Vol. 281, Issue 3, H1390-H1396, September 2001
Myocardial cross-bridge kinetics in transition to failure in
Dahl salt-sensitive rats
Daniel T.
McCurdy1,2,
Bradley M.
Palmer2,
David W.
Maughan2, and
Martin M.
LeWinter1
1 Cardiology Unit and 2 Department of Molecular
Physiology and Biophysics, University of Vermont Medical School,
Burlington, Vermont 05405
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ABSTRACT |
The role of altered cross-bridge kinetics
during the transition from cardiac hypertrophy to failure is poorly
defined. We examined this in Dahl salt-sensitive (DS) rats, which
develop hypertrophy and failure when fed a high-salt diet (HS). DS rats fed a low-salt diet were controls. Serial echocardiography disclosed compensated hypertrophy at 6 wk of HS, followed by progressive dilatation and impaired function. Mechanical properties of skinned left
ventricular papillary muscle strips were analyzed at 6 wk of HS and
then during failure (12 wk HS) by applying small amplitude (0.125%)
length perturbations over a range of calcium concentrations. No
differences in isometric tension-calcium relations or cross-bridge cycling kinetics or mechanical function were found at 6 wk. In contrast, 12 wk HS strips exhibited increased calcium sensitivity of
isometric tension, decreased frequency of minimal dynamic stiffness, and a decreased range of frequencies over which cross bridges produce
work and power. Thus the transition from hypertrophy to heart failure
in DS rats is characterized by major changes in cross-bridge cycling
kinetics and mechanical performance.
heart failure; sinusoidal analysis; cross-bridge kinetics
 |
INTRODUCTION |
THE FUNCTIONAL
ABNORMALITIES of the cardiomyocyte underlying the transition from
compensated hypertrophy to failure are unclear. In patients, virtually
all data pertaining to this question have been obtained in myocardium
from explanted, end-stage failing hearts after treatment with multiple
drugs. Thus, for example, there is considerable documentation of a
major defect in excitation-contraction coupling related to impaired
calcium pumping in end-stage myocardium, but the role this plays in the
transition to failure is unclear. Similarly, it has been known for many
years that cross-bridge cycling, assessed by myofibrillar ATPase
activity, is also depressed in end-stage myocardium. A number of other
potential mechanisms underlying the transition to failure have been
proposed, including altered adrenergic responsiveness, increased
microtubule production, and energy deficits, but once again little is
known about their functional significance during the transition to failure.
The present study, performed in "skinned" strips of left
ventricular (LV) papillary muscle, was designed to focus on the
alterations in cross-bridge kinetics and myofilament viscoelastic
properties during the transition from compensated hypertrophy to heart
failure in the Dahl salt-sensitive (DS) rat. The DS rat
(4) provides a well-characterized model of cardiac
hypertrophy and the transition to failure. We found that there
were no major abnormalities in cross-bridge kinetics and myofilament
viscoelastic properties in compensated hypertrophy, but marked changes
in failing hearts. Thus in this model depression of the contractile
machinery is associated with the transition to heart failure.
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METHODS |
Animal model.
Procedures were approved by the University of Vermont
Institutional Animal Care and Use Committee. At 8 wk of age, male DS rats (Taconic Labs, supported by Merck) were randomly divided into
populations that received either high-salt (HS, 8% NaCl) or low-salt
diet (LS, 0.3% NaCl) (Harlem Teklad). The diet was started when the
animals were 2 wk older than those in our previous study in an effort
to reduce the high late mortality we observed (~80%) in HS animals
(13). Each group (HS, LS) was separated into subgroups
that were euthanized at either 6 or 12 wk after diet initiation. Thus
there were four experimental groups divided by diet and duration (in
wk): HS-6 (n = 8) or HS-12 (n = 10) wk and LS-6 (n = 8) or LS-12 (n = 12) wk.
n is the number of strips, and when more than one strip per
animal was tested the mean values were calculated and used.
Echocardiography.
After 4, 6, 9, and 12 wk of the diet, the rats were briefly (~5
min) anesthetized with isoflurane (1%) and were lightly secured in the
supine position on a warming pad. Echocardiography was performed using
a Sequoia system (Acuson; Mountain View, CA) with a 15L8 linear array
transducer (15 MHz). Briefly, in the two-dimensional mode, parasternal
long- and short-axis views were imaged. This allowed positioning of the
M-mode cursor perpendicular to the ventricular septum and LV posterior
wall. Subsequently, M-mode images were obtained. Two-dimensional
long-axis and short-axis views of the LV were recorded, with the
short-axis at the level of the tips of the papillary muscles. After
gain settings were optimized, M-mode tracings were recorded at the same
level, and posterior wall thickness at end diastole (PWT) was measured.
