences in age (24.6 ± 4.6 versus 22.6 ± 5.4 year), height (179.1 ± 6.5 versus 179.0 ± 6.3 cm) and body mass (71.5 ± 5.8 versus 73.1 ± 9.7 kg) between controls and cyclists, respectively. The cyclists exhibited a lower percentage of body fat mass than controls (12.6 ± 2.4 versus 16.8 ± 4.5%; P < 0.001).

Standard echocardiography and TDI

Elite cyclists exhibited a marked LV hypertrophy on account of increased cavity dimension and wall thickness (Table 1). However, the ratio of wall thickness to LV radius was similar in controls and cyclists.

Table 1.

Standard echocardiography

Controls Cyclists
Morphological parameters
 LV end-diastolic diameter (mm) 49.5 ± 3.8 56.8 ± 3.1***
 LV end-systolic diameter (mm) 30.4 ± 3.6 36.2 ± 3.5***
 Septal wall thickness (mm) 11.0 ± 1.4 12.8 ± 1.3***
 Posterior wall thickness (mm) 6.8 ± 0.8 8.1 ± 1.2**
 LV mass (g) 154 ± 24 238 ± 29***
 Ratio wall thickness/end-diastolic diameter 0.36 ± 0.05 0.36 ± 0.05
Global diastolic function
 Peak E velocity (cm s−1) 80.2 ± 7.8 81.9 ± 7.7
 Peak A velocity (cm s−1) 49.5 ± 8.4 42.8 ± 7.0*
 Peak E/A ratio 1.70 ± 0.37 1.95 ± 0.30*
Global systolic function
 Fractional shortening (%) 38.6 ± 4.6 36.3 ± 4.1
 Heart rate (beat min−1) 70 ± 10 56 ± 7***
 Stroke volume (ml) 75.9 ± 11.4 100.0 ± 11.3***
 Cardiac output (l min−1) 5.3 ± 1.1 5.6 ± 1.0
Arterial pressures
 Systolic (mmHg) 135 ± 15 127 ± 8
 Diastolic (mmHg) 70 ± 9 69 ± 9
 Systemic vascular resistances (A.U.) 17.6 ± 3.2 16.1 ± 3.1

Significant differences:

*

P < 0.05

**

P < 0.01

***

P < 0.001.

Haemodynamic parameters of LV global diastolic and systolic functions are presented in Table 1. Cyclists had higher stroke volume and lower heart rate than controls. There was no difference in cardiac output, systemic vascular resistances, or fractional shortening between the two groups. The cyclists and controls showed also similar mean (i.e. mean of the 6 walls) peak Sm (7.6 ± 0.8 versus 8.0 ± 0.8 cm s−1, respectively) and AIVC (184 ± 35 versus 204 ± 63 cm s−2, respectively). Cyclists had similar peak E, but lower peak A than controls, resulting in higher E/A ratio in the former. There was no difference in mean peak Em between the two groups (11.9 ± 1.8 versus 11.5 ± 1.8 cm s−1, respectively). Mean peak Am was non-significantly lower (4.6 ± 0.8 versus 5.2 ± 1.9 cm s−1), and the E/lateral Em ratio was similar (6.2 ± 1.0 versus 5.7 ± 0.7) in the cyclists and controls, respectively.

Regional LV strains

Patterns of longitudinal, radial and circumferential strains during the cardiac cycle are reported in Fig. 2. Peak systolic and diastolic SR and their respective time to peak (expressed as percentage of systole duration) are presented in Table 2. Longitudinal strains (−19.2 ± 1.9%versus−19.5 ± 2.2%), systolic and diastolic peak and time to peak longitudinal SR (Table 2) and longitudinal SRIVR (0.19 ± 0.11 s−1versus 0.22 ± 0.09 s−1) did not differ between the cyclists and controls, respectively. Similar results were obtained for peak circumferential strains (−16.0 ± 3.5%versus−16.2 ± 3.4% at the basal level and −18.1 ± 2.5%versus−18.6 ± 4.1% at the apical level) as well as systolic and diastolic peak and time to peak circumferential SR. However, peak apical radial strains were lower in cyclists than in controls (42.7 ± 10.5%versus 52.2 ± 14.3%, P < 0.05). Peak apical radial SR was also lower in the cyclists during systole but not during diastole. HR correlated with peak apical radial strains (P < 0.01) and peak apical radial SR during systole (P < 0.05) (Fig. 3). Peak basal radial strains (41.7 ± 11.9%versus 41.5 ± 14.4%), and their respective peak and time to peak SR were not different in cyclists and controls, respectively.

