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Ann Thorac Surg 2001;72:966-974
© 2001 The Society of Thoracic Surgeons
a Department of Cardiothoracic Surgery, Stanford University School of Medicine, Stanford, California, USA
Address reprint requests to Dr Miller, Falk Cardiovascular Research Center, Stanford University School of Medicine, Stanford, CA 94305-5247
| Abstract |
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| Introduction |
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Mitral annular physiology has been studied in both experimental animals and human subjects using two-dimensional (2-D) [1] and three-dimensional (3-D) [2, 3, 6] roentgenogram marker imaging, sonomicrometry [7], magnetic resonance imaging (MRI) [8], and 2-D [9, 10] and 3-D [1114] echocardiography. The current literature consensus firmly supports dynamic motion of the annulus throughout the cardiac cycle, yet the timing and extent of annular area change has been a point of ample controversy. This debate is further compounded by discordant results in studies investigating annular motion in the setting of mitral ring annuloplasty [6, 10, 1215]. These apparent discrepancies may be due to varying patient characteristics, species differences, and methods of measurement. We reviewed our experimental data in dogs and sheep as well as the clinical and experimental data in the literature to synthesize a more complete understanding of these inconsistencies.
| Animal studies |
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The discrepancy in the timing of the actual nadiror minimalmitral area between canine [17] and ovine [2] experiments (near end-systole versus end-diastole) may possibly be related to interspecies anatomic differences. Insertion of atrial fibers in the mitral ring is more variable in dogs than in sheep, as reported by Walmsley [21]; Gorman and coworkers [7] suggested that sheep leaflets originate from atrial muscle alone, whereas the mitral leaflets in dogs are attached to the ventricular myocardium. These anatomical findings would argue for a more pronounced "atriogenic" influence in the ovine annulus, which would be responsible for more presystolic annular area reduction coincident with atrial contraction [22]. On this basis, minimal annular area would be expected to occur near end-diastole or early in systole in sheep but perhaps not in dogs.
From these experimental findings it is clear that the mitral annulus is a dynamic structure that undergoes substantial area change throughout the cardiac cycle, which is affected by inotropic state. The timing of maximum and minimum annular area and the presystolic contribution to annular area reduction vary and may be influenced by species differences. For perspective and comparison, the spectrum of measurements of annular area and extent of dynamic size change in various animal species that is available in the English literature are summarized in Figure 2.
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| Human studies |
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On the other hand, similar large mitral annular sizes measured using 3-D TEE were recently reported in normal control subjects [5]. Mean mitral area was found to be 11.8 ± 2.5 cm2 in otherwise healthy persons with normal left ventricular systolic function undergoing echocardiography in search of a source of cardiac emboli. The nonplanar shape of the mitral annulus was maintained throughout the cardiac cycle, but annular "folding" during systole was also confirmed, with the anterior annulus tilting back toward the left atrium; interestingly, this folding motion appeared to be independent of LV systolic function. For perspective, mean mitral annular area was 10.2 ± 2.4 cm2 in 5 patients with hypertrophic cardiomyopathy (HOCM) and 15.2 ± 4.2 cm2 in 3 patients with dilated cardiomyopathy (p = not significant due to small numbers). Mitral annular size was largest at end-diastole and smallest at end-systole, with a 24% ± 5% reduction between maximum and minimum area in the control subjects, 32% ± 8% in those with HOCM, and 13% ± 2.3% in the patients with dilated cardiomyopathy (p < 0.001). These TEE estimates of change in mitral annular area are relatively large, assuming that true annular motion was actually being tracked; alternatively, these large annular areas and hyperdynamic variations in annular size may possibly represent motion of the basal LV myocardium. Using 2-D echocardiography, Yiu and colleagues [27] from the Mayo Clinic recently reported mitral annular area contraction to be 36% ± 6% in normal subjects and 19% ± 7% in patients with left ventricular dysfunction and functional mitral regurgitation, or FMR (approximately one half of whom had ischemic MR). These annular area reduction measurements parallel those reported by Flachskampf and colleagues [5]; importantly, however, the systolic and diastolic mitral annular areas measured by the Mayo Clinic group in normal subjects were much smaller, being only 4.4 ± 0.7 cm2 and 6.9 ± 0.8 cm2, respectively. Indeed, these 2-D echo measurements closely approximate the areas obtained in fresh specimens [23, 24]. Why such relatively large annular area reduction was calculated by these authors is unknown.
