We extended the model of the ventricular myocyte by
Winslow et al. (Circ. Res. 1999, 84:571-586)
by
incorporating equations for Ca2+ and Mg2+
buffering and transport by ATP and ADP and equations for MgATP regulation of ion transporters (Na+-K+ pump,
sarcolemmal and sarcoplasmic Ca2+ pumps). The results
indicate that, under normal conditions, Ca2+ binding by
low-affinity ATP and diffusion of CaATP may affect the amplitude and
time course of intracellular Ca2+ signals. The model also
suggests that a fall in ATP/ADP ratio significantly reduces
sarcoplasmic Ca2+ content, increases diastolic
Ca2+, lowers systolic Ca2+, increases
Ca2+ influx through L-type channels, and decreases the
efficiency of the Na+/Ca2+ exchanger in
extruding Ca2+ during periodic voltage-clamp stimulation.
The analysis suggests that the most important reason for these changes
during metabolic inhibition is the down-regulation of the sarcoplasmic
Ca2+-ATPase pump by reduced diastolic MgATP levels. High
Ca2+ concentrations developed near the membrane might have
a greater influence on Mg2+, ATP, and ADP concentrations
than that of the lower Ca2+ concentrations in the bulk
myoplasm. The model predictions are in general agreement with
experimental observations measured under normal and pathological conditions.
 |
GLOSSARY |
Abbreviations
| ATP |
= |
adenosine triphosphate |
| ADP |
= |
adenosine diphosphate |
| SR |
= |
sarcoplasmic reticulum |
| JSR |
= |
junctional sarcoplasmic reticulum |
| NSR |
= |
network sarcoplasmic reticulum |
| RyR |
= |
ryanodine receptor |
Volumes, areas, and capacity
| Vss |
= |
subspace volume |
| Vmyo |
= |
myoplasmic volume |
| VJSR |
= |
junctional SR volume |
| Acap |
= |
capacitive membrane area |
| Csc |
= |
specific membrane capacity |
| F |
= |
Faraday constant |
Membrane currents
| INa |
= |
Na+ current |
| IKr |
= |
rapid-activating delayed rectifier K+ current |
| IKs |
= |
slow-activating delayed rectifier K+ current |
| Ito1 |
= |
transient outward K+ current |
| IK1 |
= |
time-independent K+ current |
| IKp |
= |
plateau K+ current |
| INaCa |
= |
Na+-Ca2+ exchanger current |
| I*NaK |
= |
modified Na+-K+ pump current |
| I*p(Ca) |
= |
modified sarcolemmal Ca2+ pump current |
| ICa,b |
= |
Ca2+ background current |
| INa,b |
= |
Na+ background current |
| ICa |
= |
L-type Ca2+ current |
| ICa,K |
= |
K+ current through L-type Ca2+ channel |
Concentrations
| [Na]0 |
= |
extracellular Na+ concentration |
| [K]0 |
= |
extracellular K+ concentration |
| [Ca]0 |
= |
extracellular Ca2+ concentration |
| [Na]i |
= |
intracellular Na+ concentration |
| [K]i |
= |
intracellular K+ concentration |
| [Ca]ss |
= |
free subspace Ca2+ concentration |
| [Ca]i |
= |
free myoplasmic Ca2+ concentration |
| [Ca]JSR |
= |
JSR Ca2+ concentration |
| [Ca]NSR |
= |
NSR Ca2+ concentration |
| [Mg]tot |
= |
total Mg2+ concentration |
| [Mg]ss |
= |
free subspace Mg2+ concentration |
| [Mg]i |
= |
free myoplasmic Mg2+ concentration |
| [ATP]tot |
= |
total ATP concentration |
| [ATP]ss |
= |
free subspace ATP concentration |
| [ATP]i |
= |
free myoplasmic ATP concentration |
| [CaATP]ss |
= |
subspace concentration of Ca2+-bound ATP |
| [CaATP]i |
= |
myoplasmic concentration of Ca2+-bound ATP |
| [MgATP]ss |
= |
subspace concentration of Mg2+-bound ATP |
| [MgATP]i |
= |
myoplasmic concentration of Mg2+-bound ATP |
| [ADP]tot |
= |
total ADP concentration |
| [ADP]ss |
= |
free subspace ADP concentration |
| [ADP]i |
= |
free myoplasmic ADP concentration |
| [CaADP]ss |
= |
subspace concentration of Ca2+-bound ADP |
| [CaADP]i |
= |
myoplasmic concentration of Ca2+-bound ADP |
| [MgADP]ss |
= |
subspace concentration of Mg2+-bound ADP |
| [MgADP]i |
= |
myoplasmic concentration of Mg2+-bound ADP |
Fluxes
| Jxfer |
= |
