Transmembrane potential changes caused by shocks in guinea pig papillary muscle. Zhou, Xiaohong, William M Smith, Dennis L. Rollins, Raymond E Ideker. Departments of Medicine and Pathology, Duke University Medical Center, Durham, North Carolina, 27710, the Engineering Research Center in Emerging Cardiovascular Technologies, School of Engineering, Duke University, Durham, North Carolina, 27706 and the Division of Cardiovascular Disease, Department of Medicine, University of Alabama at Birmingham, Birmingham, Alabama 35294
APStracts 3:0198H, 1996.
To study the transmembrane potential changes (_V[mu]) caused by extracellular field stimulation, V[mu] was recorded in 10 guinea pig papillary muscles by a double-barrel microelectrode which could eliminate the shock artifact during the V[mu] recording. Following 20 S1 stimuli at twice diastolic threshold, a 10 msec S2 shock field was delivered through shock electrodes 2 cm on either side of the tissue during the action potential plateau with a 30 msec S1-S2 interval or during diastole. Six shock strengths were given which created field strengths of 1.8+/-0.4, 3.8+/-0.7, 5.6+/-0.9, 7.2+/-1.1, 11.1+/-1.9 and 17.8+/-1.5 V/cm at the papillary muscle. Shocks of both polarities were given. The tissue was then treated with either 30 [mu]M TTX (n=5) or 30 [mu]M TTX plus Ca++-free (n=5) perfusion. The above six shock strengths with both polarities were given again during diastole. Results: For shocks during the action potential plateau, the net magnitudes of the _V[mu] caused by the above six potential gradients were 22.4+/-9.6, 43.6+/-17.4, 54.7+/-17.9, 60.4+/-18.1, 65.4+/-13.7 and 66.4+/-12.2 mV (p&LT.01 among changes caused by six shock strengths) for shocks causing depolarization and 41.1+/-16.5, 68.3+/-22, 80.5+/-20.4, 84.0+/-19.5, 93.6+/-16.3 and 98.9+/-15.4 mV (p&LT.01 among changes caused by six shock strengths) for shocks causing hyperpolarization. Though _V[mu] increased as the shock potential gradient increased, the relationship was not linear. For shocks during diastole, hyperpolarizing shocks induced triphasic changes in V[mu] during the shock, i.e., initial hyperpolarization, then depolarization, followed again by hyperpolarization. A new depolarization upstroke occurred immediately after the end of the shock. After TTX or TTX plus Ca++-free perfusion, neither twice nor 10 times diastolic threshold S1 could induce an action potential, but a shock field of 1.8+/-0.2 V/cm still induced action potentials. The peak value of depolarization measured with respect to the resting potential (-87+/-5 mV) during the hyperpolarizing shock decreased from +14+/-22 mV before TTX perfusion to -66+/-30 mV with TTX perfusion (p&LT0.01). The fast upstroke rate of depolarization both during and immediately after the end of hyperpolarizing shocks was inhibited by TTX perfusion. Conclusion: (1) the relationship between the _V[mu] and the shock potential gradient is not linear; (2) field but not point stimulation can induce an action potential when sodium channels are inactivated; and (3) during diastole sodium channels responsible for fast depolarization are activated twice by a 10 msec hyperpolarizing shock, once during shock-induced hyperpolarization and again immediately after the end of the shock.

Received 6 October 1995; accepted in final form 24 April 1996.
APS Manuscript Number H943-5.
Article publication pending Am. J. Physiol. (Heart Circ. Physiology).
ISSN 1080-4757 Copyright 1996 The American Physiological Society.
Published in APStracts on 8 May 96