LV internal dimensions [end-diastolic diameter (LVEDd) and
end-systolic diameter (LVESd)] were measured using the leading
edge-to-leading edge convention. LVEDd measurements were made at the
time of maximal diastolic dimension, whereas LVESd was measured at the
point of greatest anterior systolic excursion of the posterior wall.
Values from all measured beats in each animal were averaged. LV percent fractional shortening (%FS) was calculated as [(LVEDd
LVESd)/LVEDd] × 100. One observer with no knowledge of the animal's
study group analyzed the echocardiograhic images.
Dissection and strip preparation.
After 6 or 12 wk of the diet, the rats were anesthetized with
isoflurane (1%), and the heart was rapidly removed and immediately placed in a standard Krebs solution containing 30 mM 2,3-butanedione monoxime (BDM) and gassed with 95% O2-5% CO2.
Subsequent procedures have been published in detail previously
(2). Briefly, LV papillary muscles were dissected in
BDM-Krebs solution to yield thin strips (diameter
0.125 mm;
length
1.0 mm) with parallel fiber orientation. The strips
were transferred to a vessel containing relaxing solution composed of 5 mmol/l MgATP, 40 mmol/l phosphocreatine, 240 U/ml creatine kinase, 1 mmol/l free Mg2+, 0.11 mmol/l CaCl2, 5 mmol/l
EGTA, and 20 mmol/l N,N-bis
(2-hydroxyethyl)-2-aminoethanesulfonic acid buffer (pH 7.0), ionic
strength 190 mmol/l with added sodium methane sulfonate. The
strips were then demembranated (skinned) by the addition of Triton
X-100 to a final concentration of 1% wt/vol and 50% glycerol wt/vol
(with 10 µg/ml leupeptin, a protease inhibitor), and incubated
overnight at 4°C. Strips were then transferred to a vessel with a
solution of the same composition except for Triton and stored at
20°C until used within 1 wk.
At the time of study, the strips were placed in a vessel containing
relaxing solution. Aluminum T clips were attached to the ends producing
a uniform strip with a between-clip length of ~0.5 mm. The clipped
strip was transferred to a 30-µl drop of relaxing solution on a
glass-bottomed, temperature-controlled aluminum chamber filled with
mineral oil and attached to a strain gauge and piezoelectric motor
(2). A strip-chart recorder and digital storage
oscilloscope monitored analog displacement and strip force signals. A
Peltier-effect thermoelectric device maintained oil and solution
temperature at 22°C.
Attached strips were incrementally stretched to and then maintained at
a sarcomere length of 2.2 µm (measured using an inverted microscope
and filar micrometer). Strip tension (kN/m2) was calculated
by dividing force by the cross-sectional area of the strip. Strip
cross-sectional area was calculated as the product of
· a · b, where a
and b are the major and minor radii of the strip.
Calcium activation of the strips was achieved by exchanging equal
volumes of relaxing solution for activating solution and incrementally
increasing the free calcium concentration from pCa 8.0 to pCa 4.5. Activating solution had the same ionic composition as relaxing solution
except that the total CaCl2 was 5.03 mmol/l (pCa 4.5).
Solutions were formulated by solving equations describing ionic
equilibria (7). Isometric force measurements were analyzed by a nonlinear least-squares fit of the isometric force data using the
Hill equation (SigmaPlot, Jandel Scientific, SPSS; Chicago, IL).
Sinusoidal length perturbations.
Small amplitude sinusoidal length perturbation of the skinned strips
(sinusoidal analysis) was used to obtain information about diet-induced
alterations in myocardial mechanical properties and cross-bridge
kinetics at varying calcium concentrations. Details have been described
previously (2, 14). Briefly, after steady-state isometric
tension was reached at each calcium concentration, sinusoidal perturbations of 0.125% strip length (amplitude) were applied at 42 discrete frequencies (f, 0.125- 100 Hz). The length and force signals were digitized and normalized to the initial length and
cross-sectional area of the muscle strip (Fig.
1A). The complex stiffness
modulus obtained from the data provides a measure of the relative
amplitudes (dynamic stiffness, kN/m2) and phases of the
fractional length and tension sinusoids. The phase shift
(
s) corresponds to a time shift
(ts) between the two sinusoids, where
ts =
s/2
f.
