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February 1998, Melboume AUSTRALIA 2nd lntemational Conference on Bioelectromagnetism Computer Simulation of Bundle Branch Re-entry in a 3D Cellular Automata Model of the Heart Paul H. Fleisch”, and Paul Wach Department of Biophysics, Institute of Biomedical Engineering, Technical University Graz, Inffeldgasse 18, A-8010 Graz, Austria Abstract: A 3D cellular automata model of the entire The Purkinje fibre network was represented by a sheet heart was used for modelling the spread of excitation of conducting tissue on the endocardial surface of the and repolarization in the heart. By modelling ventricle. Anisotropic conduction of the ventricular ventricular pacing and premature stimuli the myocardium was modelled by different conduction inducibility of bundle branch re-entry was investigated velocities in direction of fibres and perpendicular to it. Under normal conditions bundle branch re-entry of His bundle type A and B were induced. A reduction of conduction velocity in the bundle branches resulted in multiple reentrant echo beats as well as a wider zone of re-entrant lefi posterior activation. . INTRODUCTION Akhtar et id. [l] was the first to report electrophysiologic findings in human studies that supported the hypothesis of macro re-entry via the His-Purkinje system. More complex pattern resulting in fascicular ree n q have recently been reported and show the importance of the stimulus site: [2]. In diseased hearts, sustained bundle branch reentrant tachycardia can occur when there is sufficient delay in His-Purkinje conduction such that the reentrant impulse can continue to propagate around the bundle branches. Serious hemodynamic consequences, such as sudden cardiac death or syncope, are frequently the initial clinical replesentation of this arrhyhma . In the last deciide the increase of computational power supported the devdopment of several 3D cellular automata models [3-61 for calculating the spread of excitation and the body surface electrocardiogram of the human heart. The purpose of this study was to simulate the spread of excitation in a 3D computer model of the entire heart and to test the inducibility of bundle branch re-entry. METHOD The described 3D cellular automaton model is an extended version of the previously published computer model [5-61. In brief the heart anatomy was discretized in a Cartesian co-ordinate system by a 2.5 10-3mgrid including 11 different carckiac tissues for the normal and 4 for pathologic conditions. To each element of heart anatomy an effective refractory period (ERP) value was assigned. A conduction velocity was assigned for propagation inside as well as between different cardiac tissues. In addition the conduction velocity was assumed to increase linearly after end of the ERP till the end of the relative refractory period. The earliest regions to excite the ventricle were the conjunction elements at the terminations of the bundle branches where the excitation propagated to the Purkinje fibre network and ventricular myocardium. The left bundle is separated into three branches which excited the high anterior paraseptal region, the midseptum and the posterior paraseptal apical n:gion of the ventricle 0.153s, 0.155s and 0.165s after start of sinus node activation. In the right ventricle a single lbundle excited the lower right apex and the right ventricular free wall 0.004s and 0.01s after left high anterior paraseptal activation. These locations were all close to the sites mentioned in literature [7] as being activated first. 155 /’. left midseptal branch left anterior paraseptal branch Figure 1: Schematic representation of the modeled bundle branches. The ERP dynamic depending on pacing cycle length was taken into consideration by assuming ERP dependence on the preceding time interval in the atrium whereas in the ventricle the formula pubished by Gulrajani [SI was used for all ventricular tissues by taking values from literature [9-lo]. Figure 4 shows the ERP values of ventricular myocardium and Purkinje fibre after a step increase of pacing frequency. Similar measurements were first reported by M.J. Janse in mongrel dogs [113. 10 100 1000 340 1 I340 320 320 300 I300 EFIBRE 280 8 k 260 240 220 200 180 1 ventricular myocardium 160 - 180 I 160 Figure 2: ERP dynamic of ventricular myocardium and Purkinje fibre after a shortening of the basic cycle length from 0.7s to 0.4s. The algorithm for calculating the excitation process is based on a modified version of Huygen’s principle for constructing wavefronts. Each element of the heart ~ February 1998, Melboume AUSTRALIA 2nd International Conference on Bioelectromagnetism left ventricular stimulation at least in the normal human heart. This reversed re-entrant circuit was labelled type C and involved retrograde propagation via the right bundle branch and antegrade activation via the left bundle branch. In our model type A and B were found. A possible application of the model is to use it for patient oriented simulation. By this way the computer model can be used as an additional decision tool for pharmacological antimhykuc therapy or ablation procedure. Fuaher the model can be used for calculating the magneto- and electrocar&ogram based on a known pathologic substrate. geometry can be in either of three states “excitable“, “excited or “waiting“ during the computer simulation process [SI. Ventricular