Ca2+ flux from subspace to myoplasm |
| Jrel |
= |
RyR channel Ca2+ flux |
| J*up |
= |
modified Ca2+ uptake into NSR by SR Ca2+-ATPase
pump |
| Jtrpn |
= |
buffering of Ca2+ by troponin C |
J |
= |
Mg2+ flux from subspace to myoplasm |
J |
= |
CaATP flux from subspace to myoplasm |
J |
= |
MgATP flux from subspace to myoplasm |
J |
= |
CaADP flux from subspace to myoplasm |
J |
= |
MgADP flux from subspace to myoplasm |
Time constants
xfer |
= |
time constant for transfer of Ca2+ from subspace to
myoplasm |
  |
= |
time constant for transfer of Mg2+ from subspace to
myoplasm |
  |
= |
time constant for transfer of CaATP from subspace to myoplasm |
  |
= |
time constant for transfer of MgATP from subspace to myoplasm |
  |
= |
time constant for transfer of CaADP from subspace to myoplasm |
  |
= |
time constant for transfer of MgADP from subspace to myoplasm |
Dissociation and rate constants
K |
= |
Ca2+-ATP dissociation constant |
k |
= |
Ca2+ on-rate constant for ATP |
k |
= |
Ca2+ off-rate constant for ATP |
K |
= |
Mg2+-ATP dissociation constant |
k |
= |
Mg2+ on-rate constant for ATP |
k |
= |
Mg2+ off-rate constant for ATP |
K |
= |
Ca2+-ADP dissociation constant |
k |
= |
Ca2+ on-rate constant for ADP |
k |
= |
Ca2+ off-rate constant for ADP |
K |
= |
Mg2+-ADP dissociation constant |
k |
= |
Mg2+ on-rate constant for ADP |
k |
= |
Mg2+ off-rate constant for ADP |
 |
INTRODUCTION |
A number of mathematical models have been developed to investigate
Ca2+ signaling in cardiac muscle cells (Robertson et al.,
1981
; Michailova and Spassov, 1992
; Stern, 1992
; Amstudz et al., 1996
;
Keizer and Levine, 1996
; Langer and Peskoff, 1996
; Negroni and Lascano,
1996
; Soeller and Cannell, 1997
; Jafri et al., 1998
; Hunter et al., 1998
; Nygren et al., 1998
; Peskoff and Langer, 1998
; Winslow et al.,
1998
, 1999
; Dawson et al., 1999
; Michailova et al., 1999
; Rice et al.,
1999
; Zoghbi et al., 2000
). However, these models cannot be used to
predict how the binding and transport of Ca2+ and
Mg2+ by the mobile buffers, ATP and ADP, or a fall in
[ATP]tot/[ADP]tot ratio might modulate
intracellular Ca2+, Mg2+, Na+, and
K+ concentrations, ion pumps and currents, or, conversely,
how changes in free Ca2+ concentrations during excitation
could alter free and bound concentrations of ATP and ADP. Recently, ATP
diffusion and Ca2+ and Mg2+ exchange with ATP
have been introduced in models of smooth muscle cells (Kargacin and
Kargacin, 1997
) and skeletal muscle cells (Baylor and Hollingworth,
1998
). Cardiac energetics (metabolism of high-energy phosphates,
glycogen metabolism, and lactate transport) and pH regulation have also
been integrated with electrophysiological models (Ch'en et al., 1997
,
1998
; Shaw and Rudy, 1997
).
Winslow et al. (1999)
modified the model of Jafri et al. (1998)
for
guinea pig ventricular cells to study the mechanisms of Ca2+ handling in the canine midmyocardial ventricular
myocytes. This integrative model incorporated: 1) membrane ion currents
from the Luo-Rudy phase II ventricular cell model (Luo and Rudy,
1994
); 2) the formulation of Jafri et al. (1998)
for the L-type
Ca2+ current that exhibits the mode-switching behavior
observed by Imredy and Yue (1994)
; 3) SR Ca2+ release from
RyR channels described in the Keizer and Levine (1996)
model with
receptor adaptation; 4) a subsarcolemmal space; 5) Ca2+
buffering by low- and high-affinity Ca2+ binding sites on
troponin, and Ca2+ buffering by calmodulin and
calsequestrin. In the model of Winslow et al. (1999)
, calculated
subsarcolemmal Ca2+ could reach high levels (~30 µM)
during excitation and rose more rapidly than myoplasmic
Ca2+ (~0.5-0.6 µM). It faithfully reproduced measured
Ca2+ transients in normal and failing canine ventricular
myocytes (O'Rourke et al., 1999
).
