1384 Myocardial Oxygen Consumption and the Left Ventricular Pressure-Volume Area in Normal and Hypertrophic Canine Hearts Gerald Izzi, MD; Michael R. Zile, MD; and William H. Gaasch, MD Background. To assess and compare the energy demands of normal and hypertrophic hearts, defined the relation between myocardial oxygen consumption (MVo2, an index of the energy consumed by contraction) and the left ventricular pressure-volume area (PVA, an index of the total mechanical energy generated by contraction) in eight normal and eight hypertrophic (aortic band model) dog hearts; MVO2 was also measured in the nonworking (empty beating) and basal (potassium arrest) states. Methods and Results. The hearts were studied in an isolated, blood-perfused heart apparatus. The slope of the MVo2-PVA relation (the inverse of which reflects myofibrillar efficiency) was similar in normal and hypertrophic hearts (3.89±1.91 and 4.19±1.25 ml 02/mm Hg * ml' 105, p=NS). The MVo2 in empty beating (0.038±0.006 and 0.041±0.015 mllbeat/100 g, p=NS) and potassium-arrested (1.95±0.06 and 1.98± 0.20 ml/min/100 g,p=NS) hearts was likewise similar in the two groups. Conclusions. Basal and nonworking energy demands and working efficiencies of hypertrophic hearts are equivalent to those of normal hearts. (Circulation 1991;84:1384-1392) we Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 C oncentric hypertrophy of the left ventricle is generally considered an appropriate and beneficial physiological adaptation to high intracavitary pressures.1,2 This compensatory change, however, carries certain clinical risks that include a greater cardiovascular morbidity and mortality caused by myocardial infarction, heart failure, and arrhythmias.3-7 In addition, some clinical and experimental data indicate a tendency for hypertrophic hearts to exhibit a decreased tolerance to ischemia.8 In an attempt to define the mechanisms underlying such changes, we considered the possibility that abnormal energy demands or inefficient energy metabolism could be responsible. This notion was based on studies that indicate increased nonwork-related myocardial oxygen requirements in hyperthyroidism and under the condition of inotropic stimulation.9,10 Not only does the hyperthyroid rabbit heart exhibit a decreased working efficiency and increased energy costs of excitationcontraction coupling, but there is also a tendency for From the Departments of Medicine and Cardiology, The Baptist Hospital, Boston (G.I.); the Medical University of South Carolina, Charleston, S.C. (M.R.Z.); and The Medical Center of Central Massachusetts, Worcester, Mass. (W.H.G.). Supported by the American Heart Association, Massachusetts Affiliate, Inc. G.I. is an American Heart Association PhysicianInvestigator. Address for correspondence: William H. Gaasch, MD, The Med Center/Memorial, 119 Belmont St., Worcester, MA 01605. Received August 7, 1990; revision accepted May 14, 1991. basal oxygen consumption to be higher than normal in hyperthyroid hearts.9 Since nonwork-related energy demands can also be increased during inotropic interventions,10 it would seem that such changes, if present in hypertrophy, might contribute to an altered tolerance to ischemia. Accordingly, we compared the relative energy demands and efficiencies of normal and hypertrophic dog hearts by measuring oxygen consumption under working, nonworking (empty beating), and basal conditions. The heart derives essentially all of its energy from aerobic metabolism; thus its oxygen consumption provides a measure of its total energy utilization.10-12 These energy requirements are influenced by a complex interplay among a variety of factors, all of which were recognized by Suga and associates13,14 when they developed what appears to be a reliable yet relatively simple method to assess cardiac energetics. This method is based on their demonstration of a direct relation between the total mechanical energy (or work) generated by the ventricle and the total energy utilization of the ventricle. This unique relation, formulated in terms of a time-varying elastance model, used the left ventricular (LV) pressure-volume area (PVA) as an index of the mechanical energy generated by the ventricle and the myocardial oxygen consumption (MVo2) as an index of energy utilization. Although this approach does not address underlying mechanisms, the MVo2-PVA relation, like the relation between oxygen Izzi et al Myocardial Oxygen Consumption and LVH consumption and the force-length area,15 provides a method to predict energy demands and allows a description of efficiency. Suga et al'6-18 and others have used this method in normal hearts during a variety of pharmacological and other interventions, but there is little such information available in hypertrophic hearts.10,19 Thus, within the framework of the MVoz-PVA relation, we compared working, nonworking, and basal energy demands as well as efficiencies among normal and hypertrophic hearts. Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 Methods Left ventricular hypertrophy (LVH) was produced by banding the aorta of puppies at 8 weeks of age. One year later, when substantial hypertrophy was present, the functional state of the ventricle was described (combined echocardiographic and catheterization techniques). The hearts were then excised, placed in an isolated blood-perfused heart apparatus, and myocardial energetics were studied. Eight hypertrophied hearts and eight normal control hearts were evaluated. All animals received humane care in compliance with the principles of laboratory animal care formulated by the National Society for Medical Research and the Guide for the Care and Use of Laboratory Animals prepared by the National Academy of Sciences and published by National Institutes of Health (NIH Publication No. 85-23, reviewed 1985). Left Ventricular Hypertrophy Model At 8 weeks of age, puppies were anesthetized with sodium pentobarbital (25 mg/kg i.v.) and ventilated with a tnechanical respirator. A right thoracotomy was performed through the third right intercostal space, the pericardium was opened, and the aorta was dissected free from the periaortic fat and connective tissue. A 5-mm-wide nonconstricting band was placed around the aorta approximately 2 cm above the aortic valve. After the banding procedure, the pericardium was loosely approximated and the thoracotomy was closed. The animals recovered and were then allowed to "grow into" supravalvular aortic stenosis.20 At 12 months, when substantial LVH was present, the banded animals underwent cardiac catheterization and echocardiography to define the functional state of the left ventricle. The normal control dogs did not undergo catheterization. The details of these methods and techniques were published previously.20 Isolated Heart Preparation and Measurements Our methods and a description of the isolated blood-perfused dog heart preparation have previously been described in detail.21,22 Briefly, in each experiment a support dog was anesthetized with pentobarbital (15-20 mg/kg), anticoagulated with intravenous heparin, and mechanically ventilated. The heart from the experimental dog was placed on cardiopulmonary bypass (perfused with blood from the femoral artery of the support dog); the heart was 1385 then excised, placed in the isolated heart chamber, and perfused at a constant pressure of 100 mm Hg. The coronary venous blood from the isolated heart was drained from the right atrium and right ventricle (by a large-bore catheter with multiple side holes) and returned to the femoral vein of the support dog. This system provided empty right-heart chambers throughout the experiment. Ventricular fibrillation was induced and the left atrium was opened. A balloon on a silastic mount was placed in the left ventricle through the mitral annulus and the heart was submerged in a blood bath maintained at 37°C. A heat exchanger system was used to maintain the coronary perfusion temperature at 37°C. The heart was defibrillated and the preparation was allowed to stabilize for 30 minutes before starting the experiment. All studies were performed at constant heart rate (atrial pacing at approximately 120 beats/min). LV pressure was measured with a Statham P23Db pressure transducer. Systolic and diastolic pressures were measured during incremental additions of saline to the ventricular balloon until systolic pressure exceeded 100 mm Hg. The volume associated with this peak systolic pressure was assigned a value of 100% (Vl,o) and all other volumes were related to the 100% volume. Thus, LV pressures were assessed over a range of five volumes (i.e., V20, V40, V60, V80, V100)4 Coronary blood flow was measured with an in-line flowmeter. Blood was sampled from the arterial (perfusion) and coronary venous catheters and pH, Po2 and Pco2 were determined using a blood gas analyzer (Instrumentation Laboratory, Watertown, Mass.). Arterial and venous oxygen contents were calculated from the blood oxygen saturation and the measured hemoglobin