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1 Department of Physiology II, Ca2+ handling in
excitation-contraction coupling requires considerable
O2 consumption
(VO2) in cardiac contraction. We have developed
an integrative method to quantify total
Ca2+ handling in normal hearts.
However, its direct application to failing hearts, where futile
Ca2+ cycling via the
Ca2+-leaky sarcoplasmic reticulum
(SR) required an increased Ca2+
handling VO2, was not legitimate. To quantify
total Ca2+ handling even in such
failing hearts, we combined futile
Ca2+ cycling with
Ca2+ handling
VO2 and the internal
Ca2+ recirculation fraction via
the SR. We applied this method to the canine heart mechanoenergetics
before and after intracoronary ryanodine at nanomolar concentrations.
We found that total Ca2+ handling
per beat was halved after the ryanodine treatment from ~60 µmol/kg
left ventricle before ryanodine. We also found that futile
Ca2+ cycling via the SR increased
to >1 cycle/beat after ryanodine from presumably zero before
ryanodine. These results support the applicability of the present
method to the failing hearts with futile
Ca2+ cycling via the SR.
excitation-contraction coupling; contractility; postextrasystolic
potentiation; sarcoplasmic reticulum; ryanodine
EXCITATION-CONTRACTION (E-C) coupling requires
Ca2+ on the order of 20-100
µmol/kg myocardium to be bound with various intracellular Ca2+ binding sites, including
troponin C and calmodulin, in each cardiac contraction (1, 3, 6, 8, 10,
18, 22-24). These total Ca2+
handling (flux or transport) values have been obtained either biochemically or physiologically using isolated contracting myocardial preparations. However, these analytic methods cannot be used readily to
quantify total Ca2+ handling in a
beating whole heart (9, 29). Although the popular
Ca2+ transient methods detect
sarcoplasmic free Ca2+
concentrations on the order of 0.1-2 µmol/l in beating
myocardium and whole heart preparations, they represent only a small
fraction of the total Ca2+
handling, left unbound with Ca2+
binding sites (3, 5, 6, 11, 13, 16, 18, 22). Therefore, there has been
no appropriate method to quantify total Ca2+ handling in a beating whole heart.
We recently attempted to quantify total
Ca2+ handling in the left
ventricle (LV) of the canine beating whole heart by combining LV
myocardial O2 consumption
(VO2) and the so-called intracellular Ca2+ recirculation fraction
[RF, the fraction of total released
Ca2+ that is sequestered by the
sarcoplasmic reticulum (SR)
Ca2+-ATPase pump] (29). RF
was obtained from the exponential decay beat constant of the
postextrasystolic potentiation (PESP) (2, 9, 12, 14, 20, 21, 29, 33).
Assuming no futile Ca2+ cycling
via the SR in normal hearts, we were able to estimate total
Ca2+ handling in control and
enhanced contractile states produced with
Ca2+ and epinephrine (29).
However, we could not apply this method to the failing hearts produced
by infusing intracoronary ryanodine because this intervention led to
energy-wasting, futile Ca2+
cycling from the SR rendered leaky to
Ca2+ (9, 31). This is a serious
limitation of our previous method (29). Accordingly, we have developed
a new method that enables us to quantify total
Ca2+ handling in failing hearts
that includes the energy-wasting
Ca2+ handling due to futile
Ca2+ cycling.
This new integrative method was applied to the mechanoenergetics and RF
data of hearts treated with ryanodine to produce contractile failure
and, presumably, futile Ca2+
cycling (31) to estimate the feasibility of this method.
Background. Our cardiac
mechanoenergetic framework separates VO2 for
E-C coupling from the total VO2 of a beating
heart (15, 25-27, 31). E-C coupling VO2 is
primarily due to the energy requirement of
Ca2+ handling because
Na+ handling energy for membrane
excitation is negligibly small (1, 3, 25, 29). The present method
integrates this framework with the RF concept and the different molar
Ca2+:ATP stoichiometries of the
energetically major Ca2+ handling
routes (1, 3, 8, 9, 17, 30). Figure 1
depicts these major intracellular (internal) and transsarcolemmal (external) Ca2+ handling routes,
including the sarcolemmal and SR
Ca2+ channels, the
Ca2+- and
Na+-K+-ATPase
pumps, and the
Na+/Ca2+
exchangers (1, 3, 4, 8, 9, 11, 12, 17, 19, 22, 29, 30). Although we
neglected the Na+ handling energy
for membrane excitation, we retained the
Na+ handling energy by the
Na+-K+-ATPase
pump coupled with the
Na+/Ca2+
exchange (see below) (1, 3, 9, 17, 25, 29).
![]()
ABSTRACT
Top
Abstract
Introduction
Methods
Results & Discussion
Appendix
References
![]()
INTRODUCTION
Top
Abstract
Introduction
Methods
Results & Discussion
Appendix
References
![]()
METHODS
Top
Abstract
Introduction
Methods
Results & Discussion
Appendix
References

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Fig. 1.
Schematic diagram of energetically major
Ca2+ handling routes adopted in
our present total Ca2+ handling
model in the heart. A: without futile
Ca2+ cycling.
B: with futile
Ca2+ cycling. In
A and
B, sarcoplasm is surrounded by largest
rectangle indicating sarcolemma (SL). Sarcoplasmic reticulum (SR) is
shown by largest shaded oval. Thick solid loop passing through SR and
remaining within SL is intracellular
Ca2+ recirculation route via
Ca2+ pump and ryanodine-sensitive
Ca2+ release channel of SR. Thin
solid loop running across SL is the
Ca2+ extrusion route via the
Na+/Ca2+
exchanger and the dihydropyridine-sensitive, L-type
Ca2+ channel of the SL. Hatched
loop only in B is the futile
Ca2+ cycling via the SR.