In addition to echocardiography, MRI has been used to study 3-D annular motion in humans. Komoda and coworkers [8] in Berlin studied 7 normal human volunteers and found that mitral annular area was maximal in late diastole (9.5 ± 1.4 cm2), decreased by 19% ± 8% by early systole and to 8.6 ± 1.2 cm2, and was smallest during mid to late systole (6.9 ± 1.1 cm2), for an overall size reduction of 26% ± 5% from maximum to minimum. This degree of overall relative annular size decrease was almost identical to that detected echocardiographically by Ormiston and colleagues [9] and Flachskampf and associates [5]. This same Berlin group [28] described translational motion of the posterior annulus into and out of the annular plane, which was felt to represent contraction of the bulbospiral and sinospiral muscle fibers in the basal LV myocardium. Annular systolic tilting or folding motion and the saddle or ski jump shape of the normal human mitral annulus were also observed, which supports the 3-D echocardiographic data [5]. Figure 3 illustrates the range of human mitral annular area measurements reported in the English literature; the variability of these estimates is noteworthy.
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| Annuloplasty rings |
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Echocardiographic evaluation of patients with annuloplasty rings has also generated a broad spectrum of findings. Okada and colleagues [30] reported that overall mitral annular area fell during the cardiac cycle in patients with a Duran flexible ring by 26% ± 4% but no change in area was seen in the patients with a Carpentier-Edwards ring. In the Duran group, as in the normal native human [9] and ovine [2] annulus, maximal annular size corresponded to the time of the ECG P wave (or atrial systole) during diastole, followed subsequently by both presystolic and systolic area reduction. Comparison of the two types of rings indicated that this pronounced difference in annular motion made a flexible Duran ring behave like a smaller C-E ring in systole (minimum area) but like a larger C-E ring in diastole when LV filling takes place. Despite the technical limitations inherent in this echocardiographic study, the results are provocative and favor a flexible annuloplasty ring.
Yamaura and associates [12] from this same Kobe group later investigated mitral repair in patients with Duran and Carpentier-Edwards Classic rings and in control human subjects. Mitral annular area was 6.5 ± 0.1 cm2 and 5.7 ± 0.9 cm2 at end-diastole and end-systole, respectively, in the normal controls (p = 0.0001), whereas it was 4.0 ± 0.1 cm2 and 3.6 ± 0.1 cm2 in the 29 mm Duran ring group (p = 0.0001). For patients with 30 mm Carpentier-Edwards rings, these areas were 3.3 ± 0.1 cm2 and 3.3 ± 0.1 cm2 (p = NS), which is smaller than the manufacturers geometric specifications (3.95 cm2) for this size C-E Classic ring. Consistent with their earlier findings [30], mitral annular motion in the Duran ring group was dynamic (change in area of 10% ± 2%) and similar to that seen in the control subjects (area change = 12% ± 2%). The annulus had a characteristic saddle shape at both times and descended toward the LV apex during systole. The mitral annulus in patients with a C-E ring was adynamic and had a fixed planar configuration but still moved apically during systole.
In an updated analysis using computerized 3-D image reconstruction [31], mitral annular motion was again shown to be dynamic in patients with a Duran ring, and the substantial presystolic narrowing of the human mitral annulus was confirmed again. Overall area change was 25% ± 2% in those with a Duran ring, similar to the 26% ± 4% estimate reported by Okada and colleagues [30] earlier based on 2-D TTE images. Both of these figures, however, differ markedly from the 10% ± 2% area change using TEE reported previously by this same group [12], as discussed above. Further analysis of the echocardiographic data of the Yamaura patient cohort was once again published in 1998 [32]. Mitral annular area fractional change was reported as 15% ± 2% in patients with a Duran ring (compared with 25% ± 2% reported previously in the same patient population) but this figure in their 1998 paper was the percent area change from end-diastole to end-systole rather than from the time of maximum to minimum annular area during the cardiac cycle. The raw annular areas were significantly larger for both the patients with the Duran or C-E rings than previously reported in their smaller patient cohort in 1995 (end-diastolic size of 6.6 ± 0.1 cm2 versus 4.0 ± 0.1 cm2 and 5.5 ± 0.2 cm2 versus 3.3 ± 0.1 cm2 for Duran and C-E, respectively) [12]. The most obvious explanation for this glaring inconsistency is analytical error introduced by the two different methods of computing the actual 3-D dimensions of the mitral annulus, ie, manual projections versus computerized calculations based on multiple 2-D volume data sets. Conversely, there was no demonstrable area change in patients with a C-E ring, and the annular shape was found again to be fixed in a planar configuration.
