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一个包含各向异性传播的计算机心脏模型。II. 传导阻滞的模拟

A computer heart model incorporating anisotropic propagation. II. Simulations of conduction block.

作者信息

Lorange M, Gulrajani R M, Nadeau R A, Préda I

机构信息

Research Center, Hôpital du Sacré-Coeur, Montreal, Quebec, Canada.

出版信息

J Electrocardiol. 1993 Oct;26(4):263-77. doi: 10.1016/0022-0736(93)90048-i.

DOI:10.1016/0022-0736(93)90048-i
PMID:8228716
Abstract

This study describes the simulation of the more common types of conduction blocks with a computer model of the heart incorporating anisotropic propagation. The rationale was to test the model as to its ability to simulate these blocks by physiologically justifiable adjustments of the conduction system alone. The complete blocks were generated by simply blocking conduction totally at selected sites in the proximal conduction system, and the incomplete blocks by slowing down the conduction velocity in the proximal system. Also simulated were the left fascicular blocks and the bilateral blocks. All simulated electrocardiograms, vectorcardiograms, body surface potential maps, and epicardial isochrones for these blocks were similar to clinically observed data, with the exception of the left posterior hemiblock, which was slightly atypical. This could be because such blocks are usually accompanied by other cardiac pathologies not included in our simulations. The model also supports van Dam's observation that during left bundle branch block the passage of activation from right to left occurs via slow myocardial activation with no evidence of a local delay due to a septal barrier. Finally, the model suggests that a left bundle branch block with a normal frontal plane QRS axis may simply represent a case of an incomplete left bundle block, whereas one that exhibits a left axis QRS deviation in the frontal plane represents a more severe complete left bundle branch block.

摘要

本研究描述了利用包含各向异性传播的心脏计算机模型对更常见类型的传导阻滞进行模拟。其基本原理是仅通过对传导系统进行生理学上合理的调整来测试该模型模拟这些阻滞的能力。完全性阻滞是通过在近端传导系统的选定部位完全阻断传导产生的,而不完全性阻滞则是通过减慢近端系统的传导速度产生的。还模拟了左束支阻滞和双侧阻滞。所有这些阻滞的模拟心电图、向量心电图、体表电位图和心外膜等时线均与临床观察数据相似,但左后分支阻滞略有非典型性。这可能是因为此类阻滞通常伴有我们模拟中未包含的其他心脏病变。该模型还支持范·达姆的观察结果,即在左束支阻滞期间,激动从右向左的传导是通过缓慢的心肌激活发生的,没有证据表明存在由于室间隔屏障导致的局部延迟。最后,该模型表明,额面QRS轴正常的左束支阻滞可能仅仅代表不完全性左束支阻滞的一种情况,而在额面表现为QRS轴左偏的左束支阻滞则代表更严重的完全性左束支阻滞。

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引用本文的文献

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Mathematical modeling and simulation of ventricular activation sequences: implications for cardiac resynchronization therapy.心室激动序列的数学建模与模拟:对心脏再同步治疗的启示。
J Cardiovasc Transl Res. 2012 Apr;5(2):146-58. doi: 10.1007/s12265-011-9343-6. Epub 2012 Jan 27.
2
Bundle branch reentry tachycardia: why is the HV interval often longer than in sinus rhythm? The critical role of anisotropic conduction.束支折返性心动过速:为何希氏束至心室(HV)间期常比窦性心律时更长?各向异性传导的关键作用。
J Interv Card Electrophysiol. 2001 Jun;5(2):173-6. doi: 10.1023/a:1011481508929.