Na+/Ca2+
exchange is assumed to be ionically and energetically coupled with
Na+-K+-ATPase
pump for Ca2+ and
Na+ homeostasis in each
steady-state beat. Ca2+ pump:
Ca2+-ATPase pump of SR.
Sarcolemmal Ca2+ ATPase pump is
not shown, under the assumption of its minor contribution. RF, internal
recirculation fraction of Ca2+ via
SR. XF, 1
RF: transsarcolemmal extrusion fraction of
Ca2+.
N, number of futile
Ca2+ cycling via SR.
N + 1 is total number of internal
Ca2+ cycling, where 1 cycle is
number of normal Ca2+ cycling via
the SR. A corresponds to
N = 0. B corresponds to
N > 0 due to the increased
Ca2+ permeability of the SR. Total
Ca2+, total amount of
Ca2+ handling (flux, or transport)
in each contraction. R, reactivity of an index of ventricular
contractility
(Emax) to total
Ca2+: proportional constant
relating Emax to
total Ca2+ handling.
RF decreases and 1
RF (the other fraction of total
Ca2+ transported
transsarcolemmally primarily by the
Na+/Ca2+
exchanger) reciprocally increases in various types of failing hearts
(9, 14, 20). A constant RF and
Ca2+ and
Na+ homeostasis are maintained in
steady-state beats. Otherwise, gradual changes in RF and internal
Ca2+ and
Na+ concentrations would alter
myocardial contractility over beats, disrupting the steady state (3,
12, 29). To maintain the Ca2+ and
Na+ homeostasis, the
Na+-K+
pump is coupled with the
Na+/Ca2+
exchange to remove the exchanged
Na+ influx (3).
Ca2+ handling VO2 will increase with an internal-to-external shift of Ca2+ handling because the Na+/Ca2+ exchange-Na+-K+ pump system has the 1 Ca2+:1 ATP stoichiometry in contrast to the 2 Ca2+:1 ATP stoichiometry of the SR Ca2+ pump (see below) (1, 3, 9, 29). In fact, our studies have shown that ryanodine infused at nanomolar (not micromolar) concentrations into the coronary circulation of the excised cross-circulated canine heart preparation stably decreased both LV contractility and RF without significantly decreasing Ca2+ handling VO2 (9, 31). Therefore, we suspected that not only total Ca2+ handling but also RF are major determinants of the Ca2+ handling VO2 (9, 29).
We previously proposed an original formula to calculate total Ca2+ handled or transported in the E-C coupling process from experimentally obtained Ca2+ handling VO2 and RF values in normal hearts with presumably no futile Ca2+ cycling (29). This formula was successfully applied for the first time to canine normal LVs in control and contractile states enhanced by intracoronary Ca2+ and epinephrine (29). However, we could not apply this formula legitimately to pathological hearts that are presumably wasting Ca2+ handling VO2 due to futile Ca2+ cycling via the Ca2+-leaky SR (9, 31). Therefore, we could not obtain an estimate of total Ca2+ handling in ryanodine-treated failing hearts, although we successfully estimated both Ca2+ handling VO2 and RF in these hearts (9). If futile Ca2+ cycling is occurring, total Ca2+ handling cannot simply be divided by RF into the internal and external fractions (9). Therefore, we developed the following new method.
New method. Figure 1A illustrates the Ca2+ handling model for our original method (29) and Fig. 1B illustrates that for our new method. Both have the internal and external Ca2+ handling routes in common. Both methods require Ca2+ handling VO2 and RF to divide the Ca2+ handling VO2 into the two major Ca2+ handling routes with the twofold different molar Ca2+:ATP stoichiometries (see below) (1, 3, 9, 17, 29, 30). However, the new method incorporates the futile Ca2+ cycling and the resultant extra VO2 into the original method (29), as shown by the third route (hatched loop) in Fig. 1B.
As shown in both Fig. 1A and Fig.
1B,
Ca2+ enters the cell via the
sarcolemmal Ca2+ channel and
simultaneously Ca2+ is released
into the sarcoplasm from the SR via its
Ca2+ release channel (3, 11). Most
of the Ca2+ is then bound to the
Ca2+ binding sites, including not
only troponin C to elicit cross-bridge cycling but also calmodulin,
mitochondria, etc. (3, 6, 10, 11, 13, 16, 18, 22-25). The SR
Ca2+ pump sequesters a
considerable fraction, which is the RF, of the total
Ca2+ by hydrolyzing ATP at a molar
stoichiometry of 2 Ca2+:1 ATP (1,
3, 4, 7, 8, 30). The remaining fraction (1
RF) of the total
Ca2+ is predominantly extruded by
the
Na+/Ca2+
exchanger and secondarily by the sarcolemmal
Ca2+ pump (although not shown, but
see below). The
Na+/Ca2+
exchange coupled with the
Na+-K+
pump maintains Ca2+ and
Na+ homeostasis at a molar
stoichiometry of 1 Ca2+:1 ATP (see
below) (1, 3, 4, 8, 17). Note that this stoichiometry is one-half that
of the SR Ca2+ pump. In other
words, the SR Ca2+ pump is
economical and the
Na+/Ca2+
exchange coupled with the
Na+-K+
pump is one-half economical, or twice as wasteful, in myocardial Ca2+ handling.