In an elegant, scientifically rigorous, automated 3-D TEE (Echoscan; TomTec GmbH, Munich, Germany) intraoperative, open chest assessment of both the partial Cosgrove-Edwards flexible and the rigid, complete Carpentier-Edwards Classic annuloplasty ring, DallAgata and associates [14] reported that the Cosgrove ring internal area changed by approximately 13% from end-diastole to end-systole, with a mean end-diastolic area of 4.8 ± 1.6 cm2 and mean end-systolic internal area of 4.2 ± 1.5 cm2 (for ring sizes 32 to 38 mm). The anteroposterior (A-P) mitral diameter fell significantly (p < 0.01) from 2.1 ± 0.2 cm at end-diastole to 1.9 ± 0.3 cm at end-systole, whereas the transverse (probably equivalent to the commissure-commissure dimension) mitral diameter did not change (2.5 ± 0.6 cm at ED and 2.5 ± 0.6 cm at ES) nor did the extrapolated distance between the tips of the Cosgrove band (2.3 ± 0.5 cm versus 2.1 ± 0.4 cm, respectively). As expected, the Carpentier-Edwards Classic ring completely abolished normal annular dynamics. Correlation between Cosgrove-Edwards ring true length (as provided by the manufacturer) and measured ring length was good (r = 0.95) in 16 of the 17 patient studies suitable for analysis, but the echocardiography underestimated this measurement by 11.5 mm across all ring sizes. This error was explained as possibly being due to the fact that the echocardiography measurements were based on the echo interface at the inner border of the ring. Therefore, the authors believed that these 3-D TEE measurements underestimated true dimensions and lengths by about 10% and mitral area by approximately 20%. If one multiplies the observed area by this correction factor (1.2x), the Cosgrove ring true in vivo areas would be approximately 5.8 cm2 and 5.0 cm2 at ED and ES, respectively, and the Carpentier-Edwards internal ring areas 4.4 cm2 and 4.6 cm2.
Markedly discordant measurements of partial annuloplasty ring area, however, were obtained by Cosgrove and associates [10] using TEE in 5 selected patients immediately postoperatively and at an average of 9 months after mitral repair with the Cosgrove-Edwards band. As observed with a complete flexible ring [12], these echo images confirmed that the saddle shape nature of the mitral annulus was preserved after implantation of a Cosgrove-Edwards ring. The early postoperative percent annular area reduction was 7%, increasing to a 16% area reduction 9 months later. It is noteworthy to recognize that this increase in fractional mitral area change was due in part to a 10% increase over time in diastolic area, something that is highly unlikely to occur after successful mitral ring annuloplasty, and which probably represents some type of measurement error. Systolic area was the same at both times. After 5 years, fractional mitral annular area reduction of the Cosgrove ring was found to be 28% ± 11%, closely reflecting the 25% ± 10% reduction in annular size in normal subjects [13, 33]. More troublesome is the fact that the maximum annular area of the Cosgrove ring measured in these studies was more than twice as large as that reported by DallAgata and associates [14] (vide supra). Assuming the average ring size was 30 mm, when the Cosgrove-Edwards band internal diameter is normalized to the geometry of a Carpentier-Edwards Physio ring, it would be expected to have a geometric orifice area of between 4.4 cm2 and 5.0 cm2. But the areas reported by Cosgrove and associates [10] are approximately twofold larger. This raises the question of exactly what cardiac structure was actually being imaged echocardiographically. Potentially, basal LV wall motion rather than annular motion or perhaps the external border of the ring were imaged, both of which might explain greater dynamic motion and the large annular areas reported. Since both the DallAgata group and the Cleveland Clinic group used transesophageal 3-D echocardiographic approaches, the incongruity in their data assessing the same type of ring underlines the current difficulty inherent in standardizing and calibrating 3-D TEE data, especially the derived 2-D spatial measurements.