concentration using the nomogram of Rossing and Cane.23 Pressure-Volume Area In each heart, five coordinates of systolic pressure and volume were obtained by incrementally filling the LV balloon over a range of volumes from V20 to Vloo. A volume equal to that of the plastic balloon mount (4 ml) was added to each of the five saline volume values so the pressure-volume plots reflected total LV volume. The five pressure-volume coordinates were fit by a linear equation and the slope of the systolic pressure-volume relation that represents maximum systolic elastance (Em,,) was determined by least-squares analysis. This systolic pressure-volume line represents the upper border of the PVA. In a similar fashion, the diastolic pressure-volume coordinates were fit by a linear equation; this line defined the lower border of the PVA. Thus, at any volume, the PVA is the area encompassed by the systolic and diastolic pressure-volume lines and the vertical isovolumic pressure trajectory at that volume. The PVA is expressed in millimeters of mercury times milliliters per beat per 100 g of myocardium; alternatively, 1386 Circulation Vol 84, No 3 September 1991 Normal 0) 0 0 2.0 01) n 0) ; I,) to E E 0 W z 0 cri a- C) LU) 1.0- MVO2 -5.44 PVA +0.97 r=0.95 (n z 0 0.5z X 0 0.02 Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 VOLUME (ml) it may be expressed as joules per mm Hg * ml=0.000133 J). 0.04 0.06 0.08 PVA (joules/beat/ 1 0Og) beat per 100 g (1 Myocardial Oxygen Consumption At each of the five volume states, total coronary blood flow and coronary arteriovenous oxygen difference were measured. MVo2 of the entire heart was calculated as the product of coronary blood flow (milliliters per minute) and the arteriovenous oxygen difference (milliliters of 02 per 100 ml of blood). The MVo2 of the total heart was determined with the right and left ventricles empty. The MVo2 of the right ventricle was calculated as the product of the total heart MVo2 and the ratio of the right ventricular weight to the combined weight of both ventricles; this ratio averaged 0.25+± 0.02 in the normal hearts and 0.19+0.02 in the hypertrophic hearts. Since the right ventricle was empty throughout the experiments, we assumed that the right ventricular contribution to total MVo2 remained constant throughout each experiment. Thus, the LV MVo2 at any volume is equal to the total heart MVo2 minus the (empty) right ventricular MVo2. Oxygen consumption is expressed in milliliters of 02 per beat per 100 g and in joules per beat per 100 g of myocardium (1 ml of oxygen is equivalent to 20 J). Potassium Arrest After baseline measurements of coronary blood flow and arteriovenous oxygen difference in the empty beating heart, potassium chloride (50 meq/l) was infused into the arterial perfusion line at a rate sufficient to produce asystole. After an initial bolus, an infusion rate of approximately 35 mlmin was sufficient to maintain an asystole state. Asystole was confirmed by the absence of pressure development and a flat EKG signal; manual palpation of the LV 0.10 0.12 FIGURE 1. Plots show representative normal example of a pressure -volume area (PVA) and the relation between myocardial oxygen consumption and PVA. Left panel: Five systolic and five diastolic pressure-volume coordinates define the PVA; note that the PVA does not include the zone beneath the diastolic pressure -volume line. The slope of the systolic pressure -volume line represents maximum systolic elastance (E,L); in this example E,,, equals 5.4 mm Hg/ml. Right panel: The relation between myocardial oxygen consumption (MVo) and PVA is shown. Both MVo2 and PVA are exvpressed in joules per beat per 100 g. The solid line was denrved from a least-squares best fit of the five coordinates. The slope of this relation is 5.44 and the intercept (i.e., the PVA -independent oxygen consumption) is 0. 