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Turbulence intensity in a region of interest 2cm distal to the carotid bifurcation in a family of seven anthropomorphic flow phantoms

机译:七个拟人流幻影家族中距颈动脉分叉远2cm的目标区域的湍流强度

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An in vitro flow system has been used to assess the flow disturbances downstream of the stenosis in a family of seven carotid bifurcation phantoms modelling varying plaque build-up both axially symmetrically (concentrically) and asymmetrically (eccentrically). Radio frequency data were collected for 10 s at each of over 1000 sites within each model, and a sliding 1024-point FFT is applied to the data to extract the Doppler spectrum every 12 ms. From this, the ensemble average over 10 cardiac cycles of the spectral mean velocity, and the root mean square over these same 10 cardiac cycles - the turbulence intensity (TI), can be obtained as a function of an ensemble averaged cardiac cycle at each spatial point in all phantoms. TI was investigated by looking at the average over a 25 mm2 square region of interest in the ICA centered 2 cm distal to the apex of the bifurcation. TI in the region of interest increased with stenosis severity; at 23ms following peak systole, the time point when TI was maximal for the majority of models, this ranged from 2.4±0.1 cm/s in the non-diseased model to 6.6+-0.3, 16.0+-1.4 and 26.1+-1.3 cm/s in the 30, 50 and 70% concentrically stenosed (by NASCET criteria) models, respectively. Similarly, TI was 8.3+-0.7,19.9+-1.1, and 26.2+-1.2 cm/s in the 30, 50 and 70% eccentrically stenosed models, respectively. Differences in TI between models, both in increasing stenosis severity and between eccentricities, were statistically different except between the 70% concentric and eccentric models.
机译:体外血流系统已用于评估七个颈动脉分叉模型中狭窄下游的血流扰动,该模型模拟了轴向对称(同心)和非对称(偏心)的斑块堆积变化。在每个模型的1000多个位置中的每个位置上收集了10 s的射频数据,并对数据进行了1024点滑动FFT,每12 ms提取一次多普勒频谱。由此,可以得出频谱平均速度在10个心动周期上的集合平均数,以及在相同的10个心动周期上的均方根-湍流强度(TI),作为每个空间上集合平均心动周期的函数指向所有幻像。通过查看以分叉顶点为中心2 cm的ICA中25平方毫米的目标区域的平均值,对TI进行了研究。感兴趣区域的TI随着狭窄程度的增加而增加;在峰值收缩后的23ms处,大多数模型的TI达到最大的时间点,范围从非疾病模型的2.4±0.1 cm / s到6.6 + -0.3、16.0 + -1.4和26.1 + -1.3 cm / s分别在30%,50%和70%同心球变(按NASCET标准)模型中。同样,在30%,50%和70%的偏心狭窄模型中,TI分别为8.3 + -0.7、19.9 + -1.1和26.2 + -1.2 cm / s。除狭窄程度增加和偏心率增加外,模型之间的TI差异在统计学上均不同,除了70%的同心和偏心模型之间。

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