help button home button Biophys. J.
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS

This Article
Right arrow Abstract Freely available
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Michailova, A.
Right arrow Articles by McCulloch, A.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Michailova, A.
Right arrow Articles by McCulloch, A.

Biophys J, August 2001, p. 614-629, Vol. 81, No. 2

Model Study of ATP and ADP Buffering, Transport of Ca2+ and Mg2+, and Regulation of Ion Pumps in Ventricular Myocyte

Anushka Michailova*dagger and Andrew McCullochdagger

 *Department of Biophysics, Bulgarian Academy of Science, Sofia, Bulgaria, and  dagger Department of Bioengineering, University of California, San Diego, California 92093-0412 USA


    ABSTRACT
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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<UP><SUB>xfer</SUB><SUP>Mg</SUP></UP> = Mg2+ flux from subspace to myoplasm
J<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP> = CaATP flux from subspace to myoplasm
J<UP><SUB>xfer</SUB><SUP>MgATP</SUP></UP> = MgATP flux from subspace to myoplasm
J<UP><SUB>xfer</SUB><SUP>CaADP</SUP></UP> = CaADP flux from subspace to myoplasm
J<UP><SUB>xfer</SUB><SUP>MgADP</SUP></UP> = MgADP flux from subspace to myoplasm

Time constants


 tau xfer = time constant for transfer of Ca2+ from subspace to myoplasm
 tau <UP><SUB>xfer</SUB><SUP>Mg</SUP></UP> = time constant for transfer of Mg2+ from subspace to myoplasm
 tau <UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP> = time constant for transfer of CaATP from subspace to myoplasm
 tau <UP><SUB>xfer</SUB><SUP>MgATP</SUP></UP> = time constant for transfer of MgATP from subspace to myoplasm
 tau <UP><SUB>xfer</SUB><SUP>CaADP</SUP></UP> = time constant for transfer of CaADP from subspace to myoplasm
 tau <UP><SUB>xfer</SUB><SUP>MgADP</SUP></UP> = time constant for transfer of MgADP from subspace to myoplasm

Dissociation and rate constants


K<UP><SUB>D</SUB><SUP>CaATP</SUP></UP> = Ca2+-ATP dissociation constant
k<UP><SUB>+</SUB><SUP>CaATP</SUP></UP> = Ca2+ on-rate constant for ATP
k<UP><SUB>−</SUB><SUP>CaATP</SUP></UP> = Ca2+ off-rate constant for ATP
K<UP><SUB>D</SUB><SUP>MgATP</SUP></UP> = Mg2+-ATP dissociation constant
k<UP><SUB>+</SUB><SUP>MgATP</SUP></UP> = Mg2+ on-rate constant for ATP
k<UP><SUB>−</SUB><SUP>MgATP</SUP></UP> = Mg2+ off-rate constant for ATP
K<UP><SUB>D</SUB><SUP>CaADP</SUP></UP> = Ca2+-ADP dissociation constant
k<UP><SUB>+</SUB><SUP>CaADP</SUP></UP> = Ca2+ on-rate constant for ADP
k<UP><SUB>−</SUB><SUP>CaADP</SUP></UP> = Ca2+ off-rate constant for ADP
K<UP><SUB>D</SUB><SUP>MgADP</SUP></UP> = Mg2+-ADP dissociation constant
k<UP><SUB>+</SUB><SUP>MgADP</SUP></UP> = Mg2+ on-rate constant for ADP
k<UP><SUB>−</SUB><SUP>MgADP</SUP></UP> = Mg2+ off-rate constant for ADP


    INTRODUCTION
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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.



View larger version (48K):
[in this window]
[in a new window]
 
FIGURE 1   Schematic diagram of the mechanisms involved in the model.

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.,
[<UP>ATP</UP>]<SUB><UP>tot</UP></SUB>=[<UP>ATP</UP>]<SUB><UP>tot−i</UP></SUB>=[<UP>ATP</UP>]<SUB><UP>tot−ss</UP></SUB>, (1)

[<UP>ADP</UP>]<SUB><UP>tot</UP></SUB>=[<UP>ADP</UP>]<SUB><UP>tot−i</UP></SUB>=[<UP>ADP</UP>]<SUB><UP>tot−ss</UP></SUB> (2)
The buffering of Ca2+ and Mg2+ by ATP in the subspace is given by the following equations:
[<UP>ATP</UP>]<SUB><UP>ss</UP></SUB>=[<UP>ATP</UP>]<SUB><UP>tot</UP></SUB>−[<UP>CaATP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>MgATP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (3)