97 J/beat/100 g. confirmed a flaccid asystolic heart in all experiments. Coronary blood flow and arteriovenous oxygen difference were measured at 1-minute intervals for 7 minutes and the MVo2 of the total heart was calculated from these data; as before, the LV MVo2 was determined by subtracting the right ventricular contribution to total heart MVo,. MV,2-PVA Relation Each of the five PVAs was plotted against the corresponding values for oxygen consumption, and the slope of the MVo2-PVA relation was determined by fitting the five coordinates by a linear equation. The extrapolated y intercept is an index of the MVo2 of the empty beating heart. The MVo2 of the empty beating heart (V0) was also measured directly. This analysis is illustrated in Figures 1 and 2. Myofibrillar efficiency was calculated as the ratio of PVA to excess MVo2 (the excess MVo2 equals total oxygen consumption minus that required for basal metabolism plus activation).10 This ratio is equivalent to the inverse slope of the MVo2-PVA relation. To calculate efficiency, both PVA and MVo2 are expressed in joules per beat per 100 g (see above). Thus, the ratio of PVA (in joules) to excess MVo2 (in joules) is a dimensionless parameter that reflects the chemomechanical energy transduction efficiency of the contractile machinery; we refer to this as myofibrillar efficiency. Data Analysis Data in the table and text are presented as mean+SD; mean+SEM is used in the figures. Differences in the slopes (Emax and MVo2-PVA relation) and intercepts between normal and hypertrophic groups were analyzed by using an analysis of variance of regression and an analysis of covariance with a Izzi et al Myocardial Oxygen Consumption and LVH 1387 LVH C) 0 0 -, Cu a) -0 2.0- Ci) 0 0 cm 1.5- z E E 0 2 I- W a: CO) CO) 10- Cl) z 0 MV02= 6.72 PVA + 0.68 cc a. z W r =0.97 0.5- 0 Q02 Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 VOLUME (ml) repeated-measures design. Differences in other parameters were assessed with an unpaired t test. Differences were considered significant if p<0.05. Results As in our previous studies,20 the group of aorticbanded animals developed a substantial increase in LV mass; the LV/body weight ratio was 9.2+1.6 g/kg. The functional state of the LV assessed by echocardiography and cardiac catheterization remained normal; fractional shortening was 40±9% and LV enddiastolic pressure was 9+3 mm Hg. Thus, the eight banded dogs in the current study are comparable with those reported in our previous studies of LV function, myocardial blood flow, and the tolerance to ischemia in LVH.8,20 The LV/body weight ratio of the normal control hearts was 5.2±1.2; these dogs did not undergo cardiac catheterization. Representative examples of the MVo2-PVA relations in normal and hypertrophic hearts are shown in Figures 1 and 2. The data are presented in Tables 1 and 2, and a summary of the results is shown in Figure 4. MVo2-PVA Relations At Vlo (i.e., the volume required to produce a systolic pressure of approximately 100 mm Hg) there were no significant differences in LV systolic pressure, diastolic pressure, volume, or Em.x between the two groups (Table 1). The average values for the PVA in the normal and LVH groups (1,230+300 and 1,130+200 mm Hg times milliliters per beat) were not significantly different. When expressed per 100 g of LV, the PVA in the group with LVH was significantly less than normal (928±321 versus 565+±202 mm Hg times milliliters per beat per 100 g). The MVo2 (expressed per 100 g of LV) was likewise lower than normal in the LVH group, but this difference did not achieve statistical significance. 0.04 I 0.06 I 008 FIGURE 2. Plots show representative example of pressurevolume area (PVA) (left panel) and oxygen consumption data from an animal with left ventricular hypertrophy (LVH) (right panel). Maximum systolic elastance is 5.4 mm Hg/ml. The slope of the relation between oxygen consumption and PVA is 6.72 and the PVA-independent oxygen consumption is 0.68 J/beatI100 g. 0.10 PVA (joules/beat/ 100g) There was no significant difference in the slope of the MVo2-PVA relation between normal and hypertrophic groups (3.89+1.91 versus 4.19+1.25 ml 02 millimeter of mercury times milliliters times 1O5). Thus, the relation between energy used (i.e., MVo2) and energy generated (i.e., PVA) is essentially equal in normal and hypertrophic hearts; myofibrillar efficiency is similar in normal and hypertrophic hearts (21+ 9 versus 19 +1 1, p = NS). per Nonworking and Basal MVo2 At zero PVA, the MVo2 was almost equal in the two groups (0.040±0.006 versus 0.043±0.012 ml/ beat/100 g); these extrapolated values are similar to those obtained by direct measurement (0.038+0.006 versus 0.041+0.015 ml/beat/100 g). During potassium arrest (Figure 3), MVo2 was essentially equal in the normal and hypertrophic groups (1.95+0.06 and 1.98+0.20 ml/min/100 g); thus, basal oxygen requirements in this model of LVH is not significantly different from normal. Our interpretation of these data is that the nonwork-related energy demands (basal plus activation) are normal in concentric LVH. These results are summarized graphically in Figure 4. Discussion