We have assumed that Ca2+ cycling via the SR during each contraction is only once in normal hearts; i.e., the Ca2+ transiently released and then sequestered by the SR Ca2+ pump during the same beat is no more released until the next beat (3, 29, 30). However, extra Ca2+ cycling is assumed to occur when the SR becomes leaky to Ca2+ in abnormal hearts such as those treated with ryanodine at nanomolar concentrations (3, 4, 9, 19, 31). Ryanodine at nanomolar concentrations bound to the SR Ca2+ release channel fixes the channel one-half open and makes it permeable to Ca2+ (in contrast to the complete channel closure achieved at micromolar concentrations of ryanodine) (4, 19, 31). In the Ca2+-leaky SR, part of the Ca2+ sequestered by the Ca2+ pump may leak out and be sequestered again during the same beat. Hence, the internal Ca2+ handling includes extra Ca2+ cycling (N) above and beyond the normal Ca2+ cycle in each beat. N > 0 represents the existence of the futile Ca2+ cycling (4, 31) as modeled in Fig. 1B. The new method described in this paper takes the futile Ca2+ cycling into consideration. As for the reactivity (R), see below.
Formulation. We propose the following equation to calculate the amount of ATP consumed for total Ca2+ handling that includes the futile Ca2+ cycling
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(1) |
In Eq. 1, (total
Ca2+ handling)RF gives the amount
(µmol/kg) of Ca2+ handling via
the internal route (i.e., SR), and (total
Ca2+ handling)(1
RF) gives
the amount (µmol/kg) of Ca2+
handling via the external route. These two terms were used in the
original method (Fig. 1A) that we
previously proposed to quantify total
Ca2+ handling in normal hearts,
which were assumed to have no futile Ca2+ cycling (29). The new term in
this equation, (total Ca2+
handling)N × RF, which is equal
to N × (total
Ca2+ handling)RF, estimates the
amount (µmol/kg) of Ca2+ handled
by futile cycling (N > 0) via the SR
(Fig. 1B).
The denominator 2 of two RF/2 terms in Eq. 1 is the coefficient 2 in the molar stoichiometry of 2 Ca2+:1 ATP of the SR
Ca2+ pump ATPase (1, 8, 30). The
value of 2 for both (total Ca2+
handling)RF and (total Ca2+
handling)N × RF terms in
Eq. 1 converts the respective
quantities of Ca2+ handling via
the SR into the respective amounts of ATP hydrolyzed for the normal and
futile Ca2+ handling by the SR
Ca2+ pump. The externally handled
term, (total Ca2+ handling)(1
RF), has 1, but not 2, in the denominator because its net
stoichiometry is simply 1 Ca2+:1
ATP as the result of the 3 Na+/Ca2+
exchange and the 3 Na+-2
K+-ATP pump (1, 8, 17). The
sarcolemmal Ca2+ pump, which
secondarily removes Ca2+ from the
cytoplasm, also has a 1 Ca2+:1 ATP
stoichiometry (3). As a result, RF/2 + (1
RF) + N × RF/2 is an overall
stoichiometric factor to convert total
Ca2+ handling into
Ca2+ handling ATP.
Mitochondrial oxidative phosphorylation starting with such metabolic substrates as lactate and pyruvate has a nominal stoichiometry of atomic ratio of 3 P:1 O or molecular ratio of 6 P:1 O2, where P is the high-energy phosphate of ATP. The P-to-O ratio increases by ~5% when the metabolic substrate is glucose and decreases by a similar percentage when the substrates are free fatty acids. Therefore, the P-to-O ratio falls between 2.83 and 3.17 in practice (25). On the average, 3 is a reasonable P-to-O ratio in blood-perfused hearts under aerobic conditions where the metabolic substrates are physiological mixtures of lactate, glucose, and free fatty acids (25). Table 1 is a numerical listing of the assumptions and parameters of the present Ca2+ handling model.
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Equation 1 is modified to obtain Ca2+ handling VO2
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(2) |
converts ATP in micromoles per kilogram to
VO2 in micromoles per kilogram.
Solving Eq. 2 for total Ca2+ handling yields
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(3) |
To use a unit of milliliters per 100 grams for Ca2+ handling VO2, we modified Eq. 3 to
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|
(4) |
Dividing both terms by Ca2+ handling VO2, Eq. 4 became
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|
(5) |
Figure 2A shows a family of curves derived from Eq. 5 with N as a parameter. This graph shows that total Ca2+ handling cannot be estimated even when both Ca2+ handling VO2 and RF are known unless we know N, which is not directly measurable.
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However, when we assumed N = 0 in the normal hearts, we could estimate (total Ca2+ handling)/(Ca2+ handling VO2) from RF (listed in Table 2), as indicated by the direction and order of arrows 1 and 2 in Fig. 2A. This is nothing but solving Eq. 5 for (total Ca2+ handling)/(Ca2+ handling VO2) by substituting the RF value and N = 0 into Eq. 5. We actually obtained (total Ca2+ handling)/(Ca2+ handling VO2) by solving Eq. 5 and multiplied it by Ca2+ handling VO2 to obtain the total Ca2+ handling listed in Table 2.
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The next question was how to estimate N in the ryanodine-treated, failing hearts, in which N was reasonably expected to be nonzero after ryanodine treatment at nanomolar concentrations (31). We introduced a new index of Ca2+ sensitivity or responsiveness of the contractile machinery to relate total Ca2+ handling to LV contractility (Emax) (28). We could not use the conventional Ca2+ sensitivity or responsiveness of the contractile machinery (3), because they already have their own specific definitions and are not applicable to our present study without confusion. These conventional ones refer to mechanical responses relative to sarcoplasmic free Ca2+ concentration (3), which we did not measure in the canine hearts subjected to the ryanodine studies (31). In contrast, our new index refers to the mechanical response relative to total Ca2+ handling (flux or transport) that we wanted to obtain. We designated the new index as the "reactivity of Emax to total Ca2+ handling" and abbreviated it to R. Figure 1, A and B, shows the R as a proportional constant between total Ca2+ handling and Emax.
