Teh B G, Cloutier G
Cypress Semicond., San Jose, CA.
IEEE Trans Ultrason Ferroelectr Freq Control. 2000;47(4):1025-35. doi: 10.1109/58.852086.
The present study concerns the modeling and analysis of ultrasound backscattering by red blood cell (RBC) aggregates, which under pathological conditions play a significant role in the rheology of blood within human vessels. A theoretical model based on the convolution between a tissue matrix and a point spread function, representing, respectively, the RBC aggregates and the characteristics of the ultrasound system, was used to examine the influence of the scatterer shape and size on the backscattered power. Both scatterers in the form of clumps of RBC aggregates and rouleaux were modeled. For all simulations, the hematocrit was kept constant at 10%, the ultrasound frequency was 10 MHz, the insonification angle was varied from 0 to 90 degrees , and the scatterer size (diameter for clumps and length for rouleaux) ranged from 4 mum to 120 mum. Under Rayleigh scattering by assuming a Poisson distribution of scatterers in space, the ultrasound backscattered power increased linearly with the particle volume. For non-Rayleigh scatterers, the intensity of the echoes diminished as the scatterer volume increased, with the exception of rouleaux at an angle of 90 degrees . As expected, the backscattered power was angularly dependent for anisotropic particles (rouleaux). The ultrasound backscattered power did not always increase with the size of the aggregates, especially when they were no longer Rayleigh scatterers. In the case of rouleaux, the anisotropy of the backscattered power is emphasized in the non-Rayleigh region.
本研究涉及红细胞(RBC)聚集体超声背向散射的建模与分析,在病理条件下,RBC聚集体在人体血管内血液流变学中起重要作用。基于组织矩阵与点扩散函数卷积的理论模型,分别表示RBC聚集体和超声系统的特性,用于研究散射体形状和大小对背向散射功率的影响。对RBC聚集体团块和缗钱状两种形式的散射体都进行了建模。所有模拟中,血细胞比容保持在10%不变,超声频率为10MHz,声入射角从0度到90度变化,散射体大小(团块的直径和缗钱状的长度)范围为4μm到120μm。在瑞利散射条件下,假设散射体在空间呈泊松分布,超声背向散射功率随颗粒体积线性增加。对于非瑞利散射体,除了90度入射角的缗钱状散射体外,回波强度随散射体体积增加而减弱。正如预期的那样,对于各向异性颗粒(缗钱状),背向散射功率与角度有关。超声背向散射功率并不总是随聚集体大小增加,特别是当它们不再是瑞利散射体时。在缗钱状的情况下,背向散射功率的各向异性在非瑞利区域更为明显。