pacing at a basic cycle length of 0.7s in combination with premature stimuli at different coupling intervals and different anatomical locations was modelled for testing the inducibility of bundle branch re-entry. According to reference [2] the EW of the right bundle branch was assumed to be longer compared to the left bundle. Results In case of left and right apical ventricular premature stimuli (S2) the preferred retrograde route of impulse propagation was through the left bundle branches. In addition the increment of S2H2 conduction time between premature stimulus (Sa) and E s bundle (€I2) tended to have a linear pattern in relationship to decreasing SIS2 coupling intervals similar to the results described in literature [2]. In a next step ventricular stimuli were applied near the terminations of the bundle branches for inducing re-entrant activation. Single premature stimuli near the right ventricular &ee wall resulted in single ventricular echo beats. The premature beats were retrograde blocked at the right bundle branch but sufficiently delayed to excite the left sided His-Purkinje system in retrograde and the right bundle branch in anterograde direction resultant in V3. These excitation front was then finally blocked in the HisF’urkinje system. In the left ventricle the high anterior paraseptal region was selected for inducing re-entrant activation. This time the premature stimulation resulted in fascicular re-entry. The excitation travelled in retrograde direction along the posterior bundle and excited the ventricle (V3)through the anterior bundle. Then the excitation was finally blocked in the His-Purkinje system. A reduction of conduction velocity (as found under pathologic conditions) in the bundle branches resulted in multiple re-entrant echo beats as well as in a wider S1S2 time interval of re-entrant activation. In addition the anatomical region where re-entrant activation occurred increased. DISCUSSION Several limitations and simplifications of the electrophysiologic process must be kept in mind. The excitation process was modelled on a macroscopic level and omitted electrotonic interactions between cardiac fibres. A coarse 2.5.10-3m grid was used for simulating the excitation process in the entire heart. These simplifications seemed to be justified due to the scope of modelling macro re-entrant activation. In addition the difference between antegrade and retrograde conduction velocity and effective refractory period was not taken into consideration. According to reference [2] the re-entrant circuit of HisPurkinje system re-entry can be classified into three types. Type A is the typical re-entry phenomenon seen with right ventricular stimulation where retrograde conduction is via the left bundle branch and anterograde conduction is via the right bundle branch. Type B is typical seen with left ventricular stimulation. Type B is a fascicular re-entry where retrograde conduction occurs via a left sided fascicle and anterograde conduction is via the other fascicle. The reversal of re-entrant circuit of type A was rarely seen with REFEBENCES [l] M. Akhtar, A.N. Damato, W.P. Batsford, J.B. Ogunkelu, J.N. Ruskin, “Demonstration of re-entry within the His-Purkinje system in man,’’ Circulation, vol. 50, pp. 1150-1162, 1974. [2] A. Mehdirad, S. Keim, K. Rst, T. Mazgalev and P. Tchou, “Asymmetry of retrograde conduction and re-entry within the His-Purkinje system: A comparative analysis of left and right ventricular stimulation,” JACC, vol. 24, pp. 177-184, 1994. [3] D. Wei, G. Yamada, T. Musha, H. Tsunakawa, T. Tsutsumi, and K. Hanuni, “Computer simulation of supraventricular tachycardia with the Wolff-ParkinsonWhite syndrome usmg three-dimensional heart models,” J Electrocardiol, vol. 23, pp. 261-273, 1990. [4] M. Lorange, and M.R Gulrajani, “A computer heart model incorporating anisotropic propagation. I . Model construction and simulation of normal activation,” J Electrocardiol, vol. 26, pp. 245-262, 1993. IS] R. Killmann, P. Wach, and F. Dienstl, “Threedimensional computer model of the entire human heart for simulation of re-entry and tachycardia: gap phenomenon and Wow-Parkinson-White syndrome,” Basic Res Cardiol ,vol. 56, pp. 485-501, 1991. [6] P.H. Fleischmann, G. Stark, P. Wach, “The antiarrhyhnc effect of verapamil on atrioventricular reentry in the Worn-Parkinson-White syndrome: a computer model study,” Int J Bio-Med Comput, vol. 41, pp. 125-136, 1996. [7] D. Durrer, R.Th. VAN DAM, G.E. FREUD,M.J. Janse, F.L. Meijler, and RC. Arzbaecher, “Total excitation of the isolated human heart,” Circulation, vol. 41, pp. 899912, 1970 [SI RM. Gulrajani, “Computer simulation of action potential changes in cardiac tissue, in Computers in Cardiology 1956, EEE Computer Society Press, 1986, pp. 629-632. [9] V. Elharrar, and B. Surawicz, “Action potential duration in canine Purkinje tissue: effects of precedmg excitation,” Am J Physiol, vol. 244, pp. H 782-792, 1983. [IO] M. Morgan, D. Cunningham, E. Rowland, “Relationship of the effective refiactory period and monophasic action potential duration after a step increase in pacing frequency,” PACE, vol. 13, pp. 1002-1008,1990. [111M.J. Janse, “The effect o f changes in the heart rate on the refractory period of the heart,” Ph. D. Thesis University of Amsterdam, Amsterdam, Netherlands, 1971, Acknowledgement This work was supported by the Austrian Science Foundation (FWF) grant number P-9995MED 156