Kanai Hiroshi
Department of Electronic Engineering, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan.
IEEE Trans Ultrason Ferroelectr Freq Control. 2005 Nov;52(11):1931-42. doi: 10.1109/tuffc.2005.1561662.
Though myocardial viscoelasticity is essential in the evaluation of heart diastolic properties, it has never been noninvasively measured in vivo. By the ultrasonic measurement of the myocardial motion, we have already found that some pulsive waves are spontaneously excited by aortic-valve closure (AVC) at end-systole (T0). These waves may serve as an ideal source of the intrinsic heart sound caused by AVC. In this study, using a sparse sector scan, in which the beam directions are restricted to about 16, the pulsive waves were measured almost simultaneously at about 160 points set along the heart wall at a sufficiently high frame rate. The consecutive spatial phase distributions, obtained by the Fourier transform of the measured waves, clearly revealed wave propagation along the heart wall for the first time. The propagation time of the wave along the heart wall is very small (namely, several milliseconds) and cannot be measured by conventional equipment. Based on this phenomenon, we developed a means to measure the myocardial viscoelasticity in vivo. In this measurement, the phase velocity of the wave is determined for each frequency component. By comparing the dispersion of the phase velocity with the theoretical one of the Lamb wave (the plate flexural wave), which propagates along the viscoelastic plate (heart wall) immersed in blood, the instantaneous viscoelasticity is determined noninvasively. This is the first report of such noninvasive determination. In in vivo experiments applied to five healthy subjects, propagation of the pulsive wave was clearly visible in all subjects. For the 60-Hz component, the typical propagation speed rapidly decreased from 5 m/s just before the time of AVC (t = T0 - 8 ms) to 3 m/s at t = T0 + 10 ms. In the experiments, it was possible to determine the viscosity more precisely than the elasticity. The typical value of elasticity was about 24-30 kPa and did not change around the time of AVC. The typical transient values of viscosity decreased rapidly from 400 Pa x s at t = T0 - 8 ms to 70 Pa x s at t = T0 + 10 ms. The measured shear elasticity and viscosity in this study are comparable to those obtained for the human tissues using audio frequency in in vitro experiments reported in the literature.
尽管心肌粘弹性在评估心脏舒张特性方面至关重要,但从未在体内进行过无创测量。通过超声测量心肌运动,我们已经发现,在收缩末期(T0)主动脉瓣关闭(AVC)时会自发激发一些脉冲波。这些波可能是AVC引起的心脏固有心音的理想来源。在本研究中,使用稀疏扇形扫描(其中波束方向限制在约16个),以足够高的帧率在沿心脏壁设置的约160个点几乎同时测量脉冲波。通过对测量波进行傅里叶变换获得的连续空间相位分布首次清楚地揭示了波沿心脏壁传播。波沿心脏壁的传播时间非常短(即几毫秒),无法用传统设备测量。基于这一现象,我们开发了一种在体内测量心肌粘弹性的方法。在该测量中,可以为每个频率分量确定波的相速度。通过将相速度的色散与沿浸入血液中的粘弹性板(心脏壁)传播的兰姆波(板弯曲波)理论色散进行比较,可以无创地确定瞬时粘弹性。这是关于这种无创测定的首次报道。在应用于五名健康受试者的体内实验中,所有受试者中脉冲波传播均清晰可见。对于60Hz分量,典型传播速度在AVC之前(t = T0 - 8ms)时从5m/s迅速降至t = T0 + 10ms时的3m/s。在实验中,可以比弹性更精确地确定粘度。弹性的典型值约为24 - 30kPa,在AVC时刻前后没有变化。粘度的典型瞬态值从t = T0 - 8ms时的400Pa·s迅速降至t = T0 + 10ms时的70Pa·s。本研究中测量的剪切弹性和粘度与文献报道的体外实验中使用音频频率获得的值相当。