<FR><NU><UP>d</UP>[<UP>CaATP</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=<UP>−</UP>J<SUP><UP>CaATP</UP></SUP><SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>+k<SUP><UP>CaATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>ss</UP></SUB>[<UP>ATP</UP>]<SUB><UP>ss</UP></SUB>

−k<SUP><UP>CaATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaATP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (4)

<FR><NU><UP>d</UP>[<UP>MgATP</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=<UP>−</UP>J<SUP><UP>MgATP</UP></SUP><SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>+k<SUP><UP>MgATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB>[<UP>ATP</UP>]<SUB><UP>ss</UP></SUB>

−k<SUP><UP>MgATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgATP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (5)
where k+ and k- are the corresponding on-rate and off-rate binding constants. The equations for the bulk myoplasm are similar:
[<UP>ATP</UP>]<SUB><UP>i</UP></SUB>=[<UP>ATP</UP>]<SUB><UP>tot</UP></SUB>−[<UP>CaATP</UP>]<SUB><UP>i</UP></SUB>−[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB><UP>,</UP> (6)

<FR><NU><UP>d</UP>[<UP>CaATP</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=J<SUP><UP>CaATP</UP></SUP><SUB><UP>xfer</UP></SUB>+k<SUP><UP>CaATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>i</UP></SUB>[<UP>ATP</UP>]<SUB><UP>i</UP></SUB>

−k<SUP><UP>CaATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaATP</UP>]<SUB><UP>i</UP></SUB><UP>,</UP> (7)

<FR><NU><UP>d</UP>[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=J<SUP><UP>MgATP</UP></SUP><SUB><UP>xfer</UP></SUB>+k<SUP><UP>MgATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>i</UP></SUB>[<UP>ATP</UP>]<SUB><UP>i</UP></SUB>

−k<SUP><UP>MgATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB><UP>,</UP> (8)
CaATP and MgATP fluxes (Fig. 1) are given by
J<SUP><UP>CaATP</UP></SUP><SUB><UP>xfer</UP></SUB>=<FR><NU>[<UP>CaATP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>CaATP</UP>]<SUB><UP>i</UP></SUB></NU><DE>&tgr;<SUP><UP>CaATP</UP></SUP><SUB><UP>xfer</UP></SUB></DE></FR>, (9)

J<SUP><UP>MgATP</UP></SUP><SUB><UP>xfer</UP></SUB>=<FR><NU>[<UP>MgATP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB></NU><DE>&tgr;<SUP><UP>MgATP</UP></SUP><SUB><UP>xfer</UP></SUB></DE></FR>. (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
[<UP>ADP</UP>]<SUB><UP>ss</UP></SUB>=[<UP>ADP</UP>]<SUB><UP>tot</UP></SUB>−[<UP>CaADP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>MgADP</UP>]<SUB><UP>ss</UP></SUB>, (11)

<FR><NU><UP>d</UP>[<UP>CaADP</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=<UP>−</UP>J<SUP><UP>CaADP</UP></SUP><SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>+k<SUP><UP>CaADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>ss</UP></SUB>[<UP>ADP</UP>]<SUB><UP>ss</UP></SUB>

−k<SUP><UP>CaADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaADP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (12)

<FR><NU><UP>d</UP>[<UP>MgADP</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=<UP>−</UP>J<SUP><UP>MgADP</UP></SUP><SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>+k<SUP><UP>MgADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB>[<UP>ADP</UP>]<SUB><UP>ss</UP></SUB>

−k<SUP><UP>MgADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgADP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (13)

[<UP>ADP</UP>]<SUB><UP>i</UP></SUB>=[<UP>ADP</UP>]<SUB><UP>tot</UP></SUB>−[<UP>CaADP</UP>]<SUB><UP>i</UP></SUB>−[<UP>MgADP</UP>]<SUB><UP>i</UP></SUB><UP>,</UP> (14)

<FR><NU><UP>d</UP>[<UP>CaADP</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=J<SUP><UP>CaADP</UP></SUP><SUB><UP>xfer</UP></SUB>+k<SUP><UP>CaADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>i</UP></SUB>[<UP>ADP</UP>]<SUB><UP>i</UP></SUB>

−k<SUP><UP>CaADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaADP</UP>]<SUB><UP>i</UP></SUB><UP>,</UP> (15)

<FR><NU><UP>d</UP>[<UP>MgADP</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=J<SUP><UP>MgADP</UP></SUP><SUB><UP>xfer</UP></SUB>+k<SUP><UP>MgADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>i</UP></SUB>[<UP>ADP</UP>]<SUB><UP>i</UP></SUB>

