(Hypertension. 1999;33:811-815.)
© 1999 American Heart Association, Inc.
Scientific Contributions |
From the Departments of Physiology and Biophysics (J.F.C., R.L.S., D.J.D., K.C., H.L.M.), Emergency Medicine (R.L.S.), and Surgery (D.J.D.), University of Mississippi Medical Center, Jackson; and the Institute of Physiology (J.-P.M.), University of Fribourg (Switzerland).
Correspondence to Joan F. Carroll, PhD, Department of Integrative Physiology, University of North Texas Health Science Center at Fort Worth, 3500 Camp Bowie Blvd, Fort Worth, TX 76107-2699. E-mail jcarroll{at}hsc.unt.edu
| Abstract |
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0.05) and left ventricular
hypertrophy (1.37±0.07 versus 0.98±0.03 g dry weight,
P
0.05). Compliance was assessed with the isolated
heart preparation by analyzing the passive end-diastolic
left ventricular pressure-volume relationship. The
pressure-volume relation was fit to an exponential function by
regression analysis; results showed that the modulus of
stiffness was greater in obese than in lean rabbits (1.21±0.16 versus
0.83±0.05, P
0.05), indicating that
diastolic compliance was reduced. Computer simulation
analyses suggested that an isolated reduction in
diastolic compliance may contribute to elevated cardiac
filling pressures and exercise intolerance. These data suggest that
diastolic compliance is reduced early in the development of
obesity and may be an important component in the reduction of cardiac
reserve in obesity.
Key Words: heart stroke volume obesity computer modeling diastolic pressure-volume relationship
| Introduction |
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Diastolic dysfunction may be simply described as a condition in which diastolic filling is impeded. However, diastolic filling of the left ventricle is a complex process determined by the interaction of several factors, including active ventricular relaxation and passive properties influencing left ventricular compliance. Active relaxation is related to calcium reuptake by the sarcoplasmic reticulum, whereas passive ventricular filling properties are determined by ventricular wall thickness, the dimensions of the ventricular cavities, and the structural properties of the cardiac tissue itself. A few studies have attempted to examine the diastolic pressure-volume relationship,5 6 and the data suggested that morbidly obese patients exhibit abnormalities in diastolic filling, with or without the presence of hypertension or cardiac hypertrophy.7 8
Although there is evidence that diastolic filling is altered in obesity,7 it is difficult to determine from clinical studies what role altered diastolic compliance plays in diastolic dysfunction. Little is known about the mechanisms underlying abnormal diastolic function in obesity or the relative contributions of decrements in active versus passive relaxation to filling abnormalities. In addition, little is known about how quickly diastolic dysfunction becomes manifest during the development of obesity. Therefore, our purpose was to examine the passive end-diastolic pressure-volume relationship in isolated hearts of obese and control rabbits to determine the presence and extent of obesity-related decrements in passive diastolic compliance. In addition, we used computer models of circulatory function to predict systemic effects resulting from reduced compliance both at rest and during exercise.
| Methods |
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Blood Pressure Measurement and Surgical Procedures
Acute blood pressure measurement and surgical procedures for
heart excision have been described previously.10 Briefly,
blood pressure in the conscious, unanesthetized rabbit was
measured directly from a central ear artery catheter for 60 to 90
minutes. A small arterial blood sample was then withdrawn
for measurement of hematocrit and plasma protein. After blood sampling,
general anesthesia was induced with 4% to 5% isoflurane
with an oxygen flow of 1 L/min administered with a face mask. The heart
was then subjected to cardioplegic arrest and prepared for the
Langendorff preparation. First, venous return was stopped by tying
sutures around the superior and inferior vena cavae.
Pressure was then placed on an aortic ligature, and the heart was
arrested by infusing cold (4°C) Euro-Collins solution retrograde into
the aortic root. The mitral valve was excised, and a latex balloon
containing a high-fidelity micromanometer was
positioned in the left ventricle for pressure measurements.
Isolated Heart Protocol
The relationship between left ventricular
end-diastolic pressure and volume was determined with the
isovolumic Langendorff isolated heart preparation as previously
described.10 Briefly, signals from the high-fidelity
micromanometer within the latex balloon were
sampled 6 times each minute for 6 seconds each to detect peak pressure,
end-diastolic pressure, peak +dP/dt, and peak dP/dt for
each burst. Heart function was allowed to stabilize for approximately
30 minutes, after which control measurements of peak pressure,
end-diastolic pressure, and peak +dP/dt and dP/dt were
recorded. Coronary flow was also determined by a timed
measurement of coronary effluent. After stabilization, 0.3 mL
fluid was added to the latex balloon every 3 minutes until the
end-diastolic pressure was approximately 20 mm Hg.
