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J Am Coll Cardiol, 1998; 32:1187-1193 © 1998 by the American College of Cardiology Foundation |
a Royal Brompton Hospital, London, England, United Kingdom
Manuscript received February 10, 1998; revised manuscript received June 23, 1998, accepted July 9, 1998.
Address for correspondence: Dr. Derek G. Gibson, Royal Brompton Hospital, Sydney Street, SW3 6NP, London, United Kingdom
| Abstract |
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Background. It is not clear whether these right-sided abnormalities are due to primary RV disease or are secondary to restrictive physiology on the left side of the heart. The latter regresses with angiotensin-converting enzyme inhibition (ACE-I).
Methods. Transthoracic echo-Doppler measurements of left- and right-ventricular function in 17 patients with systolic left ventricular (LV) disease and restrictive filling before and 3 weeks after the institution of ACE-I were compared with those in 21 controls.
Results. Before ACE-I, LV filling was restrictive, with isovolumic relaxation time short and transmitral E wave acceleration and deceleration rates increased (p < 0.001). Right ventricular long axis amplitude and rates of change were all reduced (p < 0.001), the onset of transtricuspid Doppler was delayed by 160 ms after the pulmonary second sound versus 40 ms in normals (p < 0.001) and overall RV filling time reduced to 59% of total diastole. Right ventricular relaxation was very incoordinate and peak E wave velocity was reduced. Peak RV to right atrial (RA) pressure drop, estimated from tricuspid regurgitation, was 45 ± 6 mm Hg, and peak pulmonary stroke distance was 40% lower than normal (p < 0.001). With ACE-I, LV isovolumic relaxation time lengthened, E wave acceleration and deceleration rates decreased and RV to RA pressure drop fell to 30 ± 5 mm Hg (p < 0.001) versus pre-ACE-I. Right ventricular long axis dynamics did not change, but tricuspid flow started 85 ms earlier to occupy 85% of total diastole; E wave amplitude increased but acceleration and deceleration rates were unaltered. Values of long axis systolic and diastolic measurements did not change. Peak pulmonary artery velocity increased (p < 0.01).
Conclusions. Abnormalities of RV filling in patients with heart failure normalize with ACE-I as restrictive filling regresses on the left. This was not due to altered right ventricular relaxation or to a fall in pulmonary artery pressure or tricuspid pressure gradient, but appears to reflect direct ventricular interaction during early diastole.
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| Methods |
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Twenty-one normal subjects, age 58 years (SD 11 years), served as controls. They were studied by the same operators and over the same time period as the study patients. None had a history of shortness of breath, hypertension, valvular or ischemic disease or pulmonary disease.
All patients were studied at rest. We obtained cross sectional two-dimensional (Andover, Massachusetts) guided M modes and Doppler velocities using a Hewlett Packard Sonos 1500 system with a 2.5 MHz transducer. With the patient lying in the left semilateral position, M modes of the LV minor axis were recorded from the parasternal long axis view with the cursor at the tips of mitral valve leaflets. Long axis M-mode recordings of RV free wall were obtained with the cursor positioned at the tricuspid valve annulus (2). All records were made during quiet expiration. Transmitral and transtricuspid Doppler flow velocities were obtained using the same echocardiograph within 5 min of one another with the sample volume at the tips of mitral and tricuspid valve leaflets in the apical four-chamber view. Aortic and pulmonary outflow tract velocities were recorded with the pulsed-Doppler sample volume at the valve tips from the parasternal short axis view and apical four-chamber view, respectively. Continuous wave Doppler traces of mitral and tricuspid regurgitation were recorded using a Doptek system (Colchester, UK), with a 2.5 MHz nonimaging transducer. The apexcardiogram was recorded using Cambridge equipment (time constant 4 s). An electrocardiogram and phonocardiogram were recorded superimposed on all M-mode, Doppler and pulse traces which were photographically recorded at a paper speed of 100 mm/s. M-mode traces were later digitized off line using a dedicated computer program (4).