Figure 1B is a representative Nyquist plot of the viscous
and elastic moduli at each frequency under activated (pCa 5.0)
conditions. Maximal oscillatory work production by the strip
corresponds to the complex modulus data point with the lowest viscous
modulus in the Nyquist plot. The strip produces maximal oscillatory
power at the data point with the maximal product of frequency and work,
which occurs at or near the frequency producing the lowest viscous
modulus.

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Fig. 1.
A: representative digitized force (F) and
length (L) signals from sinusoidal length perturbation at
one frequency. ts is the time shift between the
two sinusoids and relates to the phase shift ( s) as
ts = s/ s,
where s equals two times the sinusoid frequency (in
radians/s). B: representative Nyquist diagram of complex
modulus with data plotted from specified frequencies. The vector sum of
the viscous (Ev) and elastic
(Ee) moduli is the complex modulus. The phase
relationship between Ev and
Ee is given by . Solid line, curve fit to the
data solving for Eq. 1. C: deconvoluted Nyquist
diagram with processes A, B, and
C. Values are determined by solving the complex modulus
equation (Eq. 1, see text for details).
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The observed complex modulus was fit to the following complex modulus
equation
where y is the complex modulus at frequency
f (in Hz), with real and imaginary (elastic and viscous)
components;
has a value of 1 and units of radians; A,
B, and C are the magnitudes of processes
A, B, and C, as defined in the model (in
kN/m2); kinetic parameters b and c
are defined as the characteristic frequencies for processes
B and C; i =
11/2; and
k is a unitless exponent. Figure 1C shows the
complex modulus with the three respective processes labeled. The sum of
the three moduli is displayed as the solid line in Fig. 1B
(i.e., the curve fit to the complex modulus equation). Process
A is hypothesized to be a measure of the viscoelastic response of
parallel passive elements of the strip. Values for the hemispherical
processes B and C are thought to reflect the
number and the unitary stiffness of cycling cross-bridges per
cross-sectional area, with B representing a work or
force-producing process and C representing a work-absorbing process in the cross-bridge cycle (15, 16). Maximum
oscillatory work production by the cross bridges occurs at the nadir of
process B, corresponding to frequency
b. 2
b is the apparent rate constant for the
work-producing step and power =
· f · Ev
(
L/Lo)2, where
Ev is the viscous moduli,
L is the
amplitude of sinusoidal length pertubation, one-half peak to peak; and
Lo is the strip length. Maximum
oscillatory work absorption occurs at the apex of process
C, corresponding to frequency c, with
2
c the apparent rate constant of the work-absorbing step
(14).
Statistics.
Data are reported as means ± SD unless indicated. Two-way
analysis of variance (ANOVA) was used to detect differences. A
Student-Newman-Keuls test was used for multiple comparisons. A value of
P < 0.05 was taken to indicate significance.
 |
RESULTS |
Body weight, LV-to-body weight ratio, and mortality.
Table 1 shows the effects of diet on body
weight (BW), LV-to-BW (LV/BW) ratio, and mortality. Initiation of the
HS diet when the animals were 8 wk old rather than 6 wk old resulted in
a greatly reduced mortality (20% vs. ~80%) compared with our
previous report (13), whereas still causing a marked
increase in LV/BW ratio at 6 wk. LV/BW ratio then decreased at 12 wk as
the animals progressed toward heart failure. LV/BW ratio was
significantly higher in HS-6 and HS-12 compared with age-matched
controls. Previous studies from our laboratory as well as others have
documented that between the sixth and twelfth week of the HS diet there
are significant increases in mortality, wet lung weight, blood urea
nitrogen, and creatinine consistent with a transition to heart failure
(11, 13). BW of LS-12 rats was slightly larger than HS-12
rats.
Echocardiograhic variables.
Echocardiographic assessment was performed after 4, 6, 9, and 12 wk of
the diet. LVEDd was significantly larger in the HS-9 group compared
with both age-matched LS controls and the previous HS-6 measurement.
LVEDd continued to increase such that the HS-12 group had a
significantly larger LVEDd than either HS-9 or LS-12 groups
(P < 0.01). The LS group maintained a constant LVEDd
and LVSDd throughout. LVSDd was significantly greater in the HS-12 compared with that of the HS-9 or the LS-12 group. PWT was increased by
HS diet at 6, 9, and 12 wk compared with that of the LS controls. However, the HS-12 group PWT was smaller than that in the HS-9 group,
consistent with progressive dilatation without additional hypertrophy.
