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首页> 外文期刊>IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control >Modeling and analysis of ultrasound backscattering by spherical aggregates and rouleaux of red blood cells
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Modeling and analysis of ultrasound backscattering by spherical aggregates and rouleaux of red blood cells

机译:球形聚集体和红细胞的球蛋白在超声散射中的建模与分析

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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/spl deg/, and the scatterer size (diameter for clumps and length for rouleaux) ranged from 4 /spl mu/m to 120 /spl mu/m. 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/spl deg/. 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.
机译:本研究涉及通过红细胞(RBC)聚集体进行超声反向散射的建模和分析,该聚集体在病理条件下在人血管内血液流变学中起重要作用。基于组织矩阵和点扩散函数之间的卷积的理论模型分别代表RBC聚集和超声系统的特征,用于检查散射体形状和大小对反向散射功率的影响。以RBC团块和rouleaux团块形式的两个散射体进行了建模。对于所有模拟,血细胞比容保持恒定在10%,超声频率为10 MHz,声化角在0到90 / spl deg /之间变化,散射体大小(团块直径和rouleaux长度)为4 / spl mu / m至120 / spl mu / m。在假定空间中散射体的泊松分布的瑞利散射下,超声反向散射功率随粒子体积线性增加。对于非瑞利散射体,回声的强度随着散射体体积的增加而减小,除了rouleaux的角度为90 / spl deg /。不出所料,各向异性粒子(rouleaux)的反向散射功率与角度有关。超声的反向散射功率并不总是随聚集体的大小而增加,尤其是当它们不再是瑞利散射体时。在鲁勒的情况下,在非瑞利区域中强调了反向散射功率的各向异性。

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