−k<SUP><UP>MgADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgADP</UP>]<SUB><UP>i</UP></SUB>. (16)
CaADP and MgADP fluxes (Fig. 1) are given by
J<SUP><UP>CaADP</UP></SUP><SUB><UP>xfer</UP></SUB>=<FR><NU>[<UP>CaADP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>CaADP</UP>]<SUB><UP>i</UP></SUB></NU><DE>&tgr;<SUP><UP>CaADP</UP></SUP><SUB><UP>xfer</UP></SUB></DE></FR>, (17)

J<SUP><UP>MgADP</UP></SUP><SUB><UP>xfer</UP></SUB>=<FR><NU>[<UP>MgADP</UP>]<SUB><UP>ss</UP></SUB>−[<UP>MgADP</UP>]<SUB><UP>i</UP></SUB></NU><DE>&tgr;<SUP><UP>MgADP</UP></SUP><SUB><UP>xfer</UP></SUB></DE></FR>. (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
<FR><NU><UP>d</UP>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=<UP>−</UP>J<SUP><UP>Mg</UP></SUP><SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>−k<SUP><UP>MgATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB>[<UP>ATP</UP>]<SUB><UP>ss</UP></SUB>

+k<SUP><UP>MgATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgATP</UP>]<SUB><UP>ss</UP></SUB>

−k<SUP><UP>MgADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB>[<UP>ADP</UP>]<SUB><UP>ss</UP></SUB>

+k<SUP><UP>MgADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgADP</UP>]<SUB><UP>ss</UP></SUB><UP>,</UP> (19)
and in the bulk myoplasm by
<FR><NU><UP>d</UP>[<UP>Mg</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=J<SUP><UP>Mg</UP></SUP><SUB><UP>xfer</UP></SUB>−k<SUP><UP>MgATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>i</UP></SUB>[<UP>ATP</UP>]<SUB><UP>i</UP></SUB>+k<SUP><UP>MgATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB>

−k<SUP><UP>MgADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Mg</UP>]<SUB><UP>i</UP></SUB>[<UP>ADP</UP>]<SUB><UP>i</UP></SUB>+k<SUP><UP>MgADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>MgADP</UP>]<SUB><UP>i</UP></SUB>. (20)
The transfer flux of Mg2+ from subspace to myoplasm (Fig. 1) is given by
J<SUP><UP>Mg</UP></SUP><SUB><UP>xfer</UP></SUB>=<FR><NU>[<UP>Mg</UP>]<SUB><UP>ss</UP></SUB>−[<UP>Mg</UP>]<SUB><UP>i</UP></SUB></NU><DE>&tgr;<SUP><UP>Mg</UP></SUP><SUB><UP>xfer</UP></SUB></DE></FR>. (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):
I<SUP>*</SUP><SUB><UP>NaK</UP></SUB>(t)=S<SUB><UP>MgATP</UP></SUB>I<SUB><UP>NaK</UP></SUB>(t), (22)

I<SUP>*</SUP><SUB><UP>p</UP>(<UP>Ca</UP>)</SUB>(t)=S<SUB><UP>MgATP</UP></SUB>I<SUB><UP>p</UP>(<UP>Ca</UP>)</SUB>(t), (23)

J<SUP>*</SUP><SUB><UP>up</UP></SUB>(t)=S<SUB><UP>MgATP</UP></SUB>J<SUB><UP>up</UP></SUB>(t), (24)
where
S<SUB><UP>MgATP</UP></SUB>=<FR><NU>[<UP>MgATP</UP>]<SUB><UP>i</UP></SUB></NU><DE>[<UP>MgATP</UP>]<SUB><UP>i0</UP></SUB></DE></FR>, (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:
<FR><NU><UP>d</UP>[<UP>Ca</UP>]<SUB><UP>ss</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=&bgr;<SUB><UP>ss</UP></SUB><FENCE>J<SUB><UP>rel</UP></SUB><FR><NU>V<SUB><UP>JSR</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>−J<SUB><UP>xfer</UP></SUB><FR><NU>V<SUB><UP>myo</UP></SUB></NU><DE>V<SUB><UP>ss</UP></SUB></DE></FR>−(I<SUB><UP>Ca</UP></SUB>) <FR><NU>A<SUB><UP>cap</UP></SUB>C<SUB><UP>sc</UP></SUB></NU><DE>2V<SUB><UP>ss</UP></SUB>F</DE></FR>−k<SUP><UP>CaATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>ss</UP></SUB>[<UP>ATP</UP>]<SUB><UP>ss</UP></SUB>+k<SUP><UP>CaATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaATP</UP>]<SUB><UP>ss</UP></SUB><UP>−k</UP><SUP><UP>CaADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>ss</UP></SUB>[<UP>ADP</UP>]<SUB><UP>ss</UP></SUB>+k<SUP><UP>CaADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaADP</UP>]<SUB><UP>ss</UP></SUB></FENCE>, (26)