Reported values were the average of measurements taken during the final
40 seconds of each 3-minute period when function had stabilized.
Analytic Methods
Hematocrit was measured in duplicate with a microhematocrit
centrifuge (Adams Autocrit Centrifuge, Clay Adams) and
a microcapillary tube reader. Plasma protein was measured by
refractometry.
Statistical and Computer Simulation Analyses
Descriptive data comparing lean and obese rabbits included body
weight, blood pressure, heart rate, left and right dry
ventricular weights, and plasma hematocrit and protein.
These variables were analyzed by unpaired t
tests, with significance accepted at the 0.05 level.
Compliance was assessed by analyzing the passive end-diastolic left ventricular pressure-volume relationship. To enable comparisons among hearts, the volume at which end-diastolic pressure equaled zero was designated as the zero volume in each heart. Pressure data at increments of 0.3 mL up to a volume of 1.5 mL were then analyzed with a repeated-measures multivariate analysis of variance. When there was a significant groupxvolume interaction, pressure data at each volume were analyzed using two-sample t tests with a Bonferroni correction (P=0.01). Similar analyses were performed for peak +dP/dt and dP/dt values. In a second analysis, the pressure-volume relation was fit to an exponential function by regression analysis.11 Volumes were normalized to left ventricular weight in order to incorporate both heart size and muscle thickness and minimize their influence. From the derived equations, the average modulus of stiffness was compared between lean and obese rabbits with an unpaired t test. Significance was accepted at the 0.05 level. All data are expressed as mean±SEM.
It is difficult to interpret isolated organ findings in the context of the whole animal, so experimental results were also examined by systems analysis using a computer model of circulatory function. We used a derivative of the well-established circulatory model of Guyton and colleagues12 and a previously published model of cardiac diastolic dynamics.13 This model uses known physiological parameter interrelationships in continuous feedforward and feedback loops to predict values of a variety of hemodynamic variables over a wide range of perturbations. In this model, cardiac output is determined from factors that influence venous return and the cardiac Starling curve, with diastolic compliance (both active and passive) contributing to resistance to cardiac filling. Within this framework, changes in passive diastolic compliance seen experimentally were incorporated into the model, and the theoretical effects on cardiac output, urinary output, atrial pressure, and extracellular fluid volume were predicted. The effect of increased stress on a heart with reduced compliance was also simulated in an exercise experiment, in which exercise was simulated by a general sympathetic discharge with increases in cardiac strength and vascular tone. Cardiac output and right atrial pressure values during simulated exercise were compared in models with and without compliance changes.
| Results |
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0.05). Obesity was associated with resting
tachycardia and mild hypertension. Resting heart rates were
19% higher in obese than lean rabbits (243±12 versus 204±12 bpm,
P
0.05), and mean arterial pressure
measurements averaged 96±2 mm Hg in obese rabbits compared with
90±2 mm Hg in lean rabbits (P=0.08). Although
hypertension in this experiment was modest, in other experiments using
this model we have demonstrated increases in blood pressure averaging
10% to 21%.10 14 15 16
Obese rabbits also developed cardiac hypertrophy. Dry left
ventricular weights were 40% heavier in obese than lean
rabbits (1.37±0.08 versus 0.98±0.03 g, P
0.05), and dry
right ventricular weights were 57% heavier in obese
rabbits (0.66±0.06 versus 0.42±0.03 g, P
0.05).
Hematocrit measurements were higher in obese rabbits (0.41±0.01 versus
0.36±0.01, P
0.05), as were plasma protein levels
(5.6±0.1 versus 5.4±0.1 g/dL, P
0.05).
Figure 1A illustrates the
end-diastolic pressure-volume relationship when data were
calculated to yield a volume of zero when end-diastolic
pressure was zero. The mean volume at which end-diastolic
pressure equaled zero did not differ between lean and obese hearts
(0.73±0.02 versus 0.73±0.02 mL, respectively; P>0.05).
