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1 Department of Biomedical Engineering, Columbia University, New York, New York 10027; and 2 Abteilung Kardiologie und Angiologie, Universität Göttingen, Göttingen, Germany 37075
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ABSTRACT |
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We tested the hypothesis that economy and efficiency are independent of length in intact cardiac muscle over its normal working range. We measured force, force-time integral, force-length area, and myocardial oxygen consumption in eight isometrically contracting rabbit right ventricular papillary muscles. 2,3-Butanedione monoxime was used to partition nonbasal oxygen consumption into tension-independent and tension-dependent components. Developed force, force-time integral, and force-length area increased by factors of 2.4, 2.7, and 4.8, respectively, as muscle length was increased from 90% to 100% maximal length, whereas tension-dependent oxygen consumption increased only 1.6-fold. Economy (the ratio of force-time integral to tension-dependent oxygen consumption) increased significantly with muscle length, as did contractile efficiency, the ratio of force-length area to tension-dependent oxygen consumption. The average force-length area-nonbasal oxygen consumption intercept was more than the twice tension-independent oxygen consumption. We conclude that economy and efficiency increase with length in rabbit myocardium. This conclusion is consistent with published data in isolated rabbit and dog hearts but at odds with studies in skinned myocardium.
oxygen consumption; contractile function; 2,3-butanedione
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INTRODUCTION |
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ENERGY UTILIZATION by contracting myocardium includes several components. Energy is required for the maintenance of cell homeostasis independent of stimulation or contraction (basal metabolism). Additional energy is required to depolarize and repolarize the sarcolemma (activation energy), to support calcium release and reuptake, and for cross-bridge activity. Once basal metabolism is subtracted, the remaining three terms are related to the generation of a contraction. The ratio of work performed by a contraction to the sum of these contraction-related energy requirements has been termed net mechanical efficiency (7), whereas the ratio of external plus potential work to the energy required for cross-bridge cycling alone is referred to as contractile efficiency (21). For isometrically contracting isolated muscles, external work is zero and the force-length area provides a measure of potential work (12).
Peak force and force-time integral also have been correlated with
energy consumption and employed in energetic studies. Because these
measures do not have units of work, ratios involving them are not
efficiencies; in the case of force-time integral the term economy has
been used instead (2). By nature of their definitions, we
would expect force-length area to be most useful for analysis of
shortening contractions and force-time integral for analysis of
force-frequency studies. Neither measure has a clear theoretical advantage for isometric studies. Hisano and Cooper
(12) showed that peak force, force-length area, and
force-time integral were all equally effective correlates of
myocardial oxygen consumption (M
O2)
(correlation coefficients 0.952, 0.965, and 0.970, respectively) during
isometric contractions of ferret papillary muscles, whereas force-length area was a significantly better correlate when isometric and various shortening protocols were considered together
(12).
The use of correlations between these mechanical quantities and oxygen
consumption over the range of lengths and loading conditions likely
encountered by in vivo myocardium assumes that economy and efficiency
are independent of length. At the ventricular level, the concept of
length-independent efficiency was advanced by Suga and co-workers
(21) based on the correlation of pressure-volume area
(PVA) to M
O2. At the cross-bridge
level, length-independent economy is suggested by the fact that the
ratio of tetanized force to ATP consumption in maximally activated
skinned fibers is constant over the normal working sarcomere length
(23). However, Higashiyama and co-workers
(11), using a 2,3-butanedione (BDM) partitioning method to
measure nonmechanical oxygen consumption in isovolumically contracting
isolated rabbit hearts, found that economy was significantly higher at
the higher of two volumes tested.
We therefore tested the hypothesis that economy and efficiency are independent of length in intact isolated cardiac muscle over its normal working range. We used low-dose BDM to partition oxygen consumption into its tension-dependent and tension-independent parts in isometrically contracting rabbit right ventricular papillary muscles (1, 11, 24), allowing us to calculate economy and efficiency at each muscle length and test this hypothesis. In agreement with Higashiyama's results (11) in the isolated rabbit heart and in disagreement with results in skinned rat trabeculae, we found that economy and efficiency increased significantly as the muscle was stretched from 90% to 100% of Lmax.
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METHODS |
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This investigation conforms to the Guide for the Care and Use of Laboratory Animals published by the National Institutes of Health (NIH Publication No. 85-23, Revised 1996).
Papillary muscle isolation.