In this study, we extend the model of Winslow et al. (1999)
by
incorporating equations for Ca2+ and Mg2+
buffering and transport by ATP and ADP and equations describing ATP (or
MgATP) regulation of ion transporters (Na+-K+
ATPase pump, sarcolemmal Ca2+-ATPase pump, SR
Ca2+-ATPase pump). Our results support the hypothesis that,
under normal conditions, Ca2+ binding by low-affinity
mobile buffer ATP and diffusion of Ca2+-bound ATP (CaATP)
may contribute to the amplitude and time course of intracellular
Ca2+ signals. The inclusion of ATP and ADP buffering
slightly decreased the peak of the myoplasmic Ca2+
transient computed in response to periodic voltage-clamp stimuli. The
addition of CaATP diffusion slightly decreased the peak and accelerated
the relaxation of the Ca2+ transient in the subspace.
Metabolic changes (a fall in
[ATP]tot/[ADP]tot ratio) significantly
reduced SR Ca2+ content, increased diastolic
Ca2+ levels, and decreased systolic Ca2+ levels
computed in response to periodic voltage-clamp stimuli. As a result,
Ca2+ influx through L-type Ca2+ channels
increased while the efficiency of Ca2+ extrusion by the
Na+/Ca2+ exchanger decreased. The main reason
for these changes was reduced Ca2+ uptake by the SR
Ca2+-ATPase (SERCA2a pump) due to decreased diastolic MgATP
levels during metabolic inhibition. In ventricular myocytes, high
Ca2+ concentrations developed near the membrane might
influence Mg2+, ATP, and ADP concentrations more
significantly than the negligible alterations in these concentrations
stimulated by low myoplasmic Ca2+.
 |
MATHEMATICAL MODEL |
The overall scheme of the model is shown in Fig.
1. (See Glossary for the notations of the
parameters used throughout the study.) We provide only the additional
or modified equations necessary to include ATP and ADP as
Ca2+ and Mg2+ buffers and transporters, and ATP
as Na+-K+, sarcolemmal, and SR Ca2+
pumps regulator. The remaining equations were the same as those in the
original paper of Winslow et al. (1999)
with the corrections as given
on the author's web site.
Experimental data suggest that the SR is not accessible to the mobile
buffers, ATP and ADP (Bers, 1991
; Carmeliet, 1999
). Therefore, in the
model, ATP and ADP are free to react and diffuse within the subspace
and bulk myoplasm but not in the SR (Fig. 1). It was also assumed that
the total ATP and ADP concentrations in the subspace
([ATP]tot
ss, [ADP]tot
ss) and bulk myoplasm ([ATP]tot
i, [ADP]tot
i) are
equal, spatially uniform, and remain constant during excitation, i.e.,
|
(1)
|
|
(2)
|
The buffering of Ca2+ and Mg2+ by ATP in
the subspace is given by the following equations:
|
(3)
|
|
(4)
|
|
(5)
|
where k+ and k
are
the corresponding on-rate and off-rate binding constants. The equations
for the bulk myoplasm are similar:
|
(6)
|
|
(7)
|
|
(8)
|
CaATP and MgATP fluxes (Fig. 1) are given by
|
(9)
|
|
(10)
|
For the subspace, adjustment of ATP fluxes by a factor of
(Vmyo/Vss) is necessary
to account for the different volumes of myoplasm
(Vmyo) and subspace
(Vss).
