Editorials |
From the Division of Cardiovascular Diseases (C.P.A.), Mayo Clinic Arizona; and the Cardiovascular Biophysics Laboratory (S.J.K.), Cardiovascular Division, Washington University School of Medicine, St. Louis, Mo.
Correspondence to Dr. Christopher P. Appleton, Division of Cardiovascular Diseases, Mayo Clinic Arizona, 13400 E Shea Blvd, Scottsdale, AZ 85259. E-mail cappleton{at}mayo.edu
Key Words: editorials heart failure left atrial diastolic function
| Introduction |
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Article see p 10
Segmental LV deformation analysis for calculating contractile parameters such as strain and strain rate is now possible using noninvasive echo-Doppler techniques.2 It has been reported that LA systolic and diastolic function can also be assessed using these Doppler strain techniques.4–6 Although LA enlargement increases with the severity of diastolic dysfunction,7 the ability of LA volume measurements to discriminate asymptomatic LV diastolic dysfunction from early DHF heart failure has not been possible. However, the concept that an alteration in LA function or stiffness may indicate this change is appealing.
| The Present Study |
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There is much to be commended in this effort. The incorporation of hemodynamic data are increasingly rare in clinical studies and cannot be adequately replaced by surrogates such as Doppler E/e' ratios. The use of cardiac filling pressures with indices of LA function (strain and strain rate) to calculate LA stiffness is novel and worth exploring. The finding of similar increases in LA volume in patients with normal LVEF and diastolic dysfunction who had markedly different mean LA pressure is intriguing, goes against conventional wisdom and merits further investigation; although a detailed explanation of the methods used for LA volume should always be provided. Data which would have been helpful includes conventional mitral and pulmonary venous flow velocity variables. In addition, as seen in Figure 2, correlations and ROC curves do not always translate into clinical usefulness as a LA stiffness of 2 mm Hg, even if accurate, was associated with a PA systolic pressure range of 25 to 55 mm Hg.
In a larger sense the work Kurt et al8 points out the problem we, as investigators, have of trying to solve an important clinical issue by studying a single part (in this case the left atrium) of an integrated cardiovascular system in which the actions of all parts are coupled and affect each other. To fully understand the observations in the present work and help plan future research, it may be helpful to step back, consider how the entire heart works as it fills, and review the kinematic relationships between the left atrium and left ventricle that have already been established.
| The Constant Volume Heart |
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If the left ventricle is a large energy source, and the left atrium a small one that acts only briefly, and both chambers (but largely the ventricle) are constantly affecting the behavior of each other in a reciprocal fashion, is there a good time to study inherent atrial properties? Yes, most logically it would be during diastasis. There is no transmitral flow, there is no wall motion, and the atrium and the ventricle form a single chamber at the same pressure and at a fixed volume (see left ventricular angiogram, Movie 3). Diastasis defines the LV equilibrium volume,13 and by the constant volume property, it defines the equilibrium volume for the left atrium as well. To clarify, during diastasis, all forces are balanced (but not zero) so there is no wall motion and no transmitral flow. Hence the diastatic pressure-volume (P-V) relation can be differentiated from the end-diastolic P-V relation, which is conventionally used to determine LV stiffness.14
With the earlier discussion as background, and emphasizing that during the cardiac cycle the left heart generates external work (energy source) versus being the recipient of work (energy sink) let us examine the indexes used to characterize LA function—particularly LA diastolic function and dysfunction.
| Left Atrial Ejection Fraction |
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| LA Strain and Strain Rate |
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LA strain with LA contraction is a measure of LA systolic function relative to the load the LA faces as it pulls the mitral annulus upward and distends the LV while it simultaneously generates retrograde flow into the pulmonary veins. As discussed with LAEF it is confounded by both LV and pulmonary properties.
| Hemodynamic Measurements |
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| LA Stiffness |
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To underscore the limitations of viewing LA strain during LV systole and LA stiffness as atrial properties—consider the physiologically symmetrical measurement of placing the Doppler sample volume for strain measurement in the LV wall, just below the mitral annulus during atrial systole. A peak strain and strain rate and stiffness for the LV can be measured but are clearly a consequence of atrial systole pulling up on the mitral annulus and ventricular myocardium. Labeling the obtained values as "LV diastolic function indexes," because they occur during LV diastole, when they are caused by the work of LA systole, has obvious limitations.