Right ventricular papillary muscles were harvested from New Zealand
White rabbits (2.2-2.8 kg body wt) as follows. The animals were
euthanized, the abdomen was opened in the midline just below the
xyphoid, and the chest was entered via cuts through the diaphragm and
ribs on each side of the sternum. The great vessels and atria were
transected immediately above the atrioventricular valve rings. The
ventricles were placed in a cold (0°C) oxygenated Krebs-Ringer solution containing (mM) 152 Na+, 3.6 K+, 135 Cl
, 25 HCO


Experimental protocol. Muscles were placed into the measurement apparatus (Muscle Research System, Scientific Instruments; Heidelberg, Germany) and clamped at both ends at a length well below slack length. Muscle length was precisely manipulated and measured by micrometers graduated in 0.01-mm intervals. Muscles were perfused with Krebs-Ringer solution (composition as above without BDM) bubbled with 95% O2-5% CO2 and warmed to 37.0°C. Muscles were stretched just beyond slack length and stimulated to contract isometrically with a 5-ms pulse applied end to end at a voltage 25% above threshold and a frequency of 1 Hz. Muscles were allowed to equilibrate for 30 min before proceeding. After equilibration, muscles were stretched in 0.05-mm steps until additional stretch did not produce an increase in developed force; this length was taken as Lmax. From earlier experience with this preparation, a developed force of greater than 10 mN/mm2 at Lmax was required for inclusion in this study. Force parameters and oxygen consumption (see below) were measured under steady-state conditions at 90%, 95%, and 100% of Lmax in a random order determined by coin toss. Force parameters were additionally measured at 85% Lmax to improve the accuracy of force-length area calculations. BDM was added to the perfusate to achieve a concentration of 2 mM, and the measurement sequence was repeated. Finally, basal oxygen consumption was measured at Lmax in the presence of 30 mM BDM.
Measurement of mechanical parameters.
Isometric force was acquired digitally at 1.6-ms intervals from the
force transducer (KG4, Scientific Instruments); the raw data from three
consecutive twitches were averaged before analysis. Diastolic force was
defined as the minimum force between two contractions, total force as
the maximum force reached during an isometric contraction, and
developed force as the difference between these two. Force-time integral was calculated as the area under the twitch force curve but
above the diastolic force (Fig.
1A). All force parameters were
normalized by muscle cross-sectional area, calculated as blotted muscle
weight divided by muscle length. Force-length area was calculated as
the area between the systolic and the diastolic force-length curves
(12) and normalized by blotted muscle weight (Fig.
1B). Linear systolic and piecewise linear diastolic
force-length curves were assumed.
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Measurement of oxygen consumption.
The method used to measure oxygen consumption was described and
validated previously (17). Briefly, a miniature oxygen
electrode continuously measured PO2 in the
experimental chamber close to the muscle surface. When the flow of
perfusate was stopped, the chamber was unstirred and free of convective
currents and of oxygen leaks in the vicinity of the muscle. An oxygen
concentration gradient developed that depended on the size of the
muscle, its rate of oxygen consumption, the distance between the probe
tip and the muscle surface, and the diffusion constants of oxygen in
the muscle and the surrounding solution. The drop in
PO2 at the probe tip was measured over 20 s and compared with precalculated theoretical profiles to determine the
rate of oxygen consumption of the muscle (i.e.,
M
O2).
Partitioning of oxygen consumption.
Terms were defined by analogy to standard heat-based energetics terms
(10). Basal M
O2
referred to the oxygen consumption measured in an unstimulated muscle
in the presence of 30 mM BDM to completely inhibit cross-bridge
cycling. Nonbasal M
O2 (total M
O2
basal
M
O2) reflected oxygen costs
associated with contraction and was further separated into two
components: tension-independent M
O2
(M
O2TI), oxygen consumed to support
electrical events and calcium cycling, and tension-dependent
M
O2
(M
O2TD), the oxygen consumed for
cross-bridge cycling.
O2 was
performed according to the method of Yaku et al. (24).
Nonbasal M
O2 was plotted against force-time integral in the absence and presence of 2 mM BDM, a dose
that inhibited approximately one-half of the cross bridges without
significant effects on calcium cycling (1, 13, 19). A line
connecting these points (Fig. 2)
represented a line of decreasing number of active cross bridges
approaching the M
O2 axis (where
force-time integral = 0). The
M
O2 intercept was therefore an
estimate of M
O2TI, whereas
M
O2TD was calculated for any point
by subtracting M
O2TI from nonbasal
M
O2. Economy was calculated at each
length as the ratio of force-time
integral-to-M
O2TD (10).