Similar equations for the Ca2+ and Mg2+
exchange with ADP in the subspace and bulk myoplasm can be written as
|
(11)
|
|
(12)
|
|
(13)
|
|
(14)
|
|
(15)
|
|
(16)
|
CaADP and MgADP fluxes (Fig. 1) are given by
|
(17)
|
|
(18)
|
In the model, we assume that the transfer of free and bound ATP
and ADP from the subspace to the myoplasm occurs at the same rate. The
changes in free Mg2+ concentration during
excitation in the subspace are described by
|
(19)
|
and in the bulk myoplasm by
|
(20)
|
The transfer flux of Mg2+ from subspace to
myoplasm (Fig. 1) is given by
|
(21)
|
ATP and ADP not only buffer and transport
Ca2+ and Mg2+ ions but also have well-known
regulatory functions in the cell (Bers, 1991
; Leyssens et al., 1996
;
Carmeliet, 1999
). In cardiac myocytes, ATP (as MgATP) drives a number
of enzymes, channels (ATP-sensitive K+ channels), and
transporters (Na+-K+ ATPase pump, sarcolemmal
Ca2+- ATPase pump, SR Ca2+-ATPase pump)
(Noma, 1983
; Fozzard and Lipkind, 1995
; Shaw and Rudy, 1997
; Yokoshiki
et al., 1998
; Carmeliet, 1999
). To simulate transporter ATP regulation,
we modified the equations of Winslow et al. (1999)
for
Na+-K+ pump current
(INaK), sarcolemmal Ca2+ pump
current (Ip(Ca)), and SR Ca2+ ATPase
pump (Jup):
|
(22)
|
|
(23)
|
|
(24)
|
where
|
(25)
|
and [MgATP]i0 is the resting myoplasmic MgATP
concentration in normal conditions
([ATP]tot = 7 mM, [ADP]tot = 5 µM, free Mg2+ = 1 mM).
The equations for the [Ca]ss and [Ca]i in
the model of Winslow et al. (1999)
were modified, taking into account
that now ATP and ADP buffer Ca2+ and regulate
ion pumps:
|
(26)
|
|
(27)
|
where
ss is a rapid buffering approximation factor
for calmodulin in the subspace, and
i is a rapid
buffering approximation factor for calmodulin in the myoplasm.
 |
METHODS AND MODEL PARAMETERS |
The system of first-order nonlinear differential equations
at given initial conditions was solved using Gill's modification of
the Runge-Kutta fourth-order algorithm (Ralston and Wilf, 1960
). The
maximum step size for time integration was 0.1 ms and the maximum error
tolerance was 10
6.
Total ATP and ADP concentrations used in the model (see Table
1) are average values measured in
different cardiac tissues and species (Bers, 1991
; Leyssens et al.,
1996
; Baylor and Hollingworth, 1998
; Ch'en et al., 1998
). ATP and ADP
dissociation constants (see Table 2) were
taken from Martell and Smith (1982)
, and Kargacin and Kargacin (1997)
.
The on- and off-rate constants, k
and
k
, were obtained from Baylor and
Hollingworth (1998)
. We could not find published data for the values of
CaADP, MgATP, and MgADP on- and off-rate binding parameters. Therefore,
the typical near-diffusion-limited on-rate value of 125 µM
1 s
1 has been assumed (see Table 2)
(Soeller and Cannell, 1997
; Ch'en et al., 1998
). The corresponding
off-rate constants were obtained from the known values of equilibrium
dissociation constants (K
, K
, K
).
It is known that free Mg2+ in cardiac cells is between 0.5 and 2 mM (Bers, 1991
; Leyssens et al., 1996
; Carmeliet, 1999
; Murphy et
al., 1989
). Here we assume that, at equilibrium, free Mg2+
concentrations in the subspace and myoplasm do not differ, a value of 1 mM was used for both (see Table 3). Total
Mg2+ concentration (~7.44 mM) was estimated from the
accepted free Mg2+ concentration of 1 mM at ~100 nM free
Ca2+. We also assumed that total Mg2+
concentration in the cell remains constant, while free Mg2+
concentration varies with concentration of total ATP and ADP as
Ca2+ and Mg2+ buffers. The Mg2+
transfer-time constant from the subspace to the myoplasm (see Table
4) was chosen to be equal to the
Ca2+ transfer-time constant (
xfer) used by
Winslow et al. (1999)
. The transfer of free and bound ATP and ADP was
assumed to occur at half the rate of free Ca2+ and
Mg2+ diffusion (see Table 4) (Baylor and Hollingworth,
1998
). Unless specified otherwise in the figure legends or in the text,
the standard set of parameters and initial conditions used in the calculations is listed in the Tables. All other initial conditions and
values of the parameters that are not included in the Tables correspond
to those listed in the Appendix of Winslow et al. (1999)
.