Here, Emax is a mechanical load-independent index of ventricular contractility that Suga et al. proposed in 1973 (28; see also Ref. 26). Emax represents the maximum elastance of the LV chamber at the end of systole or the slope of the LV end-systolic pressure-volume relation line (26, 28). Emax has been considered to quantify the incremental number or amount of attached cross-bridges per unit increment in ventricular volume (26). Emax has been widely used as a practically useful index of contractility to characterize ventricular performance and mechanical energy (15, 25, 26).
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(6) |
Figure 2B shows a family of curves derived from Eq. 6 with R as a parameter. This graph shows that the response of Emax to total Ca2+ handling increases as an increasing function of R. This indicates that total Ca2+ handling can be uniquely determined from Emax if R is given and vice versa. Inversely, the R value could be determined if both Emax and total Ca2+ handling are given.
In the normal hearts, we obtained R values from their Emax and total Ca2+ handling (listed in Table 2), the latter having been estimated in Fig. 2A, as the intersection of arrows 3 and 4 in Fig. 2B.
We then assumed that R remained unchanged by ryanodine at nanomolar concentrations, taking advantage of its pharmacological specificity. It selectively fixes the ryanodine-sensitive Ca2+ channel of the SR one-half open without affecting the Ca2+ sensitivity of the troponin C and Ca2+ responsiveness of the contractile proteins (4, 19, 31). Therefore, we obtained total Ca2+ handling from the known Emax (as listed in Table 2) using the same R line as indicated by arrows 5 and 6 in Fig. 2B.
Then, this total Ca2+ handling was divided by its Ca2+ handling VO2 to obtain Ca2+ handling economy on the y-axis of Fig. 2A. Arrows 7 and 8 start from the Ca2+ handling economy and RF to obtain N as the intersection of these arrows. In reality, we solved Eqs. 5 and 6 for N by first substituting the same R as the normal R into Eq. 6 and then substituting RF and the obtained total Ca2+ handling into Eq. 5.
The method and steps we used to obtain the Ca2+ handling-related variables listed in Table 2 are described above. However, if we were not allowed to assume the unchanged R in the failing hearts, Eqs. 5 and 6 could not have been solved for R and N. For such a case, refer to APPENDIX.
Recirculation fraction. We obtained the RF in each contractile state by two different methods. The first method was the conventional one based on using the monotonically decaying PESP (12, 14, 20, 33), and the second one was our recently developed method to use the transient alternans PESP (2, 9, 21, 29). We had shown that RFs obtained by the two different methods were essentially the same in normal hearts (21). We had also shown that the same held either before or after ryanodine (9). However, RFs obtained by the two different methods were significantly decreased equally by ryanodine treatment (9). We utilized these previously obtained RF data (9) in the present study.
The details of RF determination were described in our previous paper (9). Briefly, we measured peak isovolumic pressures of regular beats and the 1st-6th postextrasystolic beats (PES1-6) of both monotonic and alternans decay types of PESP (9, 21). These pressures were normalized with respect to the regular beat pressure. The normalized pressure values of every set of PES1-6 of the monotonic type were fitted by an exponential equation
|
(7) |
e is the beat
constant of the exponential decay of the PESP (9). Those of the
alternans type were fitted by an exponential-sinusoidal
equation
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(8) |
s is the beat constant of the
sinusoidal decay. We had shown that time constant
e, but not
s, was related to RF (9, 21,
29).
We then calculated RF using RF = exp(
1/
e) (9, 12, 21,
29), where 1 means 1 beat and hence
1/
e is a dimensionless
(beat/beat) fraction of 1-beat interval relative to
e. Therefore,
exp(
1/
e) indicates
the decremental fraction of PESP (namely, RF, also dimensionless)
within one beat, as first shown by Morad and Goldman (12). This formula
has been used for years by other investigators (14, 33).
RF during steady-state beats cannot directly be assessed, but it can be
assessed during PESP intervening in the steady-state beats. In the
contemporary model of total Ca2+
handling, a constant RF in steady-state beats is assumed to hold during
the successive PESP (12, 14, 20, 33). The basic assumption to obtain RF
from the PESP decay has been that the contractility changes are
proportional to the beat-to-beat changes in the total
Ca2+ released into the sarcoplasm
and bound to Ca2+ binding sites
including troponin C (12, 14). This assumption seems reasonable on the
basis of the linear relationship between myocardial tension and total
Ca2+ bound intracellularly within
the working range of contractile force development (3, 6).
The constancy of RF over each monotonically decaying PESP has been
confirmed in a number of studies by the exponential curve fitting of
the decay (9, 14, 20, 21, 33). A constant RF is mathematically
equivalent to a constant ratio of PES pressure decay (12). This RF has
usually been obtained as the slope of a linear regression line of
contractility of the next beats
(PESx+1) on contractility of the
present beats (PESx) (12, 14, 20, 33), where x is the ordinal number of
the PES beats. The same RF is mathematically obtainable from the beat
constant
e of the exponential
decay of PESP by RF = exp(
1/
e) (12, 14, 20,
33).