Contractile efficiency was calculated as the ratio of force-length
area-to-M
O2TD.
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Statistics. All results are reported as means ± SE unless otherwise specified. Trends in each parameter with length were assessed by one-way repeated measures ANOVA using the generalized linear model procedure in SAS 6.1 (SAS Institute, Cary, NC). P values reported are based on the univariate F statistic; the Huyn-Feldt adjusted F statistic was used for data sets for which sphericity was rejected. If the overall trend with length was significant, values at 100% and 95% Lmax were each compared with the reference value at 90% Lmax using paired t-tests with the Bonferroni correction for multiple comparisons. Single comparisons were made with standard paired t-tests. A P value <0.05 was considered significant for all tests.
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RESULTS |
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Eight uniformly cylindrical papillary muscles generating at least 10 mN/mm2 at Lmax were studied. Each muscle was taken from a separate animal. Muscle length averaged 3.51 ± 0.26 mm, weight 1.05 ± 0.17 mg, and radius 0.31 ± 0.03 mm.
Mechanical parameters.
Diastolic and developed force, force-time integral, and force-length
area all increased significantly with muscle length (Fig. 3A). There was no difference
between resting (unstimulated) and basal (unstimulated, 30 mM BDM)
force (3.39 ± 0.69 vs. 3.17 ± 0.57 mN/mm2 at
Lmax, P = 0.14).
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Oxygen consumption.
As muscle length increased from 90% to 100% of
Lmax, M
O2
increased from 3.58 ± 0.40 to 4.77 ± 0.64 ml
O2 · min
1 · 100 g
1 (Fig. 3B). This represented a 33% increase
in total oxygen consumption and a 63% increase in nonbasal
M
O2. The
M
O2TD component of nonbasal
M
O2 also increased with length
(ANOVA P = 0.03), whereas the tension-independent
(M
O2TI) component did not change
significantly (ANOVA P = 0.13).
O2 as
oxygen consumption in an unstimulated preparation at
Lmax and basal
M
O2 as oxygen consumption at
Lmax in the presence of 30 mM BDM to completely inhibit cross-bridge cycling (17). Although this
distinction between resting and basal conditions was important in
diseased human myocardium, in the present study it was irrelevant.
There was no significant difference between oxygen consumption in the resting or basal states (1.78 ± 0.20 vs. 1.65 ± 0.19, P = 0.56) nor was there an effect of length on resting
oxygen consumption (paired t-test 90% vs. 100%
Lmax in 5 muscles, P = 0.23).
Economy and efficiency.
As shown in Fig. 3, the length-dependent increases in force-time
integral and force-length area were proportionally greater than the
measured increases in tension-dependent
M
O2, indicating increased economy
and efficiency. Calculated economy was 7.3 ± 0.6 mN · s · g/mm2 · µl
O2 at 90%, 10.6 ± 1.1 mN · s · g/mm2 · µl
O2 at 95%, and 12.2 ± 1.0 mN · s · g/mm2 · µl
O2 at 100% Lmax (ANOVA
P = 0.04). Economy was significantly increased at 100%
(P < 0.01) but not at 95% Lmax
(P = 0.06) compared with 90%
Lmax. Contractile efficiency was 0.10 ± 0.01 at 90%, 0.22 ± 0.02 at 95%, and 0.33 ± 0.03 at 100%
Lmax (ANOVA P = 0.002) and was
significantly increased at both 95% (P < 0.01) and
100% Lmax (P < 0.001) compared
with 90% Lmax.
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DISCUSSION |
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Does the close correlation of oxygen consumption with force-time
integral and force-length area across a range of conditions (lengths,
frequencies, and afterload) imply that economy and efficiency are
constant for a given muscle across those conditions? We and other
investigators have assumed this to be the case. However, the
current study demonstrates that both economy and efficiency change
significantly with muscle length in isometrically contracting rabbit
papillary muscles. Gibbs and Chapman (8) have pointed out
that most muscle models would not predict a constant contractile efficiency and suggested an autoregulatory process may explain the
linearity of the M
O2-PVA
relationship. Higashiyama et al. (11) suggested that a
population of nonforce-producing cross bridges may exist and consume an
amount of oxygen that is linearly proportional to PVA.
Length-dependent changes in economy.