The uniquely aerobic character of myocardial metabolism underlies the use of MVo2 as an index of the heart's total energy utilization. The factors that influence conversion of chemical energy into mechanical work (i.e., the factors governing MVo2) are well described, and several indexes have been proposed as major and minor determinants of MVo2.12 Prominent among the major factors are those related to the development of systolic force; changes in force development or the time integral of force exhibit strong positive correlations with MVo2.24 27 An essential limitation of these indexes is that the MVo2 is related 1388 Circulation Vol 84, No 3 September 1991 Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 TABLE 1. Left Ventricular Energetics in Normal and Hypertrophied Hearts Normal (n =8) Left ventricular pressure at V1l+ 110±9 Peak systolic (mm Hg) End diastolic (mm Hg) 5.6+2.5 Left ventricular volume (Vl0 in ml) 24.9+4.2 Left ventricular mass (g) 132.7+20.4 Emax (mm Hg/ml) 5.36±+1.17 Total mechanical energy at Vloo PVA (mm Hg * mlfbeat) 1,230+296 928+321 (mm Hg. ml/beat/100 g) Myocardial oxygen consumption 0.073±+0.015 Working LV (ml 02 /beat/100 g at Vloo) 0.038±0.006 Empty beating LV (ml 02/beat/100 g) 1.95+±0.06 Potassium arrest (ml 02/min/100 g) MVo2-PVA relation 3.89± 1.91 Slope (ml 02/mm Hg * ml 105) 5.83±3.03 (dimensionless) 0.040±0.006 Intercept (ml 02/beat/100 g) 0.80±0.13 (joules/beat/100 g) 21±9 Myofibrillar efficiency (%) Hypertrophy (n=8) 112+6 8.8+3.1 22.6+9.0 205.0+44.5* 5.97±2.96 1,130±200 565-+202* 0.067±0.019 0.041+0.015 1.98±0.20 4.19± 1.25 6.25±2.01 0.043±0.012 0.89+0.30 19± 11 LV, left ventricle; PVA, pressure-volume area. *p<O.05. to factors other than force development and external work. Recognizing that myocardial energy requirements are determined by the sum of external and internal work, Britman and Levine28 used a model of the myocardium consisting of a contractile element in TABLE 2. Regression Equations for the MVo2-Pressure-Volume Area Relations in Normal and Hypertrophied Hearts Regression equation r Normal 1 2 3 4 5 6 7 8 MVo2=5.23 PVA+0.82 MVo2=4.99 PVA+0.58 MVo2=5.44 PVA+0.97 MVo2=12.06 PVA+0.82 MVo2=2.96 PVA+0.69 MVo2=4.54 PVA+0.77 MVo2=8.39 PVA+0.93 MVo2=3.01 PVA+0.84 0.97 0.97 0.95 0.95 0.99 0.99 0.99 0.83 Hypertrophy MVo2=6.11 PVA+0.73 MVo2=9.36 PVA+0.85 MVo2=5.42 PVA+ 1.51 MVo2=2.17 PVA+0.74 MVo2=6.72 PVA+0.60 0.99 0.97 0.99 0.86 0.97 0.89 MVo2=7.06 PVA+0.92 0.87 MVo2=6.72 PVA+0.92 0.96 MVo2=6.44 PVA+0.91 Linear regression analysis was used to determine the correlation coefficient (r). The MVo2 and pressure-volume area (PVA) are expressed in joules per beat per 100 g; thus, the slope of the MVo2-PVA relation is dimensionless and the intercept is given in joules per beat per 100 g. 1 2 3 4 5 6 7 8 series with an elastic element. With knowledge of the elastic element stiffness, it was possible to calculate contractile element work (CEW) and to relate this variable to MVo2 over a wide range of altered hemodynamics in anesthetized dogs. They found a high correlation between CEW and MVo2, and they demonstrated that this relation was significantly better than that found between oxygen consumption and pressure-time per minute, force-time per minute, or fiber shortening. This model of a contractile element in series with an elastic element has significant shortcomings29 and partly for this reason, CEW is not widely used as an index of energy utilization. However, the principle that MVo2 is influenced by mechanical factors other than external work is of major physiological importance. Using a time-varying elastance model of the left ventricle, Suga et al3,14 recognized a positive linear relation between the MVo2 and the total PVA of the working left ventricle. Thus, the energy used by the left ventricle was found to be closely related to the size of the area defined by the end-diastolic and end-systolic pressure-volume lines (and the systolic trajectory of pressure-volume between end diastole and end systole). In the ejecting heart, this area consists of the systolic pressure-volume loop (external work) plus the triangular area to the left of this loop (potential energy); in the nonejecting (isovolumic) condition, there is no external work and the total mechanical energy is represented by the triangular area to the left of a vertical line defined by the systolic pressure development. Importantly, MVo2 is linearly related to the PVA regardless of whether the Izzi et al Myocardial Oxygen Consumption and LVH 1389 6 CJ 0 0 c 5- 2 4 - Baseline 44 E FIGURE 3. Plot showing left ventricular consumption during potassium arrest in normal hearts and hearts with left ventricular hypertrophy (LVH). Baseline data were obtained in the empty beating (nonworking) state. The oxygen consumption fellfrom baseline values of 4. 