Figure 2.

Figure 2

LV basal and apical circumferential and radial strains and LV longitudinal strains in sedentary subjects (•) and cyclists (◯)

Table 2.

Peak and time to peak strain rates during systole and diastole

Controls Cyclists


Peak Time to peak Peak Time to peak
Systole
 Longitudinal SR (s−1) −1.08 ± 0.15 45 ± 9 −1.01 ± 0.13 49 ± 5
 Radial SR (s−1)
  Basal level 1.64 ± 0.35 41 ± 14 1.39 ± 0.33* 41 ± 12
  Apical level 1.59 ± 0.33 47 ± 17 1.33 ± 0.22* 57 ± 14
 Circumferential SR (s−1)
 Basal level −1.15 ± 0.29 38 ± 10 −1.02 ± 0.23 40 ± 12
  Apical level −1.15 ± 0.28 53 ± 8 −1.01 ± 0.19 50 ± 8
 Rotational rate (deg s−1)
  Basal level −68.2 ± 23.0 51 ± 12 −56.5 ± 16.8 55 ± 8
  Apical level 56.1 ± 20.4 26 ± 10 35.8 ± 15.0** 26 ± 6
 Torsional rate (deg s−1) 72.3 ± 22.9 49 ± 12 48.5 ± 17.7** 59 ± 17*
Diastole
 Longitudinal SR (s−1) 1.55 ± 0.33 138 ± 9 1.38 ± 0.25 138 ± 7
 Radial SR (s−1)
  Basal level −1.58 ± 0.35 137 ± 21 −1.33 ± 0.30* 135 ± 26
  Apical level −2.12 ± 0.49 144 ± 13 −1.72 ± 0.59* 150 ± 10
 Circumferential SR (s−1)
  Basal level 1.25 ± 0.41 129 ± 15 1.14 ± 0.28 132 ± 19
  Apical level 1.36 ± 0.29 147 ± 8 1.32 ± 0.29 144 ± 11
 Rotational rate (deg.s−1)
  Basal level 47.6 ± 15.8 123 ± 24 54.5 ± 23.9 118 ± 17
  Apical level −47.1 ± 29.5 170 ± 11 −44.0 ± 14.0 175 ± 8
 Torsional rate (deg s−1) −72.9 ± 20.7 121 ± 14 −68.2 ± 33.5 122 ± 24

SR: Strain rate; Time to peak expressed as percentage of systolic duration. Significantly different from sedentary subjects:

*

P < 0.05

**

P < 0.01.

Figure 3.

Figure 3

Correlations between heart rate and torsion, torsion rates, radial strain and strain rates

Basal and apical rotations and LV torsion are presented in Fig. 4. As viewed from the apex, positive values represent counterclockwise rotation and negative values clockwise rotation. In both groups, similar patterns of LV rotations and torsion were obtained. LV torsion was produced by counterclockwise apical rotation and clockwise basal rotation. At aortic valve closure (AVC), there was no significant difference in basal rotation between the cyclists and controls (−5.2 ± 2.4%versus−4.8 ± 3.2%, respectively). However, the cyclists showed lower apical rotation (1.7 ± 1.9%versus 4.0 ± 2.9%, P < 0.05) and lower LV torsion (6.0 ± 1.8%versus 9.2 ± 3.2%, P < 0.01) than controls, respectively. Rotational rate at the apical level and torsional rate were lower in the cyclists than in controls during systole but not during diastole. LV untwisting during isovolumic relaxation, reached 46 ± 24% in the cyclists and 44 ± 22% in controls, respectively (NS). HR correlated with LV torsion (P < 0.01) and peak torsion rate during systole (P < 0.01) but not during diastole (NS).

Figure 4.

