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威尔逊中心端的绝对电压和导联向量。

The absolute voltage and the lead vector of Wilson's central terminal.

作者信息

Miyamoto N, Shimizu Y, Nishiyama G, Mashima S, Okamoto Y

机构信息

Department of Internal Medicine, Showa University Fujigaoka Hospital, Yokohama, Japan.

出版信息

Jpn Heart J. 1996 Mar;37(2):203-14. doi: 10.1536/ihj.37.203.

Abstract

The absolute potential value of Wilson's central terminal was calculated at 2 msec intervals during a cardiac cycle in 60 clinical cases. Starting from the body surface potential data at 128 thoracic locations, the effect of immersion of the body into an infinite conductor on the surface potential was calculated to obtain values with reference to zero potential at infinity. The conductivity of the outside medium was then made to approach zero. Comparison of the result with the original map showed nearly a constant shift of the potential, corresponding to the voltage of Wilson's terminal. In addition, the cardiac vector was calculated as the first approximation of the cardiac electromotive force and the lead vector of Wilson's terminal was obtained in order that the scalar product of the cardiac vector and the lead vector approximated the observed voltage of Wilson's terminal. The results indicate that the voltage of the Wilson electrode depended on the surface voltage with a peak value near the maximal QRS force in most of the cases. The peak voltage of Wilson's terminal was either positive or negative, and was 0.15 mV in absolute value on average. Voltage variations of Wilson's terminal during a cardiac cycle were 0.20 mV as an average of all cases. The voltage of Wilson's terminal also depended on the direction of the equivalent cardiac vector. The lead vector of Wilson's terminal was found to be directed superiorly in most of the cases. The average magnitude of the lead vector of Wilson's terminal was 0.097 omega/cm, which corresponded to about 1/4 of that of lead I.

摘要

在60例临床病例中,在心动周期内以2毫秒的间隔计算威尔逊中心端的绝对电位值。从128个胸部位置的体表电位数据出发,计算身体浸入无限导体中对表面电位的影响,以获得相对于无穷远处零电位的值。然后使外部介质的电导率趋近于零。将结果与原始图谱进行比较,发现电位几乎有一个恒定的偏移,对应于威尔逊端的电压。此外,计算心脏向量作为心脏电动势的一阶近似值,并获得威尔逊端的导联向量,以使心脏向量与导联向量的标量积近似于观察到的威尔逊端电压。结果表明,在大多数情况下,威尔逊电极的电压取决于表面电压,在最大QRS波力附近有一个峰值。威尔逊端的峰值电压可为正或负,绝对值平均为0.15mV。所有病例中威尔逊端在心动周期内的电压变化平均为0.20mV。威尔逊端的电压还取决于等效心脏向量的方向。发现大多数情况下威尔逊端的导联向量向上。威尔逊端导联向量的平均大小为0.097Ω/cm,约相当于I导联的1/4。

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