7and 5.1 in normal and LVH to approximately 2 ml 02/min/100 g during arrest. There was no significant difference in oxygen consumption between the two groups. Normal A LVH * oxygen z 3- 2 CL U) 2z z W I - 11 Infusion -KCI 1 00 Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 0 2 1 3 6 5 4 7 TIME (minutes) soned that an assessment of myocardial energetics within the MVo2-PVA framework would be more relevant to the clinical problem of altered tolerance to ischemia in hypertrophic hearts.8 Therefore, we determined the slope of the MVo2-PVA relation and used the inverse of this relation as an index of efficiency. To date, only hyperthyroidism (in rabbits) has been shown to affect the slope; this is thought to be mediated through a change in the V1/V3 isomyosin ratio9; such changes are apparently not seen in dogs.35 Although basal and nonwork-related oxygen requirements are affected by the inotropic state, the slope of the MVo2-PVA relation is remarkably in- heart is freely ejecting, auxotonic, or isovolumic; it is not determined by the time course of the isovolumic pressure-volume coordinates.30 MVo2-PVA Relation and Efficiency It is generally accepted that, when systolic wall stress and inotropic state are considered, MVo2 is normal in human hypertrophic hearts.2627,31 Such studies, however, do not dissect out the relative contributions of basal and activation energy requirements, nor do they provide information on myofibrillar efficiency. Other more basic studies are important in terms of underlying mechanisms,32-34 but we rea- .Z .0 od /ormal LVH 0i CDE0 0 0.06 1.2. CD c)0. z 0 E 0.04 0.- NORMAL Emax 5.0 CD) z - 0 MV02 0.02 1.2 LVH z W ± 5.8 PVA+ 0.80 0.4_ 0 ---- BASAL- - - - Emax -5.4 ± 2.8 MV02 6.3 PVA+0.89 - 0 0.625 250 0.05 0.075 500 0.J0 (joules/beat) 750 (mmHg.mI/beat) PRESSURE VOLUME AREA (per 100 gm LV) FIGURE 4. Plot showing summary of the relations between myocardial oxygen consumption and the left ventricular pressurevolume area (PVA) in normal hearts and hearts with left ventricular hypertrophy (LVH). Oxygen consumption is expressed in milliliters of 02 per beat per 100 g and in joules per beat per 100 g (1 ml of oxygen is equivalent to 20 J). The PVA is expressed in millimeters of mercury times milliliters per beat per 100 g and in joules per beat per 100 g (1 mm Hg ml is equivalent to 0.000133 J). Symbols indicate oxygen consumption at a working volume of Vioo; see text for details. Basal and nonworking (zero PVA) energy requirements and myofibrillar efficiencies of normal and hypertrophic hearts are essentially equal. 1390 Circulation Vol 84, No 3 September 1991 Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 sensitive to pharmacological and other acute interventions that affect contractility.10 The inverse slope of the MVo2-PVA relation can be taken to represent the efficiency of chemomechanical energy conversion.10 This is not merely the efficiency of performing external work; rather, it reflects a total efficiency of performing external work plus a residual "potential energy" that remains after end systole. With each cardiac cycle some of this potential energy is converted to internal work, but most of it is dissipated as heat.14 Suga30 has emphasized several differences between the potential energy in his PVA analysis and the internal work in Britman and Levine's CEW analysis; recognizing and comparing the differing energy costs of potential energy and internal work may provide a better understanding of ventricular energetics. Myofibrillar efficiencies calculated from the inverse slope of the MVo2-PVA relation were essentially the same in our normal and hypertrophic hearts (21% and 19%, respectively). These data are consonant with those of Starling et al,36 who studied normal in situ dog hearts and reported MVo2-PVA slopes of 3.15 and 3.48 ml 02 per millimeter of mercury times milliliters times 105; thus, the dimensionless slope was approximately 5 and myofibrillar efficiency was approximately 20%. Nozawa et al37 reported a similar efficiency in normal in-situ hearts. There is no obvious reason why these efficiency values are lower than those reported by Suga et al, but a common feature of our methods and those