Figure 4

LV basal and apical rotation and LV twist of the subendocardial and subepicardial layers in sedentary subjects (left) and cyclists (right)

Torsion–radial displacement loops (Fig. 5) showed, in both groups, a small initial clockwise twist at the onset of ejection followed by a linearly increasing, counterclockwise twist throughout systole. Torsion and displacement were linearly correlated during systole (R= 0.94 ± 0.06, range: 0.81–0.99 versus R= 0.97 ± 0.03, range: 0.81–0.99 in the cyclists and controls, respectively). However, the rate of systolic twist with respect to radial displacement, determined by the slope of systolic twist, was lower in the cyclists than in controls (1.09 ± 0.30 versus 1.85 ± 0.60 deg mm−1, respectively, P < 0.001), a difference produced by both lower peak torsion (Fig. 4) and higher radial displacement at end-systole (7.5 ± 0.8 mm versus 6.4 ± 0.9 mm, respectively, P < 0.001). Early diastole was characterized by rapid untwisting despite small radial displacement. From mid to late diastole, untwisting was smaller whereas displacement was larger.

Figure 5.

Figure 5

Torsion–radial displacement loops

Regional LV rotations and torsion in the subendocardial and subepicardial layers

Mean basal and apical rotations of the subendocardial and subepicardial layers are presented in Table 3. In controls, rotations and torsion were overall higher in the subendocardial than in the subepicardial region. At AVC, differences between the two layers reached statistical significance for basal rotation and for LV torsion, but not for apical rotation. In cyclists, who exhibited lower LV torsion than controls, there were no differences at AVC between subendocardial and subepicardial layers regarding basal and apical rotations as well as torsion. Regional differences in torsion in the six equidistant speckle tracking regions of both layers are depicted in Fig. 6. In both the cyclists and controls, only small differences in subepicardial torsion were found between regions. However, the higher subendocardial torsion in the cyclists than in controls was mainly due to the higher contribution of the lateral and anterior walls. In both groups, the larger transmural differences in torsion occurred in these two regions, but reached statistical significance only in controls.

Table 3.

Peak rotations and torsion of the subendocardial and subepicardial layers

Controls Cyclists


Subendocardial layer Subepicardial layer Subendocardial layer Subepicardial layer
Basal rotation (deg) −6.0 ± 3.6 −4.1 ± 3.0††† −4.5 ± 2.8 −3.6 ± 2.5
Apical rotation (deg) 4.0 ± 3.4 3.0 ± 2.3 1.3 ± 2.1* 1.2 ± 1.5**
Torsion (deg) 10.0 ± 4.3 7.3 ± 2.4††† 5.8 ± 3.1*** 4.7 ± 2.6**

Significantly different from sedentary subjects:

*

P < 0.05

**

P < 0.01

***

P < 0.001.

Significantly different from subendocardial layer:

†††

P < 0.001.

Figure 6. Regional LV twist at aortic valve closure of the subendocardial (filled boxes) and subepicardial (open boxes) layers in sedentary subjects (left) and cyclists (right).

Figure 6

AVC: aortic valve closure; Sept: septal; Inf: inferior; Post: posterior; Lat: lateral; Ant: anterior; Ant-Sept antero-septal.

Discussion

The aim of the present study was to evaluate LV regional strains in the athlete's heart. We used STI, a new echocardiographic tool, to assess LV normal and shear strains during the cardiac cycle in elite cyclists. The main results were a lower LV apical radial strain and shear strains contrasting with identical LV global systolic and diastolic function. These results emphasize the usefulness of STI to assess regional specificities of the myocardium in the trained heart.