However, there was a significant groupxvolume interaction
(P
0.05). Comparison of lean and obese hearts indicated
significant pressure differences at 0.9 mL (4.8±0.4 versus
9.1±1.3 mm Hg, respectively), 1.2 mL (6.0±0.4 versus
12.3±2.0 mm Hg, respectively), and 1.5 mL (7.4±0.6 versus
13.8±2.7, respectively) (all P
0.01).
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Figure 1B illustrates the pressure-volume relationship in lean
and obese rabbits fit to an exponential function where left
ventricular volumes were normalized for dry left
ventricular weight. From the derived equations, the average
modulus of stiffness was 0.83±0.05 in lean rabbits and 1.21±0.16 in
obese rabbits (P
0.05), indicating that
diastolic compliance is reduced early in the development of
obesity in this animal model. Coronary flow did not differ
between lean and obese rabbits (11.0±0.8 versus 8.7±1.0 mL/g,
respectively; P>0.05). There was no significant difference
in peak +dP/dt and dP/dt between lean and obese rabbits across the
volumes tested.
Computer Simulation Analyses
In computer simulations, we determined theoretical systemic
effects associated with the in vitro reduction in compliance. Figure 2A illustrates the effect of reduced
compliance in the resting state. Initial decreases were seen in cardiac
output and urinary output, whereas right atrial pressure and
extracellular fluid volume increased. In the long term, cardiac
output returned toward normal at the cost of further fluid retention
and higher cardiac filling pressure. Figure 2B illustrates the
effect of decreased diastolic compliance in a model made to
simulate moderate exercise. Compared with a model without compliance
changes, overall cardiac output and systemic flow were reduced during
exercise, despite further increases in filling pressure. Although this
result has been seen previously in live obese animals,17
these in vitro and computer simulation studies suggest that reduced
diastolic compliance may be a major factor in the abnormal
hemodynamic response to exercise in obesity.
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| Discussion |
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The hypertension observed in this study was modest, averaging 6 mm Hg higher (7%) in obese than lean rabbits; the increase in resting heart rate in obese rabbits averaged 19%. Although the degree of resting tachycardia in the present study was similar to that in earlier studies using this model, we have previously measured greater obesity-related increases in blood pressure (eg, 10% to 21%).10 14 15 16 Still, we believe that this is an underestimation of the chronic elevations in blood pressure and heart rate in obese rabbits. We have preliminary data demonstrating that blood pressure and heart rate measured 18 h/d with telemetry averaged 24% and 38% higher, respectively, in obese than lean rabbits (n=4 each group).
The effects of obesity on heart function in humans are often studied noninvasively with echocardiography.8 18 However, noninvasive methods such as echocardiography are limited in the extent to which mechanisms underlying these abnormalities can be identified. Animal models of obesity also have yielded little concrete information on the potential role of obesity in altering diastolic compliance, because of either contradictory results19 20 or use of an animal model with many characteristics that are clearly different from human obesity.19 20 21
The rabbit model has been shown to be useful in the study of
obesity-related hypertrophy. We have demonstrated that
obesity in this model was associated with ventricular
hypertrophy that was mainly due to myocyte
hypertrophy and not fatty infiltration.14
Ventricular hypertrophy is still evident when
dry ventricular weight is normalized for lean body mass.
Using data from Dwyer et al,22 we estimated lean
body mass of animals in the present experiment and calculated
ratios of dry left ventricular weight to lean body mass of
0.29±0.01 and 0.39±0.01 for lean and obese rabbits, respectively
(P
0.05). We also used echocardiography
to study the geometric nature of obesity-related
hypertrophy and demonstrated that there was a combined
concentric and eccentric remodeling, with increases in both wall
thickness and chamber diameter. Functionally, obese rabbits showed an
increase in peak atrial flow velocity (A wave) and an increase in the
ratio of peak atrial to peak early flow velocity
(A/E).16 Although early diastolic filling
rate (E wave) did not differ between lean and obese rabbits, there was
a slightly larger stroke volume in obese rabbits, necessitating a
compensatory increase in the contribution of atrial filling to achieve
an adequate end-diastolic volume.16 In
addition to altered rates of filling late in diastole, we
have demonstrated in the present study that reduced passive
diastolic compliance is another important factor in
obesity-related abnormalities of diastolic filling.