of Starling et al is the use of calculated oxygen contents of coronary arterial and venous blood. Suga measured oxygen content directly, and it is possible that the differences in the MVo2-PVA slope (and efficiency) is somehow related to the oximetry method. These considerations, however, have little bearing on our comparisons between normal and hypertrophic hearts; our data indicate that myofibrillar efficiency in pressure-overload hypertrophy is not significantly different from normal. MVo2 in Empty Beating Hearts The energy demands of a nonworking heart can be estimated by extrapolation of the MVo2-PVA relation to zero PVA or by directly measuring MVo2 in the empty beating condition. The extrapolated values for MVo2 in our normal (0.040 ml/ beat/100 g) and hypertrophic hearts (0.043 ml/beat/ 100 g) were essentially equal; these extrapolated values were not significantly different from those measured directly (Table 1). In an extensive review of this topic, Suga reported values ranging from 0.017 to 0.047 ml/beat/100 g; the average value from his five most recent studies was 0.028 ml/beat/100 g in empty beating hearts'0; this is equivalent to approximately 3-4.5 ml/min/100 g. Due in part to the wide range of heart rates in published experiments, 24,28,38-40 the MVo2 of nonworking hearts reportedly ranges from 2.5 to 5.5 ml/min/100 g. In our experiments, the normal and hypertrophic hearts (nonworking) consumed approximately 5 ml 02/min/100 g. Direct measurements of the energy demands of empty beating hearts theoretically overestimate those of a pure nonworking state (i.e., activation plus basal requirements) for at least two reasons. First, our experimental preparation precludes measurement in a truly empty condition (the LV contains a plastic balloon mount); thus, some isometric force is developed in the area of the mitral annulus. Second, low levels of crossbridge cycling (even in a totally empty heart) require energy; ideally, such an unmeasured contribution to the energy demands should be considered. Thus, to assess accurately the energy demands of a true nonworking state (i.e., basal plus activation) it would be necessary to inhibit all crossbridge cycling; this could be accomplished with 2,3 butenedione (BDM), a cardioplegic agent that (at low doses) selectively inhibits crossbridge cycling in a reversible manner.41-43 Such studies would be necessary to avoid an overestimation of the nonworking (i.e., basal plus activation) requirements. However, our observation that the extrapolated value for MVo2 is similar to the measured value suggests that any such error is probably small. Basal Oxygen Consumption The resting or basal metabolic rate of the intact LV is difficult to assess because the heart does not normally exhibit sufficiently long diastolic intervals to permit measurements of oxygen consumption in the absence of contraction. In our experiments, we rendered the heart inactive by infusing potassium into the coronary arterial perfusion line and thus we were able to measure an asystolic MVo0 during a continuous, stable coronary perfusion. Within 2 minutes of asystole, the MVo2 fell to approximately 2 ml/min/100 g and remained constant for the duration of the potassium infusion; the results were essentially equal in the normal and hypertrophic hearts (Figure 3). Our average values are similar to the basal MVo2 (1.9 ml/min/100 g) that Britman and Levine derived from their calculations of contractile element work in the intact working heart.28 The results are also similar to the normal basal requirements (1.5-2.0 ml/min/100 g during potassium arrest) reported by Suga et al16 and others.38,39,44 Sink et a145 found a slightly lower value in hypertrophied hearts (1.3 ml/min/100 g), and they also concluded that this was the same as that seen in normal hearts. Within the range of data reported here, basal requirements are approximately 40% of that required by empty beating hearts and 20% of that required by working hearts (Figure 4). Since basal MVo2 may increase as a function of myocardial fiber length,46 it is possible that the relative contribution of basal to total MVO, might increase as the chamber is filled. If this were the case, the myofibrillar efficiencies might be greater than we calculated. Izzi et al Myocardial Oxygen Consumption and LVH Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 Implications During cardiac surgery, the left ventricle is subjected to ischemic arrest, potassium arrest, and on occasion the empty beating