LV systolic strains

Whereas global LV function has been extensively studied (Pluim et al. 2000; Fagard, 2003), there have been no reports on regional myocardial strains in endurance-trained subjects. The results of the present study show that long-term high-intensity endurance training induces a non-uniform decrease in the three components of LV normal strains (i.e. longitudinal, circumferential and radial strains). On average, peak longitudinal strain and SR during systole in the cyclists were similar to those observed in their sedentary controls. This result confirms previous data obtained by tissue Doppler imaging (i.e. longitudinal velocities) in our laboratory (Nottin et al. 2004) or by others (Schmidt-Trucksäss et al. 2001), and highlights that LV longitudinal function is normal in the athlete's heart at rest. However, the short-axis evaluation highlighted that, whereas peak circumferential shortening was normal on both apical and basal regions, peak radial thickening at the apical level was significantly lower in the cyclists when compared to controls. The underlying mechanisms responsible for this still remain partly understood. Recently, Akagawa et al. (2007) assessed the effect of sympathetic stimulation on LV radial strains. Interestingly, radial strain increased as dobutamine doses increased along the whole dose range at the apex, but only for low concentrations at the base. This demonstrates that LV radial strain at the apex is more sensitive and dependent on sympathetic stimulation than at the base. Of note, our cyclists had a significantly lower resting HR than controls, which is largely documented in the scientific literature and attributed to training-induced changes in sympathovagal balance, including a decrease in sympathetic activity and a relatively enhanced parasympathetic stimulation (Aubert et al. 2003). A decrease in autonomic efferent activity may therefore be involved in the decreased apical radial strains in our cyclists. The significant correlation observed between HR and apical radial strain in the present study speaks in favour of this hypothesis.

Due to the various orientations of myofibres across the LV wall (i.e. subendocardial versus subepicardial layers), contraction of myocardium induces shear strains. In the present study, we evaluated LV torsion that resulted from the circumferential–longitudinal component of myocardial shear strains. Moreover, we differentiated between torsion of the inner and outer layers of the myocardium in order to evaluate the circumferential–radial component of myocardial shear strains (Buchalter et al. 1990; Hui et al. 2007). Our findings emphasized that both components of shear strains were significantly lowered in the athlete's heart at rest. Our regional evaluation highlighted that LV torsion was lower in the cyclists than in controls, especially in the subendocardial layer of the lateral and anterior walls (Fig. 6). The underlying mechanisms responsible for this training-induced decrease in LV shear strains at rest remain unclear. It has been shown that LV torsion depends on the LV wall thickness to LV radius ratio (Lumens et al. 2006). However, our cyclists' hypertrophied hearts were characterized by a normal LV wall thickness to radius ratio. MacGowan et al. (1996) reported that LV torsion depends also in part on afterload. We calculated systemic vascular resistances, an overall index of afterload, and found no difference between the cyclists and controls. Another plausible explanation for the lower LV torsion observed in the cyclists could be a specific endocardial adaptation to training. Due to their helical pathways with mutually opposite pitch direction, the fibres in the inner and outer layers of the ventricle wall exert opposite torques. Outer layers produce larger torques than inner layers because of their longer lever, resulting in a torsion that favours outer layers. LV torsion increases when subendocardial contractility diminishes, as in patients with aortic stenosis (Van Der Toorn et al. 2002), subendocardial infarction (Maruo et al. 2007) or with advanced age (Lumens et al. 2006; Takeuchi et al. 2006). To date there is a distinct lack of data as regards the specific effect of endurance training on subendocardial and subepicardial contractile function. Interestingly, previous animal studies conducted in our laboratory (Cazorla et al. 2006) or by others (Diffee & Nagle, 2003) on isolated cardiomyocytes demonstrated that the effect of exercise training on contractile properties was more pronounced in the subendocardial than in the subepicardial region. This regional training-induced adaptation, if present in humans, could constitute a potential mechanism involved in the lower LV torsion observed in our cyclists. This hypothesis needs further investigation to be confirmed. Finally, it has likewise been shown that LV torsion is partly driven by sympathetic activity (Rademakers et al. 1992; Akagawa et al. 2007; Notomi et al. 2006; Notomi et al. 2008). The aforementioned reduced sympathetic stimulation at rest in our cyclists might therefore have also contributed to their lower LV torsion.