Although these ratio and time constant methods are theoretically
equivalent, we preferred to use the time constant method because we
were able to directly fit a nonlinear curve to the PESP decay by the
least-squares method using DeltaGraph (Delta Point, Monterey, CA) on a
Power Macintosh computer (Apple Japan, Tokyo, Japan). We had obtained
RF values before and after ryanodine treatment (9). Their mean ± SD values obtained from both monotonic and alternans types of
PESP are listed in Table 2.
Ryanodine experiments.
We used the standard excised cross-circulated (blood-perfused) canine
heart preparation (15, 25). The details of our ryanodine experiments
were documented in the original paper (31). Briefly, ryanodine was
continuously infused at a constant rate of 1.4 ± 0.5 nmol/min into
the cross-circulated heart via the coronary arterial circulation for
~1 h (31). Because coronary flow was 51 ± 21 ml · min
1 · 100 g LV
1, we calculated the
intracoronary concentration of ryanodine to be 29 ± 13 nmol/l
coronary blood. Note that ryanodine at nanomolar (not micromolar)
concentrations did not abolish the
Ca2+ release function of the SR
(19, 31). Emax
gradually fell to nearly one-half of control over 1 h. We obtained
mechanoenergetics data, including LV pressure and volume,
Emax, total
VO2, and unloaded VO2,
in steady-state beats with constant atrial pacing. We found that
spontaneous PESP occurred sporadically. Basal metabolic
VO2 was measured under KCl arrest at the end of
each experiment. Ca2+ handling
VO2 was obtained by subtracting basal metabolic
VO2 from unloaded
VO2 at zero pressure-volume area.
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RESULTS AND DISCUSSION |
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To test the feasibility of the present method in cases with N > 0, we applied it to our previous mechanoenergetics data obtained in the ryanodine-treated failing canine LVs (9, 31). Table 2 lists the experimentally obtained mechanoenergetics data (31). The Emax and VO2 values are the mean ± SD values during control conditions before the ryanodine treatment and in the failing condition after the ryanodine treatment (9, 31).
The RF values in Table 2 are the data that we had calculated from the
beat constants (
e) of the
exponential decay of the monotonically decaying PESP and the
exponential decay component of the transient alternans PESP (9).
We assumed N = 0 in the control contractile state before ryanodine and N > 0 in the depressed contractile state after ryanodine treatment (9, 31). We also assumed that R remained virtually unchanged by the ryanodine treatment at nanomolar concentrations (4, 9, 31). The bases of these assumptions are described in METHODS.
Table 2 lists all the resultant Ca2+-related values calculated from the mechanoenergetics and RF data by the present method. Although the RF values obtained from the monotonic and alternans PESPs were not significantly different (9), we combined these RF values separately with the same representative set of mechanoenergetic data as shown by the two PESP-type columns (patterns A and C) in Table 2. The resultant total Ca2+ handling values for both RF values are comparable either before or after ryanodine. The resultant total Ca2+ handling values were considerably smaller after ryanodine than before. Moreover, these total Ca2+ handling values in both control and ryanodine-treated hearts fell within the physiological range (20-100 µmol/kg) documented in the literature (1, 3, 6, 8, 10, 18, 22-24).
We obtained total Ca2+ handling of
56 (from pattern A) and 60 (from
pattern C) µmol/kg at a baseline
Emax of 4.2 mmHg · ml
1 · 100 g. This Emax
value is approximately one-third to one-fourth of the maximum
Emax with high
doses of intracoronary Ca2+ or
catecholamines (15, 28). Considering the maximum
Ca2+ binding capacity of
20-100 µmol/kg of intramyocardial sites including troponin C and
calmodulin (3, 6, 10, 16, 22, 23), the ~60 µmol/kg of
Ca2+ could be interpreted as a
rather high value for the baseline Emax.
However, our present Ca2+ handling values are dynamic values calculated on a per-beat basis, whereas the apparently maximum Ca2+ binding capacity values were biochemically determined under steady-state conditions. The rate constants of Ca2+ binding to troponin C and the other Ca2+ binding sites (18, 22) indicate that Ca2+ binding to them is not immediate after the Ca2+ release. This suggests that part of the released Ca2+ may be removed before effective binding to the Ca2+ binding sites. Our simulation study of Ca2+ kinetics, similar to that of Robertson et al. (18), has shown that a significant fraction (20-30%) of the total released Ca2+ has been sequestered by the SR by the time of one-half peak force development (13). Therefore, our total Ca2+ handling values could be considered reasonable if part of the total released Ca2+ is removed by the SR Ca2+ pump immediately after its release and is not used effectively for E-C coupling (3, 7).
The high-affinity Ca2+ binding sites (50-70 µmol/kg, 2 Ca2+ per 1 troponin C molecule) of troponin C (25-35 µmol/kg) seem to be almost fully saturated even at a low diastolic free Ca2+ level (3, 6, 10, 23). Therefore, the total Ca2+ handling we obtained appears to be related to the beat-to-beat changes in the amount of Ca2+, which are proportional to contractile force development in excess of the stably bound amount of Ca2+ independent of the twitch force development. The beat-to-beat change in Ca2+ includes that bound to the low-affinity Ca2+-specific sites (25-35 µmol/kg, 1 Ca2+ per 1 troponin C molecule) of troponin C as well as other Ca2+ bound to calmodulin and all other Ca2+ binding sites on a per-beat basis (3, 7).
Because we assumed the same R after ryanodine (see Table 2) as that before ryanodine, the resultant total Ca2+ handling was proportional to Emax before and after ryanodine (Fig. 2B). Despite the considerably decreased total Ca2+ handling from 56-60 to 31-33 µmol/kg after ryanodine, Ca2+ handling VO2 was only little decreased after ryanodine, as seen in Table 2. This disproportionately high value for Ca2+ handling VO2 in the ryanodine-treated heart is now accounted for by the combination of the significantly decreased RF and markedly increased N despite the nearly halved total Ca2+ handling associated directly with E-C coupling.