Measurements. End diastolic LV dimensions were taken at the onset of the q wave of the electrocardiogram (ECG), and end systolic dimensions were taken at the first high-frequency component of the aortic component of the second heart sound (A2) of the phonocardiogram. Left ventricular fractional shortening was estimated as the percentage fall in dimension during ejection with respect to end diastolic dimension. Isovolumic relaxation time was measured from the mitral valve echogram as the time interval between A2 and the onset of mitral cusp separation. Right ventricular, long axis total excursion was measured from the innermost point (at end systole) to the outermost point (at end diastole). The A wave was taken as the extent of additional long axis motion between the end of the P wave of the ECG and the onset of the succeeding systole. Incoordinate relaxation was measured as the amplitude of abnormal movement after A2 or P2 (the pulmonary second sound), during early diastole, before the onset of mitral or tricuspid flow motion, respectively, towards the ventricular apex being expressed as positive and toward the atria as negative. The identities of A2 and P2, the aortic and pulmonary components of the second heart sound, were routinely checked against the corresponding valve closure artifact on the aortic and pulmonary Doppler flow velocity traces. From the digitized traces, peak LV minor axis and RV, long axis shortening (in systole) and lengthening (in diastole) were measured as well as the time interval between the q wave and peak shortening rate and the second heart sound, A2 or P2, and peak lengthening rate.
From the transmitral and transtricuspid pulsed-Doppler traces, peak early and late diastolic filling velocities were measured and the E/A ratio calculated. Total LV and RV filling times were measured as the total duration of transmitral and transtricuspid flow, respectively, and the ratio of each to total diastolic time calculated. Total diastolic time itself was measured as the period between the onset of P2 and the onset of the q wave of the ECG of the succeeding beat. Mitral and tricuspid E-wave acceleration times were measured from onset to peak velocity, and mean acceleration rates as peak velocity divided by corresponding acceleration time. Deceleration times and rates were measured in the same way on both sides of the heart, the former being derived by extrapolation if the A wave was partially superimposed on the descending limb of the E wave. A wave velocity was measured with respect to baseline. Pressure gradients in mm Hg·cm1 were calculated as 0.075 x acceleration rate in m·s2. Right ventricular to RA systolic pressure drop was measured from the peak tricuspid regurgitation velocity as assessed by continuous wave Doppler and presented in mm Hg, using the simplified Bernoulli equation. Peak LV and RV outflow tract velocities were measured from the pulsed-Doppler trace. Aortic and pulmonary total ejection times were measured from the same trace, and stroke distance was derived. The percentage of end diastolic A wave amplitude to total pressure amplitude was measured from the apexcardiogram.
Statistics. Values are expressed as mean ± SD. Patients values before treatment with ACE-I were compared with controls using unpaired Student t test. Patient data before and after treatment were compared using a paired t test. In view of multiple t tests, a Bonferroni correction was implemented and the statistical significance was taken to apply when p value was less than 0.017.
| Results |
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On the right side (Fig. 1)
The RVRA peak systolic pressure drop fell by 15 mm Hg, although all aspects of systolic long axis function (total excursion, peak shortening rate and time interval between q wave and peak shortening rate) were unaltered (Tables 2 and 3). However, there were major changes in transtricuspid flow velocities. The onset of the E wave occurred 85 ms earlier with respect to P2, peak E wave velocity more than doubled; deceleration time was prolonged but neither mean acceleration rate nor deceleration rate changed. Peak A wave velocity was also unchanged, so that E/A ratio doubled. The shortening of the time interval P2 to the onset of tricuspid flow meant that the extent of long axis lengthening before the onset of flow fell, but peak long axis lengthening rate itself was unchanged, as was the timing of the peak value that remained earlier than normal with respect to P2. Total tricuspid flow period more than doubled, although diastolic time itself increased only by 20% so that there was a marked increase in the ratio of flow time to total diastolic time (p < 0.001). Peak pulmonary artery velocity also increased (Table 3).