We noted in the present investigation that peak +dP/dt and dP/dt values did not differ significantly between lean and obese hearts. This is not incompatible with a reduction in compliance because the rate and extent of relaxation are two different properties of the myocardium. Rate of relaxation, as illustrated by dP/dt, affects the pressure-volume relation early in diastole because it affects the atrioventricular pressure gradient and ventricular filling during the rapid phase of filling.23 In agreement with these data, we have found echocardiographic evidence that early diastolic filling is not altered in obesity.16 In contrast, the extent of relaxation is the state of the myocardium after relaxation has been completed, and this determines equilibrium length and volume of the left ventricle. If the extent of relaxation is impaired, as the present experiment suggests, equilibrium volumes will be smaller and end-diastolic pressures higher.
Ventricular hypertrophy may affect the extent of relaxation because the associated decrease in capillary density and coronary vasodilator reserve results in ischemia.23 Although coronary flow was not significantly different between lean and obese hearts in the present study, it did appear somewhat reduced in obese hearts and may have contributed to reduced compliance. Hypertrophy may also reduce uptake of calcium by the sarcoplasmic reticulum. In addition to slowing the rate of relaxation, this may affect the extent of relaxation if greater amounts of calcium remain in the cytoplasm at end-relaxation. Future work is needed to determine whether function of the sarcoplasmic reticulum is reduced in obesity.
Another contributing factor to decreased diastolic compliance in obesity may be collagen deposition. We have shown that interstitial and perivascular collagen is significantly increased in obese rabbit hearts.24 Although this has been identified as a factor in increased diastolic stiffness in renovascular hypertension and pressure-overload models of hypertension, increased concentrations of collagen have not been identified in obesity. The initiating event in myocardial fibrosis is not clear but may be associated with neural or humoral factors such as the renin-angiotensin system.25 Although we have determined that obese rabbits demonstrate an increase in resting plasma renin activity,14 further work is necessary to determine whether angiotensin II plays a role in development of obesity-related myocardial fibrosis.
Using the present experimental results in a computer simulation, we showed that under resting conditions, an isolated reduction in ventricular compliance resulted in near-normal cardiac output. However, cardiac output is maintained at the expense of increased extracellular fluid volume and increased atrial filling pressure. Increased volume together with reduced compliance can result in an abnormally increased filling pressure during maneuvers that increase central blood volume such as passive supine leg raising and supine exercise.3 Furthermore, our simulation also demonstrated that increased diastolic stiffness alone can cause reduced cardiac output and systemic flow during exercise despite increased filling pressure. This suggests that increases in extracellular fluid volume and filling pressure can maintain heart function at rest but that they are insufficient to maintain adequate pumping capacity during periods of increased demand. In this respect, the computer simulations are consistent with experimental studies. In obese dogs, we have previously shown abnormal cardiovascular responses to exercise that were consistent with a defect in diastolic function.17 In these animals obesity was associated with increased resting left atrial pressure, an abnormal increase in left atrial pressure during exercise, and frank exercise intolerance. Our computer simulation studies suggest that an isolated reduction in diastolic compliance can be an important component in this reduction of cardiac reserve in obesity.
In the present study, we used the Langendorff isolated heart preparation to assess passive diastolic compliance. This method has been criticized for its lack of reflex and humoral background and feedback. However, this feature is also one of the great strengths of the method in that it allows study of intrinsic heart function without interference from neurohumoral sources. In our analyses, we used both nonnormalized (Figure 1A) and normalized (Figure 1B) pressure-volume data to assess chamber stiffness. Although normalization of data may produce misleading information,26 both analyses suggested the same conclusion regarding early development of diastolic dysfunction in obesity. Nevertheless, determination of the stress-strain relationship and a myocardial stiffness constant would add another dimension to the characterization of left ventricular function and allow further inferences regarding myocardial functional and structural defects.
In summary, we used the rabbit model of obesity to identify reduced diastolic compliance as a potential factor in abnormalities in diastolic filling seen in obesity. Using the isolated heart technique, we demonstrated that the passive end-diastolic pressure-volume relationship was shifted to the left as a result of an increase in the modulus of stiffness. An associated computer simulation suggests that a change in compliance alone is sufficient to increase cardiac filling pressure and contribute to the occurrence of congestive heart failure. Taken together, these results suggest that reduced diastolic compliance occurs early in obesity and may be a major factor in the increased risk of congestive heart failure associated with obesity.
| Acknowledgments |
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Received August 14, 1998; first decision September 18, 1998; accepted November 10, 1998.
| References |
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