| Concluding Remarks |
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Because of its increasing clinical importance DHF in patients with normal LVEF will remain a field of intense scrutiny and clinical relevance. Further advances in the use of noninvasive imaging (echocardiography, cardiac MRI, cine-CT) complemented by modeling of atrial-ventricular coupling in the context of the constant-volume attribute may help identify intrinsic LA properties that may be contributors to the development of DHF. It is also conceivable that as computer models of LV, 2-chamber and 4-chamber heart function become more tractable16–19 new physiological relations will be found that more fully characterize the role of intrinsic LA function in DHF. Ultimately, imaging and modeling in synergy, which includes the arterial system,20 will lead to earlier diagnosis of DHF and implementation of therapy. Although skeptics remain whether diastolic function is the primary disorder in DHF,21 and the role of atrial remodeling and dysfunction has been considered,22 continued investigation at the cellular and molecular level will help determine the ultimate causes of changes in LV structure and function that result in DHF.3
| Acknowledgments |
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Sources of Funding
Dr Appleton is supported in part by the Reid-Family Trust. Dr Kovács is supported in part by Bames-Jewish Hospital Foundation and Alan A. and Edith Wolff Charitable Trust.
Disclosures
None.
| Footnotes |
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The online-only Data Supplement is available at http://circimaging.ahajournals.org/cgi/content/full/2/1/6/DC1.
| References |
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8. Kurt M, Wang J, Torre-Amione G, Nagueh SF. Left atrial function in diastolic heart failure. Circulation Imaging. 2009; 2: 10–15.[CrossRef]
9. Bowman AW, Kovács SJ. Assessment and consequences of the constant-volume attribute of the four-chambered heart. Am J Physiol Heart and Circ Physiol. 2003; 285: H2027–H2033.
10. Waters EA, Bowman AW, Kovács SJ. MRI determined left ventricular "crescent effect": a consequence of the slight deviation of the contents of the pericardial sack from the constant-volume state. Am J Physiol Heart Circ Physiol. 2005; 288: H848–H853.
11. Riordan M, Kovács SJ. Relationship of pulmonary vein flow to LV short-axis epicardial displacement in diastole: model-based prediction with in-vivo validation. Am J Physiol Heart Circ Physiol. 2006; 291: H1210–H1215.
12. Bowman AW, Kovács SJ. Left atrial conduit volume is generated by deviation from the constant-volume state of the left heart: an MRI-echocardiographic study. Am J Physiol Heart Circ Physiol. 2004; 286: H2416–H2424.
13. Zhang W, Chung CS, Shmuylovich L, Kovács SJ. Viewpoint: is left ventricular volume during diastasis the real equilibrium volume and, what is its relationship to diastolic suction? J Appl Physiol. 2008; 105: 1012–1014.
14. Zhang W, Kovács SJ. The diastatic pressure-volume relationship is not the same as the end-diastolic pressure-volume relationship. Am J Physiol Heart Circ Physiol. In press [doi:10.1152/ ajpheart. 00200.2008.]
15. Lisauskas JB, Singh J, Courtois M, Kovács SJ. The relation of the peak Doppler E-wave to peak mitral annulus velocity ratio to diastolic function. Ultrasound Med Biol. 2001; 27: 4:499–507.
16. Modeling of diastole. In: Kovács SJ, Meisner JS, Yellin EL, eds. Diastolic Function and Dysfunction. Chapter 4: Cardiology Clinics of North America. Orlando, FL: WB Saunders & Co; 2000:18;3: 459–490.
17. Kovács SJ, McQueen MD, Peskin CS. Modeling cardiac fluid dynamics and diastolic function. Phil Trans Royal Soc A. 2001; 359: 1299–1314.[CrossRef]
18. Kerckhoffs RCP, Narayan SM, Omens JH, Mulligan LJ, McCulloch AD. Computational modeling for bedside application. Heart Failure Clin. 2008; 4: 371–378.[CrossRef]
19. Kerckhoffs RCP, Neal M, Gu Q, Bassingthwaighte JBB, Omens JH, McCulloch AD. Coupling of a three-dimensional finite element model of cardiac ventricular mechanics to lumped systems models of the systemic and pulmonic circulation. Ann Biomed Eng Jan. 2007; 35: 1–18.
20. Kawaguchi M, Hay I, Fetics B, Kass DA. Combined ventricular systolic and arterial stiffening in patients with heart failure and preserved ejection fraction. Circulation. 2003; 107: 714–720.
21. Burkhoff D, Maurer MS, Packer M. Heart failure with a normal ejection fraction. Is it really a disorder of diastolic function? [editorial]. Circulation. 2003; 107: 656–658.
22. Melenovsky V, Borlaug BA, Rosen B, Hay I, Ferruci L, Morell CH, Lakatta EG, Najjar SS, Kass DA. Cardiovascular features of heart failure with preserved ejection fraction versus nonfailing hypertensive left ventricular hypertrophy in the urban baltimore community: the role of atrial remodeling/dysfunction. J Am Coll Cardiol. 2007; 49: 198–207.
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