Fusejima K, Miyatake K, Okamoto M, Kinoshita N, Ohwa M, Tsumura K, Masuda K, Sakakibara H, Nimura Y
National Cardiovascular Center, Suita.
J Cardiol. 1987 Mar;17(1):139-48.
The purpose of this study was (1) to analyze the factors responsible for errors in the two-dimensional Doppler echographic measurements of cardiac output (C.O.) and (2) to establish a noninvasive method for measuring C.O. The subjects were 50 cardiac patients who had neither aortic valve disease nor intracardiac shunts. The C.O. was calculated using the following formula: C.O. (l/min) = mean flow velocity (cm/sec) x pi(aortic ring diameter/2)2 (cm2) x 60/10(3) Left ventricular ejection flow velocity was recorded in the center of the aortic ring from the apical approach. Mean velocity was calculated by integration of instantaneous mean velocity in the ejection phase divided by the cardiac cycle length, and was corrected by the Doppler incident angle. The inner diameter of the aortic ring was measured in the parasternal long-axis view at the time of the maximum ejection flow velocity. The following results were obtained: 1. Sources of error in the measurement of cardiac output. 1) Accuracy of instantaneous mean velocity calculating circuit: This calculating circuit was accurate in model experiments using pulsatile flow. 2) Effect of high-pass filter: In model circuits, application of high-pass filter overestimated flow velocity. The higher the cut-off frequency of the high-pass filter, the larger the overestimation. This was probably due to the parabolic flow velocity profile in the circuit. 3) Flow velocity profile in the aortic ring: The flow velocity profile seemed to be flat in the aortic ring except near the anterior aortic wall. Therefore, the effect of the high-pass filter was considered to be negligible in case of clinical application. 4) The effects of shift and size of sample volume: The location of sample volume relative to the aortic valve ring shifted about 7 mm during systole. However, the shift and size of sample volume seemed to have little effect on the measured C.O., because the flow velocity profile was nearly flat in the aortic ring. 5) Ultrasound beam incident angle: From a practical viewpoint, it was necessary to set an incident angle of less than 50 degrees for minimizing the error. We were able to set the angle within 50 degrees in all but one of patients. 6) Diameter of the aortic ring: Two-dimensional echographic measurement of the aortic ring diameter was not so accurate; it seemed to become a major source of error in the calculation of C.O.(ABSTRACT TRUNCATED AT 400 WORDS)
(1)分析二维多普勒超声心动图测量心输出量(C.O.)时产生误差的因素;(2)建立一种无创测量C.O.的方法。研究对象为50例既无主动脉瓣疾病也无心脏内分流的心脏病患者。C.O.采用以下公式计算:C.O.(升/分钟)=平均流速(厘米/秒)×π(主动脉环直径/2)²(平方厘米)×60/10³。左心室射血流速从心尖途径在主动脉环中心记录。平均流速通过将射血期瞬时平均流速积分除以心动周期长度来计算,并通过多普勒入射角进行校正。在最大射血流速时,于胸骨旁长轴视图测量主动脉环的内径。获得了以下结果:1. 心输出量测量中的误差来源。1)瞬时平均流速计算电路的准确性:该计算电路在使用脉动流的模型实验中是准确的。2)高通滤波器的影响:在模型电路中,应用高通滤波器会高估流速。高通滤波器的截止频率越高,高估程度越大。这可能是由于电路中的抛物线流速分布。3)主动脉环中的流速分布:除主动脉前壁附近外,主动脉环中的流速分布似乎是平坦的。因此,在临床应用中,高通滤波器的影响被认为可以忽略不计。4)样本容积的偏移和大小的影响:在收缩期,样本容积相对于主动脉瓣环的位置偏移约7毫米。然而,样本容积的偏移和大小似乎对测量的C.O.影响很小,因为主动脉环中的流速分布几乎是平坦的。5)超声束入射角:从实际角度来看,为使误差最小化,有必要将入射角设置小于50度。除1例患者外,我们能够将所有患者的角度设置在50度以内。6)主动脉环的直径:二维超声心动图测量主动脉环直径不太准确;它似乎成为计算C.O.时的主要误差来源。(摘要截断于400字)