There are a number of differences between whole heart and isolated
muscle studies that might have explained the difference between the
results of Higashiyama (11), who found increased economy
at a larger volume in isolated rabbit hearts, and studies reporting
length-independent economy in skinned fibers (14, 23).
Isolated hearts may work at lower sarcomere lengths, may undergo
different shape changes during isovolumic contraction at different
volumes [an effect demonstrated by Rankin and co-workers (20) in closed-chest dogs], or may display
preload-dependent changes in synchrony of contraction of various
ventricular regions. However, a highly significant increase in economy
was observed with increased muscle length in the present study of
isolated muscle, suggesting that length-dependent changes in economy
are a basic property of intact cardiac muscle. Great care was taken to
ensure adequate oxygenation of the muscles in this experiment (see
METHODS), making shifts in the ratio of ATP production to oxygen consumption unlikely. Because the force-time integral is a sum
over the entire muscle of mechanical events at the cellular level, the
observed increase in the ratio force-time integral to
M
O2TD therefore indicated either an
increase in the amount of cross-bridge work performed per ATP consumed
or an increase in the efficiency of transducing cross-bridge work into
force generation. Data from previous studies on skinned muscle
preparations provide little support for either possibility.
Length-dependent changes in contractile efficiency.
Regression of PVA against nonbasal
M
O2 across contractions at multiple
volumes assumes length-independent efficiency and interprets the
PVA-M
O2 correlation intercept as
M
O2TI, the portion used for
activation and calcium handling (21). In this study, using
2 mM BDM to deactivate approximately half the cross bridges and
extrapolating to a point of no cross-bridge activity to estimate
M
O2TI gave values half the intercept
of the force-length area-M
O2
regression line (Fig. 4A).
This is in direct agreement with the studies by Yaku et al.
(24) and Higashiyama et al. (11), who
reported that mechanically unloaded
O2
was twice their
O2-force-time integral
intercept. We conclude that roughly half the nonbasal energy
expenditure of an unloaded contraction at the length at which no force
is developed (L0) or the analogous volume
V0 can be attributed to activation and calcium cycling, with the other half consumed by cross-bridge activity. This provides an
alternate explanation for the data of de Tombe et al. (6), who reported in agreement with our data that low-dose BDM altered the
intercept but not the slope of the
PVA-M
O2 regression line in
isovolumically contracting isolated blood-perfused canine ventricles (Fig. 4B). The authors concluded that low-dose BDM did not
act as expected for a calcium-desensitizing agent because it altered M
O2TI; their data are equally
explained by the finding that the
PVA-M
O2 intercepts include
substantial consumption for cross-bridge activity in addition to
M
O2TI.
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Partitioning of M
O2.
Our calculations of economy and efficiency rely on the ability to
accurately partition M
O2 into basal,
tension-independent, and tension-dependent parts. Basal oxygen
consumption was measured directly and agrees well with the literature.
Our value of 1.65 ± 0.17 ml · min
1 · 100 g
1 in
rabbit right ventricular papillary muscles was identical to that of
1.66 ± 0.15 reported by Goto et al. (9) in
potassium-arrested isolated rabbit hearts. Similar values were
reported in canine isolated heart and open-chest preparations,
including 2.0 ml · min
1 · 100 g
1 by McKeever et al. (16), 1.43 by
Boerth et al. (3), and 1.02 ± 0.42 by Nozawa
et al. (18) during potassium arrest. Significantly higher
values were reported in unstimulated cat papillary muscle preparations [4.73 ml · min
1 · 100 g
1 by Cranefield and Greenspan (5) and
4.13 by Coleman (4)].
O2TI was estimated by
extrapolation, increasing the influence of measurement error.
Extrapolation error could have been reduced by using a higher dose of
BDM to generate a third point closer to the
M
O2 axis but at the risk of
introducing systematic error via the effects of larger doses of BDM on
calcium cycling. Most investigators have reported minor effects of BDM
on calcium cycling to concentrations of at least double those used in
the present study. Alpert et al. (1) reported that
force-time integral and initial heat remained linearly correlated at
BDM concentrations up to 4 mM in rabbit trabeculae. Yaku et al.
(24) found negligible effects on calcium cycling measured
using Indo-1 in isolated rabbit hearts perfused with BDM at
concentrations up to 10 mM. Using iontophoretically loaded fura 2 in
rat ventricular trabeculae, Jiang and Julian (13) recently
showed that 2 and 5 mM doses of BDM reduced internal calcium transients
by only 2% and 4%, respectively, while decreasing force by 35% and
60%. However, Perreault et al. (19) reported decreases of
~10% in calcium transients from human myocardium with 2.5 mM BDM.