| Discussion |
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Right-side events also changed strikingly with ACE-I. As would be expected from a fall in LA pressure, the systolic pressure drop across the tricuspid valve fell by 15 mm Hg. In spite of this, the dynamics of right-side long axis did not change. The main changes were in the pattern of transtricuspid flow. The onset became earlier, and its overall duration increased by over 100 ms, so that it came to occupy 80% of the total diastolic time. E wave amplitude increased, but neither mean acceleration rate nor local pressure gradient changed. A wave amplitude was unaltered, but E/A ratio increased. ACE-I thus led to a normalization of RV filling, the changes being largely in the opposite direction to those occurring on the left side.
Mechanisms. There are a number of possible mechanisms for these right-side abnormalities. In any population of patients with LV disease, additional involvement of the right ventricle by the same or a related disease process will be present to a variable extent in individual patients (6). In addition, the right heart is subject to abnormal loading conditions caused by elevation of the LA pressure transmitted via the pulmonary artery and also of RA pressure (7). A low stroke volume may be imposed on it by severe left-side disease. Finally, the right side is subject to ventricular interaction mediated either via the pericardium or the septum (810). Some of these possible mechanisms were seen in the present series of patients. The peak systolic pressure drop supporting tricuspid regurgitation was increased under control conditions and fell with treatment. The reduced extent of RV, long axis shortening is compatible with additional RV disease rather than abnormal loading because neither its extent nor its velocity was affected as RV to pulmonary artery pressure difference fell.
The most striking abnormality under control conditions was in the timing of tricuspid flow so that its onset was more than 100 ms later than normal, leading to marked asynchrony when compared to early diastolic lengthening of the RV long axis. Neither the timing nor the velocity of this lengthening was affected by ACE-I, making a primary disturbance of RV relaxation a very unlikely cause. As the timing of flow reverted toward normal, the extent of asynchrony regressed. Once the transtricuspid E wave pressure gradient developed, it was normal under control conditions, and was slightly affected by treatment. A change in the magnitude of the pressure gradient therefore was not the cause of abnormal flow. An increase in peak tricuspid regurgitation pressure is always accompanied by prolongation of overall RV systole by approximately 10 ms for each 10 mm Hg peak pressure increase (11). This effect was demonstrated with ACE-I in our patients with a fall in the interval from P2 to the end of regurgitation by 15 ms, but it was much too small to explain the change in the timing of flow, thus excluding another possible mechanism. There was a striking return of the timing of transtricuspid flow towards normal, however, as the restrictive filling pattern on the left side of the heart resolved by treatment. This was apparent not only from group values but from those in individual patients (Fig. 2). It occurred as the left-side pressure gradient fell from supranormal values before treatment to abnormally low volumes afterward. It seems, therefore, that the likeliest explanation for our findings is an early diastolic ventricular interaction and we hypothesize that high left-side pressures may delay the onset of a forward pressure gradient and hence atrioventricular diastolic flow on the right side.
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Conclusions. Our results indicate that a restrictive filling pattern of the left side of the heart is often associated with striking delay in the onset of transtricuspid flow on the right side, with secondary incoordination and reduction in peak E-wave velocity. Right ventricular disease or a primary disturbance of RV relaxation are unlikely causes. Their regression along with that of the restrictive filling pattern on the left side with ACE-I strongly suggests that right-side filling abnormalities may be directly related to high early diastolic pressures in the left ventricle. The time relations between the two within the cardiac cycle seem to indicate a direct ventricular interaction rather than the simple effect of secondary pulmonary hypertension. We suggest that the implications of these right-side abnormalities merit further study, particularly with respect to their relation to fluid retention, exercise tolerance and heart rate variability. Their prompt regression with ACE-I provides further evidence of the comprehensive effects of these remarkable drugs.
| Acknowledgments |
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| Footnotes |
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| References |
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