The present method has several limitations. First of all, the present model may appear too simple to calculate accurately total Ca2+ handling because of the numerous assumptions incorporated into the model. However, we have included the major ATP-consuming processes of Ca2+ handling and neglected minor ones on the basis of the contemporary knowledge (1, 3, 4, 8, 9, 11, 12, 17, 19, 22, 29, 30). Although the new knowledge of other minor Ca2+ handling processes is available (3, 11, 22), it cannot readily be incorporated into our model, because it was obtained by reductionistic methodology in isolated, but not in situ, myocytes of animals other than dogs. For example, we neglected the contribution of the reverse mode of the Na+/Ca2+ exchanger to the transsarcolemmal Ca2+ entry according to its relatively small contribution in normal rabbit myocytes (3). However, this contribution is yet unknown in canine hearts. Therefore, even if we adopt reductionistic knowledge obtained in rabbit myocytes into the present model, this may not guarantee improvement of the model. Nevertheless, the present study warrants further efforts to improve the integrative approach toward better understanding of myocardial Ca2+ handling by integrative methods.
Despite this limitation, we would consider that our estimates of total Ca2+ handling in Table 2 appear reasonably realistic in the light of the literature data (1, 3, 6, 8, 10, 18, 22-24). Any of Eqs. 1-5 indicates mathematically that a relatively small error in RF, N, and Ca2+ handling VO2 due to our neglect of minor Ca2+ handling processes would produce a comparably small error in total Ca2+ handling.
In relation to this limitation, we assumed N = 0 in the normal hearts before the ryanodine treatment and the same R value before and after ryanodine to estimate total Ca2+ handling. As described in Formulation and APPENDIX, if we had not used these assumptions, we could not have obtained estimates of N, R, and total Ca2+ handling values after ryanodine treatment. However, if one were satisfied with mechanoenergetic differentiation between normal and failing hearts, the assumptions for N and R are not required. Then, comparison of the R-N relation between them would be a very helpful new method (Fig. 3C).
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Second, we used mechanoenergetics and PESP data documented only in our previous studies (9, 31) to test the feasibility of our new method. We had already applied the part with N = 0 to a baseline Emax in a different group of normal hearts (29). There, the representative data were Emax of 4.7 mmHg/ml, Ca2+ handling VO2 of 0.011 ml O2/beat, both per 100 grams, and RF of 0.55. All these values are close to the present control data listed in Table 2. N was assumed to be 0 in the normal hearts in control and enhanced contractile states with Ca2+ and epinephrine (29) as in the normal hearts in control contractile state before ryanodine in the present study. Then, the calculated total Ca2+ handling was 40 µmol/kg, which is of the same order as the present control value for total Ca2+ handling. This similarity among different groups of normal hearts supports the feasibility of the present method for the hearts with N = 0. However, the feasibility of the formula with N > 0 was tested for the first time in this study. We must admit that the present method remains to be tested using various types of failing hearts whose Ca2+ handling processes are abnormal, although some limitation remains, as explained in APPENDIX.
A third limitation would be our assumption that residual cross-bridge cycling does not contribute to the Ca2+ handling VO2. Although residual cross-bridge cycling appeared to contribute considerably to unloaded VO2 in rabbit hearts (34), we have obtained evidence supporting the view that residual cross-bridge cycling energy, if any, is negligibly small in the Ca2+ handling VO2 of canine blood-perfused hearts (32).
Other limitations are that we only used average RF and mechanoenergetics data to calculate total Ca2+ handling and that the intracoronary ryanodine concentrations were, at most, 40 nmol/l. Because we only used PESPs following spontaneous extrasystoles, which occurred sporadically, we could not deal with a larger number of matched sets of mechanoenergetics and RF data. Therefore, we had to use the average data as listed in Table 2 as representative values. As for the ryanodine concentration, Emax gradually decreased to one-half of the control over 1 h during continuous intracoronary infusion of ryanodine at 1.4 nmol/min (31). Emax was already low enough to judge the heart to be in a failing state (31). Moreover, end-diastolic pressure started to rise in isovolumic contractions at a fixed intermediate volume (31). We could not obtain any stable data thereafter. Because of these limitations, future controlled studies are warranted.
In conclusion, our present heart-level method may contribute to a better understanding of total Ca2+ handling in ryanodine-treated, failing hearts characterized by futile Ca2+ cycling. We consider this to be so because no better methods are yet available to achieve the same goal. When using this method, one must realize the limitations remaining to be overcome. The utility of this integrative analysis method may be increased by conquering these limitations.
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APPENDIX |
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We eliminated total Ca2+ handling by combining Eqs. 5 and 6 and obtained
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|
(9) |
Therefore, we rewrote Eq. 9 as
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|
(10) |
In Eq. 10, both O2 cost of Emax and RF are measurable, but N and R are unknown and to be obtained. Rearranging Eq. 10 yields
|
(11) |
Figure 3C shows four specific R-N relations for the representative data sets of O2 cost of Emax and RF (listed in Table 2) in the normal hearts and the ryanodine-treated, failing hearts. The two upper lines are of the failing hearts. The two lower lines are of the normal hearts. In both pairs, the upper line corresponds to the pattern C data and the lower one to the pattern A data.
