Paeng D G, Cao P J, Shung K K
Acoustics Program, The Pennsylvania State University, University Park, PA 16802, USA.
Ultrasound Med Biol. 2001 Sep;27(9):1245-54. doi: 10.1016/s0301-5629(01)00405-7.
Although a number of recent studies have demonstrated that the echogenicity of blood varies as a function of time under pulsatile flow, the fundamental mechanisms responsible for it are still uncertain. To better understand this phenomenon, the Doppler power from porcine blood and polystyrene microsphere suspensions was measured at the center of the tube as functions of two crucial parameters, flow velocity and stroke rate (for pulsatile flow), under steady and pulsatile flow in a mock flow loop. In the present study, the experimental results were obtained with a 10-MHz pulsed Doppler system with a frequency response estimated more accurately by electronic injection, and validated by comparing to the radiofrequency (RF) signal acquired from the same Doppler instrument. The results show that the Doppler power from microspheres and porcine red blood cell (RBC) suspensions did not vary appreciably (< 2 dB), with either the speed or stroke rate (for pulsatile flow only) under steady and pulsatile flow. It was found that the Doppler power from porcine whole blood under steady flow decreased with the speed by approximately 13 dB from 3 to 33 cm/s and was only 3 dB higher than that from RBC suspension at 33 cm/s, suggesting minimal RBC aggregation in whole blood at this speed. The apparent cyclic variation from whole blood was observed at 20 and 40 beats/min (BPM). The cyclic variation became more obvious as the speed and stroke rate decreased. The mean Doppler power over a cycle increased as the peak speed decreased. The Doppler power reached a maximum near peak systole and a minimum at late diastole at the center of the tube. This pattern cannot be explained by RBC aggregation due to the shear rate alone, and may be attributed to acceleration and deceleration along with aggregation. The cyclic variation was not observed at 60 BPM, probably because of a lack of time for aggregation to occur.
尽管最近的一些研究表明,在脉动流作用下,血液的回声性会随时间变化,但其背后的基本机制仍不明确。为了更好地理解这一现象,在模拟血流回路中,分别在稳态流和脉动流条件下,测量了猪血液和聚苯乙烯微球悬浮液在管中心处的多普勒功率,该功率是流速和搏率(针对脉动流)这两个关键参数的函数。在本研究中,实验结果是通过一个10兆赫的脉冲多普勒系统获得的,其频率响应通过电子注入得到更精确估计,并与从同一多普勒仪器获取的射频(RF)信号进行比较来验证。结果表明,在稳态流和脉动流条件下,微球和猪红细胞(RBC)悬浮液的多普勒功率,随速度或搏率(仅针对脉动流)变化不明显(<2分贝)。研究发现,稳态流条件下猪全血的多普勒功率随速度从3厘米/秒降至33厘米/秒时下降约13分贝,在33厘米/秒时仅比RBC悬浮液的多普勒功率高3分贝,这表明在此速度下全血中红细胞聚集极少。在20次/分钟和40次/分钟(BPM)时观察到全血有明显的周期性变化。随着速度和搏率降低,周期性变化变得更明显。一个周期内的平均多普勒功率随峰值速度降低而增加。在管中心处,多普勒功率在收缩期峰值附近达到最大值,在舒张期末期达到最小值。这种模式不能仅用剪切率导致的红细胞聚集来解释,可能归因于加速、减速以及聚集。在60次/分钟(BPM)时未观察到周期性变化,可能是因为没有足够时间发生聚集。