state is maintained for variable periods of time. During these periods, any increased oxygen requirement (basal or activation) might lead to increased ischemic injury. The current results indicate that oxygen requirements are normal in our model of concentric LVH. Therefore, any reduced tolerance to such surgical procedures is not likely to be due to increased oxygen demands per se. It is possible, however, that heightened sympathetic tone or the administration of positive inotropic agents might augment basal or activation-related oxygen demands and in this manner contribute to an impaired tolerance to ischemia, independent of work-related demands. In the absence of such increased "basal plus activation" oxygen demands, abnormal myocardial perfusion or depressed baseline energy stores are likely responsible for the increased sensitivity to ischemic injury seen in some hypertrophic hearts.8 The MVo2-PVA relation that we applied in these studies of isolated dog hearts might have potential in clinical studies of myocardial energetics. The echocardiogram is ideally suited to measure LV cavity size or volume and wall mass. Coupled with measurements of intracavitary pressure, a PVA is relatively easy to obtain. Methods to measure coronary blood flow and MVo2 in humans are likewise available. Thus, LV energetics and efficiency in patients with and without heart disease can be described; such methodology might be particularly useful in the evaluation of new pharmacological therapies for patients with heart disease. References 1. Grossman W: Cardiac hypertrophy: Useful adaptation or pathologic process? Am J Med 1980;69:576-584 2. Swynghedauw B, Schwartz K, Apstein CS: Decreased contractility after myocardial hypertrophy: Cardiac failure or successful adaptation? Am J Cardiol 1984;54:437-440 3. Koyanagi S, Eastham CL, Harrison DG, Marcus ML: Increased size of myocardial infarction in dogs with chronic hypertension and left ventricular hypertrophy. Circ Res 1982; 50:55-62 4. Koyanagi S, Eastham CL, Marcus ML: Effects of chronic hypertension and left ventricular hypertrophy on the incidence of sudden death following coronary occlusion in conscious dogs. Circulation 1982;65:1192-1197 5. Kannel WB: Prevalence and natural history of electrocardiographic left ventricular hypertrophy. Am J Med 1983;75:4-11 6. Messerli FH, Ventura HO, Elizardi DJ, Dunn FG, Frohlich ED: Hypertension and sudden death: Increased ventricular ectopic activity in left ventricular hypertrophy. Am J Med 1984;77:18-22 7. MeLenachan JM, Henderson E, Morris KI, Dargie HJ: Ventricular arrhythmias in patients with left ventricular hypertrophy. 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Gibbs CL, Papadoyannis DE, Drake AJ, Noble MIM: Oxygen consumption of the nonworking and potassium chloride arrested dog heart. Circ Res 1980;47:408-417 40. Goto Y, Slinker BK, LeWinter MM: Similar normalized Ema. and 02 consumption-pressure volume area in rabbit and dog. Am J Physiol 1988;255(24):H366-H374 41. Li T, Sperelakis N, Teneick RE, Solaro RJ: Effects of diacetyl monoxime on cardiac excitation-contraction coupling. J Pharmacol EKp Ther 1985;232:688-695 42. Loiselle DS, Shine PJM: Estimating the cost of the ECG using BDM (2,3-butanedione monoxime). J Mol Cell Cardiol 1986; 18(suppl 1):271-277 43. Alpert NR, Blanchard EM, Mulieri LA: Tension independent heat in rabbit papillary muscle. J Physiol (Lond) 1989;414: 433-453 44. McKeever WP, Gregg DE, Canney PC: Oxygen uptake of the nonworking left ventricle. Circ Res 1958;6:612-623 45. Sink JD, Hill RC, Attarian DE, Wechsler AS: Myocardial blood flow and oxygen consumption in the empty beating, fibrillating, potassium-arrested hypertrophied canine heart. Ann Thorac Surg 1983;35:372-379 46. Loiselle DS: The rate of resting heat production of rat papillary muscle. Pflugers Arch 1985;405:155-162 KEY WORDS * left ventricular hypertrophy * left ventricular pressure-volume area myocardial oxygen consumption myocardial energetics Myocardial oxygen consumption and the left ventricular pressure-volume area in normal and hypertrophic canine hearts. G Izzi, M R Zile and W H Gaasch Downloaded from http://circ.ahajournals.org/ by guest on July 31, 2017 Circulation. 1991;84:1384-1392 doi: 10.1161/01.CIR.84.3.1384 Circulation is published by the American Heart Association, 7272 Greenville Avenue, Dallas, TX 75231 Copyright © 1991 American Heart Association, Inc. All rights reserved. Print ISSN: 0009-7322. 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