LS-6 %FS was ~40% and remained at about this value during the
study. HS-6 %FS was increased compared with LS-6 and, in combination
with the increased PWT, indicates compensated hypertrophy. At 9 wk %FS
had decreased compared with HS-6 and was similar to the age-matched LS
controls. This change in function at 9 wk, along with the increased LV
dimension in diastole and systole, suggests that HS-9 hearts are
starting to undergo a transition to failure. At the 12 wk time point,
%FS in the HS group (32%) was greatly reduced compared with both LS
controls and the previous HS time point. In conjunction with major
increases in LVEDd and LVSDd (~25%), this indicates LV decompensation.
Isometric tension-calcium relation.
There were no significant differences in the absolute relaxed (pCa 8.0)
or maximal tension (pCa 5.0) after 6 wk of the diet. The calcium
concentrations producing half-maximal relative (percentage of maximal)
tension generation (pCa50) were equivalent after 6 wk of
the diet (HS 5.28 ± 0.02 vs. LS 5.32 ± 0.02). Figure
2 illustrates the isometric
tension-calcium relation in strips from the 12-wk diet groups expressed
both as absolute (kN/m2) tension values (Fig.
2A) and as a percentage of maximal tension (Fig.
2B). The regression lines in Fig. 2 represent the data fit to a modified Hill equation. There was a significant increase in
pCa50 in the HS-12 group assessed from the pCa-absolute
tension relationship (LS 5.14 ± 0.05 vs. HS 5.29 ± 0.03, P < 0.03, Fig. 2A) and from the
pCa-relative tension relationship (LS 5.28 ± 0.03 vs. HS
5.39 ± 0.02, P < 0.001, Fig. 2B),
indicative of increased calcium sensitivity. The trend toward higher
maximal tension in the LS-12 group (Fig. 2A) was not
statistically significant.

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Fig. 2.
Tension-pCa relationship of skinned papillary fibers from
Dahl salt-sensitive rats on specified diet for 12 wk. Data are
means ± SD. 1 kN/m2 = 1 mN/mm2.
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Sinusoidal analysis.
In Fig. 3 a Bode plot of the dynamic
stiffness-frequency relation from the sinusoidal analysis is
illustrated for the 12-wk diet groups. When the muscle is relaxed (pCa
8.0) there is a roughly linear relationship between dynamic stiffness
and the frequency of length perturbation (Fig. 3A). With
activation (Fig. 3, B and C) there is an increase
in the magnitude of dynamic stiffness that reflects an increased number
of force-generating cross bridges. In addition, the dynamic
stiffness-frequency relation becomes more complex, with relatively low
dynamic stiffness at low frequencies that decreases to a minimum as the
frequency increases. The nadir of dynamic stiffness is referred to as
Fmin or the "dip" frequency. At frequencies greater
than Fmin there is a dramatic increase in stiffness because
an increasing number of attached cross bridges are unable to complete
the transition to the postforce producing state. There was no
difference in the magnitude of minimal dynamic stiffness or
Fmin in LS-6 and HS-6 groups at pCa 5.0 or 5.5. At pCa 5.0, Fmin was significantly lower in the HS-12 group than the
LS-12 group (3.30 ± 0.79 vs. 4.98 ± 1.28 Hz, Fig.
3C, P < 0.05). The magnitude of minimal
dynamic stiffness was 35% less in the HS-12 group, although this
difference did not reach statistical significance (P = 0.084). The difference between LS-12 and HS-12 is accentuated when
dynamic stiffness is examined at a submaximal calcium concentration of
pCa 5.5 (Fig. 3B), which is closer to normal in vivo
systolic calcium levels (6). HS-12, which has greater
calcium sensitivity (Fig. 2), displays the characteristic dip frequency
observed in maximally activated strips, whereas a clearly defined dip
in dynamic stiffness is absent in the plot for LS-12 (Fig.
3B). At pCa 5.5 HS-12 dynamic stiffness was significantly less than LS-12 between 2.6 and 6.0 Hz and is attributed to an increased sensitivity of the cross bridges to length perturbation.

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Fig. 3.
Dynamic stiffness-frequency relation after 12 wk of diet
with varying levels of calcium activation. A: pCa 8.0;
B: pCa 5.50; C: pCa 5.0. Lines are fits to
complex modulus equation (Eq. 1) using values (see Table 3)
for model-defined processes. See RESULTS for description.
Data are means ± SE; n = 9 for each group.