<FR><NU><UP>d</UP>[<UP>Ca</UP>]<SUB><UP>i</UP></SUB></NU><DE><UP>d</UP>t</DE></FR>=&bgr;<SUB><UP>i</UP></SUB><FENCE>J<SUB><UP>xfer</UP></SUB>−J<SUP>*</SUP><SUB><UP>up</UP></SUB>−J<SUB><UP>trpn</UP></SUB>−(I<SUB><UP>Ca,b</UP></SUB>−2I<SUB><UP>NaCa</UP></SUB>+I<SUP>*</SUP><SUB><UP>p</UP>(<UP>Ca</UP>)</SUB>)</FENCE> (27)

×<FR><NU>A<SUB><UP>cap</UP></SUB>C<SUB><UP>sc</UP></SUB></NU><DE>2V<SUB><UP>myo</UP></SUB>F</DE></FR>−k<SUP><UP>CaATP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>i</UP></SUB>[<UP>ATP</UP>]<SUB><UP>i</UP></SUB>+k<SUP><UP>CaATP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaATP</UP>]<SUB><UP>i</UP></SUB>

<FENCE><UP>−</UP> k<SUP><UP>CaADP</UP></SUP><SUB><UP>+</UP></SUB>[<UP>Ca</UP>]<SUB><UP>i</UP></SUB>[<UP>ADP</UP>]<SUB><UP>i</UP></SUB>+k<SUP><UP>CaADP</UP></SUP><SUB><UP>−</UP></SUB>[<UP>CaADP</UP>]<SUB><UP>i</UP></SUB></FENCE>,
where beta ss is a rapid buffering approximation factor for calmodulin in the subspace, and beta i is a rapid buffering approximation factor for calmodulin in the myoplasm.


    METHODS AND MODEL PARAMETERS
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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<UP><SUB>+</SUB><SUP>CaATP</SUP></UP> and k<UP><SUB>−</SUB><SUP>CaATP</SUP></UP>, 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<UP><SUB>D</SUB><SUP>CaADP</SUP></UP>, K<UP><SUB>D</SUB><SUP>MgATP</SUP></UP>, K<UP><SUB>D</SUB><SUP>MgADP</SUP></UP>).


                              
View this table:
[in this window]
[in a new window]
 
TABLE 1   Standard buffer and ionic concentrations


                              
View this table:
[in this window]
[in a new window]
 
TABLE 2   Rate and dissociation ATP and ADP constants

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 (tau 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).


                              
View this table:
[in this window]
[in a new window]
 
TABLE 3   Initial conditions


                              
View this table:
[in this window]
[in a new window]
 
TABLE 4   Time constants

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
TOP
ABSTRACT
GLOSSARY
INTRODUCTION
MATHEMATICAL MODEL
METHODS AND MODEL PARAMETERS
RESULTS
DISCUSSION
REFERENCES

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%.



View larger version (19K):
[in this window]
[in a new window]
 
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. 2C 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<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP>. 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<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP> 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<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP>. The model results (Fig. 2 C, dotted line) also showed that the JSR is again almost <FR><NU>2</NU><DE>3</DE></FR> depleted (~62%) by a single beat. Including J<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP> 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<UP><SUB>xfer</SUB><SUP>CaATP</SUP></UP> 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<UP><SUB>xfer</SUB><SUP>Mg</SUP></UP>, J<UP><SUB>xfer</SUB><SUP>CaADP</SUP></UP>, J<UP><SUB>xfer</SUB><SUP>MgATP</SUP></UP>, J<UP><SUB>xfer</SUB><SUP>MgADP</SUP></UP>) had no observable influence on [Ca]ss, [Ca]i, and [Ca]JSR (Fig. 2A-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.



View larger version (10K):
[in this window]
[in a new window]
 
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).



View larger version (10K):
[in this window]
[in a new window]
 
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 5B 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).



View larger version (13K):
[in this window]
[in a new window]
 
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.



View larger version (26K):
[in this window]
[in a new window]
 
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.

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