In this paper, the effects of ATP and ADP buffering, transport, and
regulation in normal conditions and during metabolic inhibition were
examined in response to periodic voltage-clamp stimuli (
97 mV holding
potential, 3 mV step potential, 200 ms duration) at a frequency of 1 Hz.
 |
RESULTS |
Ion and buffer concentrations and ion currents in normal conditions
Ca2+, Na+, K+ concentrations
and ion currents with inclusion of Mg2+, ATP, and ADP
Here we report the results of several simulations, investigating
how including 1 mM Mg2+, 7 mM ATP, and 5 µM ADP may
contribute to the amplitude and time course of intracellular
Ca2+, Na+, and K+ transients and
ion currents.
In the first set of simulations, [Ca]ss and
[Ca]i (10th cycle, 9-10 s) were calculated
according to the approximation of Winslow et al. (1999)
, i.e., without
Mg2+, ATP, and ADP included. The solid lines in Fig.
2, A and B, show that [Ca]ss reached a peak of ~30 µM after ~4 ms,
whereas [Ca]i reached a peak of ~0.54 µM after ~48
ms. As shown in Fig. 2 C (solid line), JSR was
almost depleted during Ca2+ release. The change in
[Ca]JSR from a diastolic level of ~229 µM to ~83
µM was ~64%.

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|
FIGURE 2
Model outputs in response to 1-Hz periodic
voltage-clamp pulse of 97 mV holding potential, 3 mV step potential,
and 200 ms duration. Only responses to the 10th stimulus (9-10 s) are
shown. (A) Subspace Ca2+ transient.
(B) Myoplasmic Ca2+ transient. (C)
JSR Ca2+ transient. (D) L-type Ca2+
current. Mg2+, ATP, and ADP not included (solid line). ATP
and ADP treated as stationary buffers (dashed line). CaATP flux or all
fluxes included (dotted line). For simulations (dashed and dotted
lines) [ATP]tot = 7 mM, [ADP]tot = 5 µM, free Mg2+ = 1 mM. In all simulations shown,
[Mg]tot = 7.44 mM, [K]0 = 4 mM,
[Na]0 = 138 mM, [Ca]0 = 2 mM.
|
|
In the second set of simulations, ATP and ADP were treated as
stationary buffers to examine the effects of Ca2+ and
Mg2+ exchange with ATP and ADP. In the subspace,
[Ca]ss time course was not affected (dashed line in Fig.
2 A coincides with solid line) whereas, in the myoplasm,
Ca2+ concentration had a slightly reduced amplitude (Fig.
2 B, dashed line). In addition, these calculations
demonstrated that the changes in Ca2+ concentrations are
mainly due to Ca2+ and Mg2+ binding by ATP.
Neither [Ca]ss nor [Ca]i time courses (Fig.
2 A, solid or dashed lines; Fig. 2 B, dashed
line) were affected by changes in total ADP concentration from 0 µM
to 100 µM.
Including 1 mM Mg2+, 7 mM ATP, and 5 µM ADP in the model
did not affect JSR Ca2+ concentration levels or the L-type
Ca2+ current (Fig. 2, C and D, solid
and dashed lines coincide). [Na]i and
INa current were influenced to some extent, but
not notably (not shown). [K]i,
INaCa,
I*p(Ca), ICa,K,
ICa,b, IKr,
IKs, Ito1,
IK1, IKp,
I*NaK, and INa,b
remained unchanged after adding Mg2+, ATP, and ADP.
To study the significance of the mobility of Mg2+, ATP, and
ADP in determining Ca2+, Na+, and
K+ concentrations and ion currents, we performed another
set of calculations, including initially only
J
. The outputs of the model (10th
cycle, 9-10 s) in response to rhythmically applied clamp pulses are
shown in Fig. 2 (dotted lines). Figure 2 A shows that
[Ca]ss amplitude decreased and [Ca]ss
relaxation slightly accelerated when
J
was included. Additionally, the
simulations demonstrated that the changes in [Ca]ss
transient slightly affected the time course of
ICa (Fig. 2 D, dotted line). Figure
2 C (dotted line) shows that the diastolic JSR
Ca2+ level was elevated and that the JSR was less depleted
after the inclusion of J
. The model
results (Fig. 2 C, dotted line) also showed that the JSR is
again almost
depleted (~62%) by a single beat. Including J
elevated the stationary
[Ca]i peak (Fig. 2 B, compare dashed and
dotted lines). However, the simulation indicated that, under normal
conditions, ATP and ADP buffering and transport has a negligible effect
on the [Ca]i transient (Fig. 2 B, solid and
dotted lines almost coincide). Including
J
resulted in small changes in the
stationary [Na]i and INa time courses (10th cycle, 9-10 s) while [K]i,
INaCa,
I*p(Ca), ICa,K,
ICa,b, IKr,
IKs, Ito1,
IK1, IKp,
I*NaK, and INa,b
currents remained essentially unchanged (not shown). The calculations
also indicated that adding other fluxes
(J
, J
,
J
, J
)
had no observable influence on [Ca]ss,
[Ca]i, and [Ca]JSR (Fig.