Comparison of these two pairs of the R-N relations could explicitly differentiate the ryanodine-treated failure from the control even if we do not know the working R-N points on the individual relations. This comparison does not require such assumptions as N = 0 in the normal hearts and the unchanged R despite ryanodine treatment. Therefore, the R-N relation even without specifying R and N may help quantify total Ca2+ handling in any heart and be used to compare it among different hearts. However, unless we know R and N values, we could not estimate total Ca2+ handling from Ca2+ handling VO2.
The steps we took to obtain the R and N in the ryanodine-treated, failing hearts in Fig. 2, A and B, are exemplified in Fig. 3C. The assumed N = 0 and the resultant R in the normal canine hearts correspond to the x-axis intercept of a control R-N line (either pattern A or pattern C). The assumed unchanged R in the failing hearts corresponds to arrow 9 in Fig. 3C. Arrow 10 starting from the intersection of arrow 9 and a ryanodine R-N line (either pattern A or pattern C) yields the y-axis intercept. This intercept is the N of the failing heart. Once R and N are thus obtained, Fig. 2, A and B, gives us an estimate of total Ca2+ handling.
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ACKNOWLEDGEMENTS |
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We thank Kimikazu Hosokawa for animal care and Eiko Oka and Masayo Ogawa for clerical and computer work.
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FOOTNOTES |
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This study was partly supported by Grants-in-Aid for Scientific Research (07508003, 08670052, 09670053, 09307029, 09470009, 10770307, 10558136, 10877006) from the Ministry of Education, Science, Sports and Culture; a Research Grant for Cardiovascular Diseases (7C-2) from the Ministry of Health and Welfare; 1997-1998 Frontier Research Grants for Cardiovascular System Dynamics from the Science and Technology Agency; and research grants from the Ryobi Teien Foundation and the Mochida Memorial Foundation, all of Japan.
Address reprint requests to H. Suga.
Received 7 July 1997; accepted in final form 29 July 1998.
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REFERENCES |
|---|
|
|
|---|
1.
Alpert, N. R.,
E. M. Blanchard,
and
L. A. Mulieri.
Tension-independent heat in rabbit papillary muscle.
J. Physiol. (Lond.)
414:
433-453,
1989
2.
Araki, J.,
M. Takaki,
T. Matsushita,
H. Matsubara,
and
H. Suga.
Postextrasystolic transient contractile alternans in canine hearts.
Heart Vessels
9:
241-248,
1994[Medline].
3.
Bers, D. N.
Excitation-Contraction Coupling and Cardiac Contractile Force. Dordrecht, Germany: Kluwer Academic, 1991.
4.
Bers, D. M.,
and
J. H. B. Bridge.
Relaxation of rabbit ventricular muscle by Na-Ca exchange and sarcoplasmic reticulum Ca-pump. Ryanodine and voltage sensitivity.
Circ. Res.
65:
334-342,
1989
5.
Endoh, M.
The effects of theophylline on aequorin light transients and force in the isolated dog right ventricular myocardium.
J. Mol. Cell. Cardiol.
26:
87-98,
1994[Medline].
6.
Fabiato, A.
Calcium-induced release of calcium from the cardiac sarcoplasmic reticulum.
Am. J. Physiol.
245 (Cell Physiol. 14):
C1-C14,
1983
7.
Feher, J. J.,
N. H. Manson,
and
J. L. Poland.
The rate and capacity of calcium uptake by sarcoplasmic reticulum in fast, slow, and cardiac muscle: effects of ryanodine and ruthenium red.
Arch. Biochem. Biophys.
265:
171-182,
1988[Medline].
8.
Hasenfuss, G.,
L. A. Mulieri,
P. D. Allen,
H. Just,
and
N. R. Alpert.
Influence of isoproterenol and ouabain on excitation-contraction coupling, cross-bridge function, and energetics in failing human myocardium.
Circulation
94:
3155-3160,
1996
9.
Hata, Y.,
J. Shimizu,
S. Hosogi,
H. Matsubara,
J. Araki,
T. Ohe,
M. Takaki,
T. Takasago,
T. W. Taylor,
and
H. Suga.
Ryanodine decreases internal Ca2+ recirculation fraction of the canine heart as studied by postextrasystolic transient alternans.
Jpn. J. Physiol.
47:
521-530,
1997[Medline].
10.
Hofman, P. A.,
and
F. Fuchs.
Bound calcium and force development in skinned cardiac muscle bundles: effect of sarcomere length.
J. Mol. Cell. Cardiol.
20:
667-677,
1988[Medline].
11.
Lee, J. A.,
and
D. G. Allen.
Modulation of Cardiac Calcium Sensitivity. A New Approach to Increasing the Strength of the Heart. Oxford, UK: Oxford Medical, 1993.
12.
Morad, M.,
and
Y. Goldman.
Excitation-contraction coupling in heart muscle: membrane control of development of tension.
Prog. Biophys. Mol. Biol.
27:
257-313,
1973.
13.
Namba, T.,
M. Takaki,
J. Araki,
K. Ishioka,
T. Akashi,
L. Y. Zhao,
T. Matsushita,
H. Ito,
W. Fujii,
H. Matsubara,
and
H. Suga.
Ca2+ sensitivity of contractile machinery and Ca2+ handling energy. Simulation.
Jpn. Heart J.
34:
601-616,
1993[Medline].
14.
Noble, M. I. M.,
and
W. A. Seed
(Editors).
The Interval-Force Relationship of the Heart. Bowditch Revisited. Cambridge, UK: Cambridge University Press, 1992.
15.
Ohgoshi, Y.,
Y. Goto,
O. Kawaguchi,
H. Yaku,
H. Takaoka,
K. Hata,
T. Takasago,
and
H. Suga.
Epinephrine and calcium have similar oxygen costs of contractility.