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The phase-frequency relation shown at pCa 5.0 for the 12-wk diet groups
in Fig. 4 represents the
s
of the recorded force sinusoid relative to the length sinusoid and
corresponds to an actual ts in the two
sinusoids. A negative phase shift indicates a negative viscous modulus
and that work (net mechanical energy) produced by the strip over one
complete perturbation cycle is greater than that absorbed by the strip
from the apparatus. A positive phase shift indicates net absorption of
energy by the strip from the apparatus. There was no difference between
groups in the phase shift after 6 wk. However, the frequency at which the phase shift was most negative was lower in the HS-12 group (1.62 ± 0.017 Hz vs. LS-12 2.57 ± 0.024 Hz, Fig. 4,
P = 0.005). In addition, the HS-12 peak positive phase
shift (net energy absorbed by the strip) also had a substantially lower
frequency (HS-12 6.45 ± 0.43 Hz vs. LS-12 11.42 ± 0.99 Hz,
P < 0.001). These findings indicate that there are
fundamental differences in the frequency-dependent viscoelastic
properties of the HS-12 strips.
The oscillatory power output of the strip reflects the active viscous
component supplied by the strip over and above the passive viscous
property of the strip. There were no significant differences in the
oscillatory power output frequency distribution in the 6-wk diet groups
(data not shown). Figure 5 shows the
frequency-oscillatory power relation for frequencies 0.0125 to 4 Hz at
maximal activation (pCa 5.0) for the 12-wk diet groups. The HS-12
strips produce power over a substantially lower range of frequencies
(
2.0 Hz) than LS-12 (approximately <3.0 Hz).

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Fig. 5.
Plot of oscillatory power-frequency relation after 12 wk
of diet at pCa 5.0. For ease of presentation the net power produced
axis is inverted. , LS; , HS.
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Mean values for the processes (coefficients) A,
B, and C and kinetic parameters b and
c (in Hz) obtained by solving the complex modulus equation
are presented in Table 2. There was a
small but statistically significant increase in c in LS-12
compared with LS-6. The reason for this increase is unclear, although
neither LS time point was significantly different from the
corresponding HS value. Of greater significance was the lower
b value in HS-12 compared with LS-12 (2.20 vs. 3.56 Hz,
P < 0.01). Therefore, according to our model, the
apparent rate constant (2
b) of cross-bridge force
generation (and work production) was also lower. Thus kinetic processes
attributable to cross-bridge function are altered in muscle strips from
hearts undergoing a transition to failure.
 |
DISCUSSION |
To understand the mechanisms responsible for the transition from
compensated cardiac hypertrophy to myocardial failure, it is important
to measure functional characteristics during each of these phases. Such
information is unavailable from patients, because myocardial tissue is
not ordinarily available during the compensated or transition phases.
The DS rat model is well suited to address this problem because it
undergoes a well-characterized, predictable transition from
compensation to failure. Thus 6 wk of the HS diet induces compensated
hypertrophy with normal chamber diameter and %FS (Tables 1 and
3).(11, 13) In skinned
strips, we found that the isometric tension-calcium relation, dynamic stiffness, and complex modulus model parameters were unchanged at this
time (Table 2). After 12 wk of the HS diet, the hearts had undergone a
transition to a decompensated state accompanied by LV dilatation and a
decrease in %FS (Tables 1 and 3). In HS-12 skinned strips, an increase
in calcium sensitivity of isometric tension was observed, with no
change in maximal tension (Fig. 2). Sinusoidal analysis indicated that
there is a decrease in Fmin, a reduced frequency range for
oscillatory power output, and a decrease in the apparent rate constant
for the work-producing step in the cross-bridge cycle (Table 2).
Corresponding to the changes in Fmin and power frequency
range, the maximum positive and negative phase shifts occur at lower
frequencies in HS-12 rats. Thus, whereas there are no significant
changes in myofilament viscoelastic properties in the compensated
state, the transition to a decompensated state is associated with major
viscoelastic alterations involving depression of both cross-bridge
cycling and mechanical performance.
We previously reported that compensated hypertrophy in DS rats is
associated with a relatively modest increase in the percentage of V3
isomyosin (from 10 to 44%) and a 25% decrease in maximum myofibrillar
ATPase (13). With decompensation, V3 isomyosin increases to about 75% and myofibrillar ATPase decreases by 44%. Consequently, it is unlikely that myofilament alterations that occur
during the transition to failure are attributable entirely to the
isomyosin shift and reduced ATPase, because both are significantly altered in the compensated phase. Furthermore, V3 isomyosin expression per se does not necessarily result in myocardial failure as evidenced by animals rendered hypothyroid who convert to 100% V3 isomyosin (18).