2, A-C, dotted lines), or on [Na]i and
[K]i transients and ion currents.
Free and bound Mg2+, ATP, and ADP concentrations in the
presence and absence of fluxes
Kargacin and Kargacin (1997)
reported that, during excitation in
smooth muscle cells, the high Ca2+ signal near the membrane
might significantly influence free subspace ATP concentration in
contrast to the negligible changes in free myoplasmic ATP concentration
stimulated by the low myoplasmic Ca2+ signal. Our
simulations in ventricular myocytes showed that high subspace
Ca2+ concentrations indeed caused more sensitive changes in
the [ATP]ss than the low Ca2+ signal
stimulated in [ATP]i. However, these changes were not as
significant as they were in smooth muscle cells (in smooth muscle
cells, rest ATP was ~70 µM whereas, in ventricular myocytes, rest
ATP was ~560 µM). During excitation, free [ATP]ss and
[ATP]i (10th cycle, 9-10 s) decreased from the initial
level by ~30.5 µM and by ~0.477 µM, respectively, when ATP and
ADP were treated as stationary buffers (Fig.
3, A and B, dashed
lines). The inclusion of Mg2+, ATP, and ADP fluxes (Fig. 3,
A and B, dotted lines) decreased the diastolic
[ATP]ss level by ~6.24 µM and the diastolic
[ATP]i level by ~0.484 µM.

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FIGURE 3
(A) Effect of changes in subspace
Ca2+ concentration on free subspace ATP concentration and
(B) of changes in myoplasmic Ca2+ concentration
on free myoplasmic ATP concentration. ATP and ADP treated as stationary
buffers (dashed line). All fluxes included (dotted line). Only
responses to the 10th voltage-clamp stimulus ( 97 mV holding
potential, 3 mV step potential, 200 ms duration, frequency 1 Hz) are
shown. [ATP]tot = 7 mM, [ADP]tot = 5 µM, free Mg2+ = 1 mM.
|
|
Numerical studies also showed that, as free ATP concentration (10th
cycle, 9-10 s) falls during excitation, free Mg2+
concentration rises, but not notably. Systolic [Mg]ss
increased from the diastolic level of 1 mM by 49.3 and 1.1 µM and
systolic [Mg]i by 0.75 and 0.72 µM with ATP and ADP
stationary or mobile (not shown).
Most notably, the changes in [Ca2+]ss from
~0.1 to ~30 µM (10th cycle, 9-10 s) influenced
[CaATP]ss. [CaATP]ss increased from 0.22 µM up to ~80 µM in the absence, and up to ~8.25 µM in the presence of fluxes. The changes in [Ca2+]i
from ~0.1 to ~0.53 µM did not strongly influence
[CaATP]i. [CaATP]i increased from 0.22 µM
up to ~1.42 µM (ATP and ADP stationary) and up to ~1.466
µM (ATP and ADP mobile). In contrast to the notable changes in
[CaATP]ss, the changes in [MgATP]ss were
small and not as significant as in smooth muscle cells (Kargacin and
Kargacin, 1997
). Systolic [MgATP]ss decreased by ~49
µM from the initial level of 6.44 mM (ATP and ADP stationary) and by
~1.8 µM in the presence of fluxes. Model studies also suggested
that, under normal conditions (7 mM ATP, 5 µM ADP, and 1 mM free
Mg2+), changes in systolic [MgATP]i
concentration (10th cycle, 9-10 s) are negligible.
[MgATP]i dropped by ~0.75 µM from the initial level
of 6.44 mM when ATP and ADP were treated as either stationary or mobile.
Changes in the systolic [Ca]ss transient (Fig.