Assuming 2 mM BDM in fact reduced calcium currents and
M
O2TI by 10%, this error would
double with extrapolation to 20% and would not alter our conclusions.
Expressed per beat, our estimates of
M
O2TI (0.0072 ± 0.003 ml · beat
1 · 100 g
1 at
90% and 0.0116 ± 0.004 at 100% Lmax)
agree well with those reported by Yaku et al. (24) (0.014 ml · beat
1 · 100 g
1) and by
Higashiyama et al. (11) (0.0132 ± 0.009 ml · beat
1 · 100 g
1 at a
low volume and 0.0137 ± 0.008 at a higher volume). Assuming 1 ml
O2 provides 20.0 J of energy (21), our
estimates of M
O2TI translate to 1.5 and 2.3 mJ · beat
1 · g
1 at
90% and 100% Lmax, respectively. These values
compare well with tension-independent heat measured by Loiselle and
Gibbs (15) (1.6 mJ · beat
1 · g
1 for rat and
2.5 mJ · beat
1 · g
1 for
both guinea pig and cat papillary muscles studied over a range of
lengths and frequencies at 27°C) and by Alpert et al. (1) (1.00 ± 0.17 mJ · beat
1 · g
1 at 100%
Lmax and 0.78 mJ · beat
1 · g
1 at 89%
Lmax in rabbit papillary muscles at 21°C and
0.2 Hz).
Limitations and sources of error.
The principal source of error in measurements of both mechanical
parameters and M
O2 was the
determination of muscle radius. Radius was confirmed optically with a
calibrated eyepiece grid in the microscope used to observe the muscle
chamber; optical radius differed by no more than 10% from the radius
calculated from blotted muscle weight. There was no evidence for
systematic errors in muscle radius, with good repeatability between
investigators and no consistent trend in differences between optical
and calculated radii. However, at small radii even a 10% error has
substantial consequences. For example, at an actual radius of 0.3 mm,
an underestimation of 10% would result in a 23% overestimation of
force per cross-sectional area, a 10% underestimation of oxygen
consumption, and consequent 27% underestimation of economy.
O2TI. This variability
may have prevented detection of an actual length dependence of
M
O2TI at our sample size (ANOVA vs.
length, P = 0.14) However, the BDM partitioning method
introduced, at most, small systematic errors (
20%) insufficient to
alter our conclusion that economy changes with muscle length. Similarly small errors may have been introduced in the calculation of efficiency by the assumption of a linear systolic force-length relation. Muscle
contraction in this study was isometric, and it has been shown that
damaged ends are stretched as centrally located sarcomeres shorten in
this preparation (22). This effect is relatively smaller
at longer muscle lengths, with an 8% central sarcomere shortening near
Lmax compared with a 14% shortening at 90%
Lmax (22). The small resulting
difference in the proportion of cross-bridge work lost to internal
deformation seems unlikely to explain the large economy changes we
observed, especially because the force generation-ATP consumption
relationship in skinned fibers is length independent under both
isometric (14) and sarcomere length-clamped (23) conditions.
In summary, this study demonstrates that economy and efficiency change
significantly with muscle length in isometrically contracting rabbit
papillary muscles. This conclusion is consistent with published data in
isolated rabbit and dog hearts but at odds with studies in skinned
myocardium. The basis for the difference between findings in intact
myocardium and in skinned fibers is not clear, and further studies are
needed to determine the mechanism of the observed length-dependent
changes in economy.
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ACKNOWLEDGEMENTS |
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The authors gratefully acknowledge the assistance of Dr. Konrad Güth of Scientific Instruments.
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FOOTNOTES |
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This work was supported by a grant from the Bundesministerium für Wissenschaft, Bildung und Forschung und Technologie (BMFT, BMBF 0311006). J. W. Holmes was supported by the Alexander von Humboldt-Stiftung.
Address for reprint requests and other correspondence: J. W. Holmes, Biomedical Engineering, 351 Engineering Terrace, Columbia Univ., MC 8904, 1210 Amsterdam Ave., New York, NY 10027 (E-mail: jh553{at}columbia.edu).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
First published April 4, 2002;10.1152/ajpheart.00687.2001
Received 2 August 2001; accepted in final form 22 March 2002.
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