LV diastolic function

In healthy adults, a MRI evaluation of the time sequence of LV strain development showed that myocardial shear strains resulting from the unfolding of myofibres occur early in diastole (Rosen et al. 2004) and are critical in the rapid decrease in LV pressure inducing early filling (Rademakers et al. 1992; Notomi et al. 2006; Notomi et al. 2008). In the present study, despite a decrease in LV shear strains, global diastolic function, assessed by the pattern of LV filling throughout the mitral valve, remained unchanged in the cyclists. We referred to peak longitudinal SRIVR (Wang et al. 2007) and peak untwist rate in the early diastole (Notomi et al. 2006), as new less load-dependent indexes of LV diastolic function. In our elite cyclists, both indexes of global LV relaxation remained in the same range as those of their sedentary controls, further supporting the notion of normal LV global function at rest in the athlete's heart. Moreover, the twist-displacement loops highlighted that, in both groups, substantial untwisting occurred despite a relatively small radial displacement, in early diastole, whereas untwisting was markedly smaller during the late phases of diastole in spite of substantial radial displacement. This highlights the fact that, in cyclists as well as in controls, the ventricle untwists, rapidly recoiling and creating diastolic suction (Notomi et al. 2008). However, since LV shear strains and consequently elastic recoil were lower in the cyclists, other factors such as improved enhanced calcium reuptake by the sarcoplasmic reticulum, via an increase in sarcoplasmic reticulum Ca2+-ATPase activity during diastole (Morán et al. 2003) might well be involved to allow the cyclists to maintain their LV global diastolic function during resting conditions.

Functional implications

Notomi et al. (2006) recently used the concept of LV systolic torsion and subsequent diastolic untwisting to explore the mechanisms of diastolic filling during exercise. They observed that the magnitude of increase in twisting and untwisting rates during exercise was significantly greater than the corresponding changes in LV length and radius. This finding suggests that the enhanced diastolic function during exercise is mainly due to the more vigorous untwisting motion of the LV, especially at the apical level, which induces an increase in intraventricular pressure gradient and thus LV suction. In the present study, despite lower LV apical strains and LV shear strains in the cyclists than in controls, overall systolic and diastolic functions were similar. We can reasonably hypothesize that the reduced shear strains observed at rest in the cyclists could represent a greater reserve of shear strains during exercise. In the athlete's heart, this greater reserve could constitute a mechanism by which endurance-trained subjects enhanced their diastolic function during upright exercise compared to sedentary subjects (Matsuda et al. 1983; Di Bello et al. 1996). This may be a key factor in their greater increase in stroke volume and cardiac performance.

Study limitations and future research

This study suffers from some limitations. Since a cross-sectional study is by nature descriptive, further studies including training programmes will be needed to ascertain that differences in LV normal and shear strains reported here are effectively linked to training stimuli. We did not use any gold standard to measure LV torsion. The exact location of the basal and apical planes may be different from patient to patient, resulting in some measurement errors. However, a previous study has recently validated the accuracy of STI versus tagged MRI (Helle-Valle et al. 2005). On the other hand, STI analysis cannot eliminate errors introduced by through-plane motion, particularly at the basal level. For the assessment of circumferential-radial shear strains, we used an index based on the intramural differences in LV torsion. This method requires the ROI corresponding to the subepicardium and subendocardium layers to be determined subjectively. Future experiments using 3D tagged MRI, which is to date considered as the gold standard method to evaluate shear strains inside the myocardium, might resolve this issue.

The results of the present experiment raised a number of important questions. One potential mechanism for the reduced LV strains and torsion observed in our athletes could be their reduced sympathetic stimulation during resting conditions, and further studies using dobutamine stress echocardiography will be needed to test this assumption. Another plausible explanation is related to a specific effect of endurance training on subendocardial and subepicardial contractile function. Further experiments using animal models will have to be carried out to check this hypothesis and, if this effect is confirmed, to better understand the underlying mechanisms responsible for such regional adaptations. Finally, patterns of LV normal and shear strains should be evaluated during effort to see whether the alterations observed in the present study at rest have functional significance during exercise.

Conclusion

STI allowed the assessment of LV normal and shear strains in elite endurance cyclists and sedentary controls. The athlete's heart was characterized by specific adaptations including lower LV apical radial strain and shear strains. These physiological adaptations observed during resting conditions raised some questions. Further studies are needed to evaluate their role in the enhanced cardiac performance observed during exercise in highly trained athletes.

Acknowledgments

We thank GE Medical Systems–Ultrasound France for providing the ultrasonic equipment used for this study. The authors affirm that they have no personal interest, financial or otherwise, with any commercial company with potential financial interest in the subject matter enclosed in this article.

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