We also previously documented a small change in troponin T isoform
distribution and a decrease in troponin T phosphorylation in failing
Dahl rats (13). More recently, we reported a decrease in
troponin I (TnI) phosphorylation and, using a combination of isolated
native thin filaments and skeletal muscle myosin in the in vitro
motility assay, a reduction in calcium sensitivity of unloaded velocity
in failing DS rats (28). The latter finding indicates that
a change in the thin filament contributes to the altered cross-bridge
kinetics in the failing state. The decreased phosphorylation of TnI is
likely due at least in part to decreased
-adrenergic responses.
However, this effect may not be a primary cause of the transition to
failure, because there is a decreased
-adrenergic response
independent of
-adrenergic receptor density or L-type
Ca2+ channel function in the compensated heart (3,
12, 21). Thus it may not be possible to ascribe the transition
from compensated hypertrophy to failure to a simple alteration in thin
filament proteins.
We found striking reductions in the frequency of maximal work and power
generation by the myofilaments during the transition to failure. An
impairment of force augmentation with increasing contraction frequency
and a decrease in the optimal frequency of force production has been
demonstrated repeatedly in failing myocardium in vitro and in vivo
(5, 20). Because the force-frequency relationship (FFR) is
the most important determinant of increased contractile performance
during exercise (22), the depression observed in failing
myocardium may have major clinical consequences. It has generally been
considered that the depressed FFR in failing myocardium results from
impairment of both
-adrenergic responsiveness (22) and
excitation-contraction coupling, the latter related to depressed
sarcoplasmic reticulum calcium pumping (8, 26). However,
our observation of a decrease in characteristic frequency b
and apparent rate constant 2
b of the work-producing step
in HS-12 strips, as well as the reduced frequency range over which the
HS-12 strips produced work and power, suggests that depressed cross-bridge kinetics and alteration of the intrinsic viscoelastic properties of the myofilament may also contribute to FFR depression.
The substantial decrease in Fmin after the transition to
failure in our study is consistent with similar results in human heart
failure studies (9, 24). Whereas Fmin reflects
the mean cycling rate of the cross bridges (1, 14, 23,
27), it more precisely indicates the frequency where there is
maximal resonance between the imposed length change and the
frequency-dependent oscillatory force produced by the cross bridges. A
reduction in mean cross-bridge cycling rate or rate of maximal work
output is consistent with our previous report of decreased myofibrillar ATPase and increased V3 isomyosin (13). It is intriguing
that in the compensated state there was no difference in
Fmin despite a 24% reduction in ATPase in association with
an increase in V3 to about 45% of total myosin. Fmin may
thus be a more sensitive indicator of the complex alterations in
contractile proteins and thin filament composition accompanying the
transition to myocardial failure. Moreover, changes in ATPase rate may
not necessarily result in closely correlated changes in contractile
performance. In in vitro motility assay studies (10), pure
populations of V1 or V3 myosin produced velocities proportional to
their actin-activated ATPase rates. However, mixtures of myosin species
resulted in velocities that reflected complex mechanical interactions
and did not yield a linear relationship.
We documented an increased calcium sensitivity of isometric tension in
HS-12 strips. The increased sensitivity is consistent with previous
reports in both human (19, 25, 29) and canine (30) failing myocardium. The observed decrease in
characteristic frequency b (apparent rate constant of force
production 2
b) reported here suggests a mechanism
responsible for this result. We postulate that a reduction of
2
b leads to an increase in the number of cross bridges in
a preforce, weakly bound state that promotes cooperative activation of
myosin S1 binding to the thin filament (2, 17). The effect
of cross bridges accumulating in this state would be most evident in
the submaximal range of calcium activation, where the amplitude of
force development depends considerably on the cooperative activation of
the thin filament by S1 binding.
In summary, isometric tension generation and sinusoidal analysis of
papillary muscle strips from DS rats revealed no differences in the
mechanical response at the compensated hypertrophy stage of adaptation
but major alterations with the transition to failure. The latter are
associated with multiple changes in contractile protein composition and
appear to be an important mechanism for the transition to depressed
contractile function in this model.
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FOOTNOTES |
Address for reprint requests and other correspondence:
M. M. LeWinter, Cardiology Unit, Fletcher Allen Health Care,
111 Colchester Ave., Burlington, VT 05401 (E-mail:
Martin.LeWinter{at}vtmednet.org).
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.
Received 1 March 2001; accepted in final form 29 May 2001.
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