Heart Vessels
7:
123-132,
1992[Medline].
16.
Pierce, G. N.,
K. D. Philipson,
and
G. A. Langer.
Passive calcium-buffering capacity of a rabbit ventricular homogenate preparation.
Am. J. Physiol.
249 (Cell Physiol. 18):
C248-C255,
1985
17.
Reeves, J. P.,
and
C. C. Hale.
The stoichiometry of the cardiac sodium-calcium exchange system.
J. Biol. Chem.
259:
7733-7739,
1984
18.
Robertson, S. P.,
J. D. Johnson,
and
J. D. Potter.
The time-course of Ca2+ exchange with calmodulin, troponin, parvalbumin, and myosin in response to transient increases in Ca2+.
Biophys. J.
34:
559-569,
1981
19.
Rousseau, E.,
J. S. Smith,
and
G. Meissner.
Ryanodine modifies conductance and gating behavior of single Ca2+ channel.
Am. J. Physiol.
253 (Cell Physiol. 22):
C364-C368,
1987
20.
Seed, W. A.,
M. I. M. Noble,
J. M. Walker,
G. A. H. Miller,
J. Pidgeon,
D. Redwood,
R. Wanless,
M. R. Franz,
M. Schettler,
and
J. Schaefer.
Relationships between beat-to-beat interval and the strength of contraction in the healthy and diseased human heart.
Circulation
70:
799-805,
1984
21.
Shimizu, J.,
M. Takaki,
K. Kohno,
J. Araki,
H. Matsubara,
and
H. Suga.
Sinusoidal and exponential decays of postextrasystolic transient alternans in excised blood-perfused canine hearts.
Jpn. J. Physiol.
45:
837-848,
1995[Medline].
22.
Sipido, K. R.,
and
W. G. Wier.
Flux of Ca2+ across the sarcoplasmic reticulum of guinea-pig cardiac cells during excitation-contraction coupling.
J. Physiol. (Lond.)
435:
605-630,
1991
23.
Solaro, R. J.,
R. M. Wise,
J. S. Shiner,
and
F. N. Briggs.
Calcium requirements for cardiac myofibrillar activation.
Circ. Res.
34:
525-530,
1974
24.
Somlyo, A. V.,
H. Shuman,
G. McClellan,
and
A. P. Somlyo.
Comparison of sarcoplasmic reticulum in situ by electron probe. X-ray microanalysis.
Nature
268:
556-558,
1977[Medline].
25.
Suga, H.
Ventricular energetics.
Physiol. Rev.
70:
247-277,
1990
26.
Suga, H.
Paul Dudley White International Lecture: Cardiac performance as viewed through the pressure-volume window.
Jpn. Heart J.
35:
263-280,
1994[Medline].
27.
Suga, H., Y. Goto, O. Kawaguchi, K. Hata, T. Takasago, A. Saeki,
and T. W. Taylor. Ventricular perspective on efficiency.
Basic Res. Cardiol. 88, Suppl. 2: 43-65, 1993.
28.
Suga, H.,
K. Sagawa,
and
A. A. Shoukas.
Load independence of the instantaneous pressure-volume ratio of the canine left ventricle and effects of epinephrine and heart rate on the ratio.
Circ. Res.
32:
314-322,
1973
29.
Syuu, Y.,
J. Araki,
S. Lee,
S. Suzuki,
J. Mizuno,
S. Mohri,
T. Mikane,
J. Shimizu,
M. Takaki,
and
H. Suga.
Effects of Ca2+ and epinephrine on Ca2+ recirculation fraction and total Ca2+ handling in canine left ventricles.
Jpn. J. Physiol.
48:
123-132,
1998[Medline].
30.
Tada, M.,
and
A. M. Katz.
Phosphorylation of the sarcoplasmic reticulum and sarcolemma.
Annu. Rev. Physiol.
44:
401-423,
1982[Medline].
31.
Takasago, T.,
Y. Goto,
O. Kawaguchi,
K. Hata,
A. Saeki,
T. Nishioka,
and
H. Suga.
Ryanodine wastes oxygen consumption for Ca2+ handling in the dog heart. A new pathological heart model.
J. Clin. Invest.
92:
823-830,
1993.
32.
Takasago, T.,
Y. Goto,
O. Kawaguchi,
K. Hata,
A. Saeki,
T. W. Taylor,
T. Nishioka,
and
H. Suga.
2,3-Butanedione monoxime suppresses excitation-contraction coupling in the canine blood-perfused left ventricle.
Jpn. J. Physiol.
47:
205-215,
1997[Medline].
33.
Ter Keurs, H. E. D. J.,
W. D. Gao,
H. Bosker,
A. J. Drake-Holland,
and
M. I. M. Noble.
Characterization of decay of frequency induced potentiation and post-extrasystolic potentiation.
Cardiovasc. Res.
24:
903-910,
1990[Medline].
34.
Yaku, H.,
B. K. Slinker,
T. Mochizuki,
B. H. Lorell,
and
M. M. Lewinter.
Use of 2,3-butanedione monoxime to estimate nonmechanical
O2 in rabbit hearts.
Am. J. Physiol.
265 (Heart Circ. Physiol. 34):
H834-H842,
1993
35.
Yamaguchi, H.,
M. Takaki,
H. Matsubara,
S. Yasuhara,
and
H. Suga.
Constancy and variability of contractile efficiency as a function of calcium and cross-bridge kinetics: simulation.
Am. J. Physiol.
270 (Heart Circ. Physiol. 39):
H1501-H1508,
1996
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