2 A) also stimulated a decrease of 0.036% (ATP and ADP
stationary) and a decrease of 0.0003% (mobile ATP and ADP) in
[ADP]ss, while [ADP]i remained almost
unchanged. Under normal conditions, the increase in systolic [CaADP]ss and [CaADP]i concentrations (10th
cycle, 9-10 s) from the initial diastolic level of ~0.1 nM was also
negligible. Surprisingly, the time courses of [MgADP]ss
and [MgADP]i demonstrated an interesting behavior in the
presence and absence of the fluxes. During excitation, [MgADP]ss and [MgADP]i rose when ATP and
ADP were treated as stationary buffers (Fig.
4, A and B, dashed
lines) in contrast to [MgATP]ss and
[MgATP]i, which decreased (not shown). Another
interesting result was that the fluxes were able to invert the
stationary [MgADP]ss time course (Fig. 4 A,
dotted line) but were not able to invert the stationary
[MgADP]i time course (Fig. 4 B, dotted line).

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FIGURE 4
Time courses of MgADP (9-10 s) in (A)
subspace and (B) myoplasm. ATP and ADP treated as stationary
buffers (dashed line). All fluxes included (dotted line). Simulations
are generated in response to 1-Hz voltage-clamp pulse ( 97 mV holding
potential, 3 mV step potential, 200 ms duration).
[ATP]tot = 7 mM, [ADP]tot = 5 µM, free Mg2+ = 1 mM.
|
|
Calculations also indicated that high Ca2+ concentrations
developed near the cell membrane (10th cycle, 9-10 s) increased the resting [CaATP]ss/[MgATP]ss ratio
~250-fold (stationary ATP and ADP) or ~36-fold (mobile ATP and
ADP). [CaATP]i/[MgATP]i ratio increased
~6.87-fold with ATP and ADP stationary or mobile. Changes in free
Ca2+ concentrations over the range of 0.1 to ~30 µM did
not affect the subspace or myoplasmic high-energy phosphate ratio
(MgADP/MgATP). In smooth muscle cells, Kargacin and Kargacin (1997)
also predicted significant changes in CaATP/MgATP concentration ratio
and no alterations in MgADP/MgATP ratio during cell excitation.
Ion and buffer concentrations, and ion currents during metabolic
inhibition
Experimental studies have demonstrated that block of oxidative
metabolism and a fall in [ATP]tot/[ADP]tot
ratio cause important changes in ion concentrations
([K+]0, [H+]i,
[Na+]i, [Ca2+]i,
[Mg2+]i) and have important effects on
channels and carriers (Murphy et al., 1989
; Marban et al., 1990
; Wagner
et al., 1990
; Isenberg et al., 1993
; Wilde and Aksnes, 1995
; Carmeliet,
1999
; Huser et al., 2000
). Ch'en et al. (1998)
reported that, while
creatine phosphate is present, total ATP and ADP concentrations remain constant, at ~7 and ~0 mM, respectively. Once ATP is depleted, ADP
starts to increase, and, after ~460 s, total ATP and ADP levels become approximately equal (~3 mM) during ischemia. Taking these results into consideration, we calculated ion and buffer concentrations and simulated ion currents when [ATP]tot and
[ADP]tot were 3 mM and mobile. Initial free
Mg2+ concentrations (t = 0 s) in the
subspace and myoplasm ([Mg]ss, [Mg]i) were
estimated to be ~2.248 mM, assuming that total intracellular Mg2+ concentration remains constant (7.44 mM) after the
fall in [ATP]tot/ [ADP]tot ratio from
1400 (normal conditions) to unity. During these simulations, the
initial free and bound metabolic ATP and ADP concentrations were
[ATP]ss = 112 µM, [CaATP]ss = 0.05 µM, [MgATP]ss = 2.888 mM,
[ATP]i = 112 µM, [CaATP]i = 0.047 µM, [MgATP]i = 2.888 mM,
[ADP]ss = 694 µM, [CaADP]ss = 0.045 µM, [MgADP]ss = 2.3 mM,
[ADP]i = 694 µM, [CaADP]i = 0.038 µM, and [MgADP]i = 2.3 mM. Under metabolic
conditions for the period of 10 s stimulation, the extracellular
concentrations of K+, Na+, and Ca2+
were kept constant at normal values ([K]0 = 4 mM,
[Na]0 = 138 mM, and [Ca]0 = 2 mM). All other initial conditions and values of the parameters used
were those listed in our Tables and in the Appendix of Winslow et al.
(1999)
.