Roentgenogram fluoroscopic determination of annular motion in human subjects in the setting of mitral annuloplasty has been used by Scrofani and colleagues [34] at 10 days, 1 year, and 5 years after mitral repair. The computed "annular areas" were actually "hemiareas" as a pericardial annuloplasty strip was placed only on the posterior annulus from commissure to commissure and thus did not include the area of the anterior annulus. Annular hemiarea reduction during systole was determined to be 9% ± 6%, 8% ± 6%, and 15% ± 10% at 10 days, 1 year, and 5 years after the operation, respectively, mirroring the apparent increasing flexibility of a Cosgrove-Edwards ring over time as reported above [10, 33]. These results must be interpreted cautiously, however, as the anterior annulus, which normally is less dynamic than the posterior annulus [3, 17, 28], was not included in these calculations of area change. Therefore, the percent hemiarea reduction probably does not reflect total annular area reduction accurately since these calculations were based only on the motion of the most dynamic portion of the mitral annulus. For easier interpretation and perspective, data from all the above studies investigating mitral orifice area and the motions of flexible annuloplasty rings in human are depicted graphically in Figure 5.
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| Conclusion |
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Clinical measurements of mitral annular dynamics, mostly derived from either 2-D or 3-D echocardiography, are fraught with even greater inconsistencies (Fig 3). For instance, both Gillinov and associates [13] and DallAgata and associates [14] used 3-D echocardiography to assess orifice area of the Cosgrove-Edwards ring but the reported annular area size obtained by the former group was about twice as large as the expected ring areas should be according to the manufacturers physical specifications. Methods of image analysis can also introduce error into area calculations as evidenced by Yamauras measurement of Duran ring area published in 1995 [12] that was 40% smaller than that reported in 1998 [32] even though some of the same patients were used in both studies. Other factors may also impact substantially on the measurement of mitral dynamics. The anatomical definition of the annulus in echocardiographic images is only defined as the leaflet "hinge point," which may differ from the true annulus that is visually identifiable and where myocardial markers or piezoelectric miniature crystals are implanted. In addition, planar geometry of the annulus is assumed in some investigations, but the annulus is actually "saddle" or "ski jump" shaped [5, 27, 35]. Individual patient variability, the presence or absence of cardiac pathology, andimportantlydifferences in LV loading conditions and inotropic state could also be responsible for some of the disagreement. Besides, "control" subjects are not necessarily "normal" individuals. In an experimental setting, this variability is eliminated to a large degree and normal hearts can be analyzed but species differences must still be considered when comparing results across different experimental models.
Definition of cardiac cycle timing markers can also contribute to differences in measured end-diastolic and end-systolic annular areas as these definitions are either not standardized (Table 1) nor explicitly mentioned in most studies. Differences in image acquisition rate can limit the number of time points at which annular area is determined; therefore annular area reduction, if calculated from maximum to minimum area, may be affected. Experimental studies have shown that factors affecting cardiac function (LV preload, LV afterload, heart rate, rhythm, and contractile state) also clearly influence annular dynamics [1, 15, 19, 22] and therefore inconsistencies may not be so surprising when different contractile state and hemodynamic conditions are taken in account. For example, Cosgrove ring annular area reduction was reported to be 7% and 16% immediately postoperatively and at 9 months, respectively [10], but this difference could reflect myocardial dysfunction in the early period after cardiopulmonary bypass rather than measurement error. Annular dynamics should thus be interpreted in the overall context of the investigation being conducted to avoid misinterpretation.
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Proper imaging of the mitral annulus in pathologic states such as patients with dilated cardiomyopathy [5, 23, 36] also adds to our understanding of cardiac pathophysiology and the pathogenesis of mitral regurgitation. In addition, echocardiographically determined mitral annular velocity has recently been used as an indicator of systolic [37] and diastolic [38] LV function, and advances in echocardiographic techniques such as Doppler proximal flow convergence [27, 39] are bound to contribute further to our knowledge of mitral annular physiology. It is clear that precise measurement of annular dynamics would yield more detailed knowledge of annular physiology, which may translate directly to medical and surgical management of patients. This review underscores the need for standardization of methods, control of hemodynamic variables and loading conditions, and adjustment for individual subject characteristics to allow for valid comparisons. Future advancements in 3-D echocardiography may provide better measurements than what is currently available but validation studies are needed. An ideal validation experiment would consist of comparing 3-D TEE or epicardial 3-D echocardiographic data with measurements determined using 3-D marker cinefluoroscopy in the same animals. Additionally, new techniques such as MRI RF tagging or MR phase contrast pulse sequence imaging, which allows for tracking of discrete cardiac sites throughout the cardiac cycle, may offer other avenues to investigate the dynamics of the human mitral annulus in a noninvasive yet accurate manner.
| Acknowledgments |
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| References |
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