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Published online 17 March 2003 doi:10.1085/jgp.200308787
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© Rockefeller University Press, 0022-1295/2003/4/311/ $5.00
Journal of General Physiology, Volume 121, Number 4, April 2003 311-324

Simulation of Calcium Sparks in Cut Skeletal Muscle Fibers of the Frog

W.K. Chandler1, S. Hollingworth2 and S.M. Baylor2

1 Department of Cellular and Molecular Physiology, Yale University School of Medicine, New Haven, CT 06520
2 Department of Physiology, University of Pennsylvania School of Medicine, Philadelphia, PA 19104

Address correspondence to S.M. Baylor, Department of Physiology, University of Pennsylvania School of Medicine, Philadelphia, PA 19104-6085. Fax: (215) 573-5851; E-mail: baylor{at}mail.med.upenn.edu

Spark mass, the volume integral of {Delta}F/F, was investigated theoretically and with simulations. These studies show that the amount of Ca2+ bound to fluo-3 is proportional to mass times the total concentration of fluo-3 ([fluo-3T]); the proportionality constant depends on resting Ca2+ concentration ([Ca2+]R). In the simulation of a Ca2+ spark in an intact frog fiber with [fluo-3T] = 100 µM, fluo-3 captures approximately one-fourth of the Ca2+ released from the sarcoplasmic reticulum (SR). Since mass in cut fibers is several times that in intact fibers, both with similar values of [fluo-3T] and [Ca2+]R, it seems likely that SR Ca2+ release is larger in cut fiber sparks or that fluo-3 is able to capture a larger fraction of the released Ca2+ in cut fibers, perhaps because of reduced intrinsic Ca2+ buffering. Computer simulations were used to identify these and other factors that may underlie the differences in mass and other properties of sparks in intact and cut fibers. Our spark model, which successfully simulates calcium sparks in intact fibers, was modified to reflect the conditions of cut fiber measurements. The results show that, if the protein Ca2+-buffering power of myoplasm is the same as that in intact fibers, the Ca2+ source flux underlying a spark in cut fibers is 5–10 times that in intact fibers. Smaller source fluxes are required for less buffer. In the extreme case in which Ca2+ binding to troponin is zero, the source flux needs to be 3–5 times that in intact fibers. An increased Ca2+ source flux could arise from an increase in Ca2+ flux through one ryanodine receptor (RYR) or an increase in the number of active RYRs per spark, or both. These results indicate that the gating of RYRs, or their apparent single channel Ca2+ flux, is different in frog cut fibers—and, perhaps, in other disrupted preparations—than in intact fibers.

Key Words: spark mass • ryanodine receptors • excitation-contraction coupling • frog muscle


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