Ca2+, Na+, K+ concentrations
and ion currents
The results demonstrated that a fall in
[ATP]tot/[ADP]tot ratio produced
significant changes in intracellular Ca2+ concentrations
and ion currents (ICa,
INaCa, I*NaK,
I*p(Ca)), calculated in response to a periodic
voltage-clamp stimuli with 200-ms duration and
97 mV and 3 mV holding
and step potentials.
Figure 5 C (top trace) shows
that, following the first stimulus, [Ca2+]JSR
load is greatly reduced when [ATP]tot and
[ADP]tot were each 3 mM. This significantly decreased the
[Ca]ss transient and increased ICa
during the subsequent stimulus (Fig. 5 A and Fig.
6 A, top traces). Figure
5, B and C (top traces), also show that
increased ICa was not able to increase the
[Ca]i transient or [Ca2+]JSR
loading. The [Ca]ss, [Ca]i, and
[Ca]JSR transients continued to decline. Figure
5 A (9-10 s, solid line) shows that normal [Ca]ss amplitude dropped ~50% and that the
pathological [Ca]ss transient reached the diastolic level
earlier than the normal [Ca]ss. Figure 5 B
(9-10 s, solid line) shows that the normal [Ca]i peak
also decreased ~50% and that a second higher slow peak appeared. In
contrast to accelerated [Ca]ss relaxation (Fig.
5 A, solid line), the pathological [Ca]i
transient decayed more slowly than normal. The model also predicted
that diastolic [Ca]i (~0.13 µM) and diastolic
[Ca]ss (~0.15 µM) levels reached during metabolic
inhibition were higher than those under normal conditions. Figure
5 C (9-10 s, solid line) shows that less Ca2+
was stored in the junctional SR after a fall in
[ATP]tot/[ADP]tot ratio. The pathological
[Ca2+]JSR level was more depleted and the
recovery of [Ca]JSR was more delayed than under normal
conditions. In response to 1-Hz voltage-clamp pulses after 10 s,
intracellular [Na]i increased by ~0.33 mM, whereas the
intracellular [K]i decreased slightly (~0.13 mM).

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FIGURE 5
Model outputs in response to 1-Hz periodic
voltage-clamp pulse of 97 mV holding potential, 3 mV step potential,
and 200 ms duration. (A) Subspace Ca2+ transient
(9-10 s). (B) Myoplasmic Ca2+ transient (9-10
s). (C) JSR Ca2+ transient (9-10 s). ATP and
ADP are treated as mobile Ca2+ and Mg2+
buffers. [ATP]tot = 7 mM,
[ADP]tot = 5 µM, free Mg2+ = 1 mM
(dotted line). [ATP]tot = 3 mM,
[ADP]tot = 3 mM, free Mg2+ = 2.248 mM (solid line). [ATP]tot = 0 mM,
[ADP]tot = 0 mM, free Mg2+ = 7.44 mM (dash-dot line). Top traces in (A), (B), and
(C) show [Ca]ss, [Ca]i, and
[Ca]JSR transients during metabolic inhibition
([ATP]tot = [ADP]tot = 3 mM, free
Mg2+ = 2.248 mM) for the period 0-11 s.
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FIGURE 6
Model simulations for a periodic voltage-clamp pulse of
97 mV holding potential, 3 mV step potential, 200 ms duration,
frequency 1 Hz. (A) L-type Ca2+ current.
(B) Na+-Ca2+ exchange current.
(C) Na+-K+ pump current.
(D) Sarcolemmal Ca2+ pump current. ATP and ADP
are treated as mobile Ca2+ and Mg2+ buffers.
[ATP]tot = 7 mM, [ADP]tot = 5 µM, free Mg2+ = 1 mM (dotted line).
[ATP]tot = 3 mM, [ADP]tot = 3 mM,
free Mg2+ = 2.248 mM (solid line).
[ATP]tot = 0 mM, [ADP]tot = 0 mM,
free Mg2+ = 7.44 mM (dash-dot line). Top traces in
(A), (B), (C), and (D) show
ICa, INaCa,
I*NaK, and
I*p(Ca) with metabolic inhibition
([ATP]tot = [ADP]tot = 3 mM, free
Mg2+ = 2.248 mM) for the period 0-11 s.
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The model also predicted that a fall in
[ATP]tot/[ADP]tot ratio has an important
modulatory effect on the ion currents and carriers. Figure
6 A (9-10 s, solid line) shows that the decreased [Ca]ss transient caused notable increase in L-type
Ca2+ current (ICa). Changes i