Nonuniform Epicardial Activation and Repolarization Properties of in Vivo Canine Pulmonary Conus

The relation between nonuniform epicardial activation and ventricular repolarization properties was studied in 14 pentobarbital anesthetized dogs and with a computer model. In 11 dogs, isochrone maps of epicardial activation sequence were constructed from electrograms recorded from the pulmcnary conus with 64 electrodes on an 8 × 8 grid with 2-mm electrode separation. The heart was paced from multiple sites on the periphery of the array. Uniformity of epicardial activation was estimated from activation times at test sites and their eight neighboring sites. Acceleration shortened and deceleration prolonged refractory periods. The locations of acceleration and deceleration sites of activation differed during drives from various sites, and differences in uniformity of activation during pairs of drives were correlated to differences fa refractory periods (r =0.76, range 0.59–0.93). In three additional experiments, transmural activation sequence maps were constructed from electrograms recorded from needle-mounted electrodes placed upstream and downstream to epicardial activation delays. Activation proceeded from epicardium to endocardium upstream to the delays and from endocardium to epicardium downstream to the delays. A computer simulation of two-dimensional action potential propagation based on the Beeler-Reuter myocardial membrane model provided insights to the mechanism for the results of the animal experiments. The two-dimensional sheet modeled the transmural anisotropic histology of the canine pulmonary conus and corresponded to previous reports and histology of specimens from five experiments. Simulated activation patterns were similar to those found in the experimental animals. In addition, action potentials were electronically prolonged at sites of deceleration and shortened at sites of acceleration, results comparable to the animal experiments. Our findings demonstrate that the location of areas of nonuniform epicardial activation is dependent on drive site and that nonuniform activation electronically modulates repolarization properties. Therefore it seems likely that the site of origin of ectopic ventricular complexes, especially in ischemic myocardium where activation is nonuniform, could be an important determinant of whether ectopic activity initiates sustained tachyarrhythmias.

[1]  M. Spach,et al.  Relating Extracellular Potentials and Their Derivatives to Anisotropic Propagation at a Microscopic Level in Human Cardiac Muscle: Evidence for Electrical Uncoupling of Side‐to‐Side Fiber Connections with Increasing Age , 1986, Circulation research.

[2]  A. Wilde,et al.  Changes in conduction velocity during acute ischemia in ventricular myocardium of the isolated porcine heart. , 1986, Circulation.

[3]  R. W. Joyner,et al.  Effects of the Discrete Pattern of Electrical Coupling on Propagation through an Electrical Syncytium , 1982, Circulation research.

[4]  J. .. Abildskov,et al.  Effects of Activation Sequence on the Local Recovery of Ventricular Excitability in the Dog , 1976, Circulation research.

[5]  J. Spear,et al.  The effects of procainamide on conduction in anisotropic canine ventricular myocardium. , 1986, Circulation.

[6]  R. W. Joyner,et al.  Propagation through electrically coupled cells. Effects of a resistive barrier. , 1984, Biophysical journal.

[7]  M. Burgess,et al.  Effects of activation sequence on ventricular refractory periods of ischemic canine myocardium. , 1985, Journal of electrocardiology.

[8]  L. Clerc Directional differences of impulse spread in trabecular muscle from mammalian heart. , 1976, The Journal of physiology.

[9]  M H DRAPER,et al.  A comparison of the conduction velocity in cardiac tissues of various mammals. , 1959, Quarterly journal of experimental physiology and cognate medical sciences.

[10]  M. Burgess,et al.  Electrotonic Interaction during Canine Ventricular Repolarization , 1978, Circulation research.

[11]  R C Barr,et al.  Collision of Excitation Waves in the Dog Purkinje System: EXTRACELLULAR IDENTIFICATION , 1971, Circulation research.

[12]  R C Barr,et al.  Extracellular Potentials Related to Intracellular Action Potentials during Impulse Conduction in Anisotropic Canine Cardiac Muscle , 1979, Circulation research.

[13]  M S Spach,et al.  The Functional Role of Structural Complexities in the Propagation of Depolarization in the Atrium of the Dog: Cardiac Conduction Disturbances Due to Discontinuities of Effective Axial Resistivity , 1982, Circulation research.

[14]  J. Kootsey,et al.  The origin of the T-wave. , 1980, Critical reviews in bioengineering.

[15]  W Rall,et al.  Changes of action potential shape and velocity for changing core conductor geometry. , 1974, Biophysical journal.

[16]  I. Tasaki Collision of two nerve impulses in the nerve fibre , 1949 .

[17]  W. C. Randall,et al.  Structural basis for cardiac function. , 1970, The American journal of physiology.

[18]  B. M. Steinhaus,et al.  SIMULATION OF ACTIVATION SEQUENCE EFFECTS IN HEART TISSUE. , 1983 .

[19]  R. W. Joyner,et al.  Propagation through electrically coupled cells: two inhomogeneously coupled cardiac tissue layers. , 1984, The American journal of physiology.

[20]  A. M. Scher,et al.  Influence of Cardiac Fiber Orientation on Wavefront Voltage, Conduction Velocity, and Tissue Resistivity in the Dog , 1979, Circulation research.

[21]  D. Geselowitz,et al.  The Discontinuous Nature of Propagation in Normal Canine Cardiac Muscle: Evidence for Recurrent Discontinuities of Intracellular Resistance that Affect the Membrane Currents , 1981, Circulation research.

[22]  G. W. Beeler,et al.  Reconstruction of the action potential of ventricular myocardial fibres , 1977, The Journal of physiology.

[23]  J. Kingma,et al.  EFFECTS OF THE RENIN-ANGIOTENSIN SYSTEM ON SUSTAINED VENTRICULAR-TACHYCARDIA AFTER MYOCARDIAL-INFARCTION , 1986 .

[24]  C. Nicholson Electric current flow in excitable cells J. J. B. Jack, D. Noble &R. W. Tsien Clarendon Press, Oxford (1975). 502 pp., £18.00 , 1976, Neuroscience.

[25]  H. H. Rachford,et al.  The Numerical Solution of Parabolic and Elliptic Differential Equations , 1955 .

[26]  F A Roberge,et al.  Reconstruction of Propagated Electrical Activity with a Two‐Dimensional Model of Anisotropic Heart Muscle , 1986, Circulation research.

[27]  Bruce M. Steinhaus,et al.  Action Potential Collision in Heart Tissue-Computer Simulations and Tissue Expenrments , 1985, IEEE Transactions on Biomedical Engineering.

[28]  Ronald W. Joyner,et al.  Simulation of Action Potential Propagation in an Inhomogeneous Sheet of Coupled Excitable Cells , 1975, Circulation research.

[29]  J. Toyama,et al.  Anisotropic conduction properties of canine ventricular muscles. Influence of high extracellular K+ concentration and stimulation frequency. , 1985, Japanese circulation journal.