[脉冲多普勒超声心动图估计室间隔缺损的压力梯度:特别参考潜在的误差因素]。

Journal of cardiography Pub Date : 1986-03-01
H Tomita, T Shimizu, Y Arakaki, S Nakaya, S Futaki, T Nakajima, T Kamiya, K Miyatake, Y Nimura
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引用次数: 0

摘要

本文研究了脉冲多普勒超声心动图(PD)在无创室间隔缺损压差(delta P)评估中的临床有效性和一些问题。利用简化的伯努利方程将右心室左向右分流血流的最大流速(max V)转换为δ P: δ P = 4V2。我们还使用公式:δ P = 4(V2(2) - V1(2))来估计左心室左向右高速分流血流的δ P。11例患者在心导管术中同时记录左、右心室压和PD。在9例实际P值较大(大于41 mmHg)的患者和8例右心室收缩压高(等于或高于左心室收缩压)的患者中,仅从右心室左向右分流血流的最大流速来准确地多普勒估计P值是不可能的。除这17例外,39例全收缩期右心室左向右分流的PD用简化伯努利方程估计的δ P与实际测量的δ P相关性较好(Y = 0.99X + 2.77, r = 0.91, P < 0.01)。最大瞬时压力梯度和多普勒δ P的差异被认为是微不足道的(在0和7mmhg之间,平均4mmhg)。在9例左心室也观察到高速左向右分流血流(0.63约2.00 m/sec,平均1.31 m/sec),使用简化伯努利方程计算δ P,实际测量的δ P高估了2 ~ 16 mmHg (Y = 1.52X + 4.88, r = 0.95, P < 0.01)。然而,如果使用公式δ P = 4(V2(2) - V1(2))来估计δ P,而不忽略左心室(V1)的最大速度,则它与实际测量的δ P相关性良好(Y = 1.07X + 0.76, r = 0.98, P小于0.01)。因此,在左心室高速左向右分流的情况下,脉冲多普勒超声心动图对δ P的估计公式:δ P = 4(V2(2) - V1(2))更为准确。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
[Pulsed Doppler echocardiographic estimation of pressure gradient across a ventricular septal defect: with particular reference to potential factors of error].

The clinical validity and some problems concerning pulsed Doppler echocardiography (PD) in non-invasive estimates of pressure difference (delta P) across a ventricular septal defect were studied. The maximum velocity (max V) of the left to right shunt flow in the right ventricle was converted to delta P using the simplified Bernoulli equation: delta P = 4V2. We also used the equation: delta P = 4(V2(2) - V1(2)) to estimate the delta P in cases who had left to right shunt flows of high velocity in the left ventricle. Simulatenous recordings of both left and right ventricular pressures and PD were obtained during cardiac catheterization of 11 cases. Accurate Doppler estimates of delta P only from the maximum velocity of the left to right shunt flow in the right ventricle were impossible in nine cases whose actual delta P's were large (more than 41 mmHg) and also in eight cases whose right ventricular systolic pressure was high (either equal to or higher than left ventricular systolic pressure). Besides these 17 cases, delta P estimated by PD using the simplified Bernoulli equation in 39 cases, with pansystolic left to right shunt flows in the right ventricle, correlated well with the actually measured delta P (Y = 0.99X + 2.77, r = 0.91, p less than 0.01). The difference in the maximal instantaneous pressure gradient and Doppler delta P was considered insignificant (between 0 and 7 mmHg, mean 4 mmHg). In nine cases, the left to right shunt flows of relatively high speed (0.63 approximately 2.00 m/sec, mean 1.31 m/sec) were observed also in the left ventricle, and calculated delta P using the simplified Bernoulli equation overestimated the actually measured delta P by 2 to 16 mmHg (Y = 1.52X + 4.88, r = 0.95, p less than 0.01). However, if the delta P is estimated by using the equation, delta P = 4(V2(2) - V1(2)), without ignoring the maximum speed in the left ventricle (V1), it correlates well with the actually measured delta P (Y = 1.07X + 0.76, r = 0.98, p less than 0.01). Thus, in cases with left to right shunt flows with high speeds in the left ventricle, the equation: delta P = 4(V2(2) - V1(2)) was more accurate in estimating the delta P by pulsed Doppler echocardiography.

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