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Distribution of lung tissue hysteresis during free breathing

机译:自由呼吸过程中肺组织滞后的分布

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Purpose: To characterize and quantify free breathing lung tissue motion distributions. Methods: Forty seven patient data sets were acquired using a 4DCT protocol consisting of 25 cine scans at abutting couch positions on a 16-slice scanner. The tidal volume of each scan was measured by simultaneously acquiring spirometry and an abdominal pneumatic bellows. The concept of a characteristic breath was developed to manage otherwise natural breathing pattern variations. The characteristic breath was found by first dividing the breathing traces into individual breaths, from maximum exhalation to maximum exhalation. A linear breathing drift model was assumed and the drift removed for each breath. Breaths that exceeded one standard deviation in period or amplitude were removed from further analysis. A characteristic breath was defined by normalizing each breath to a common amplitude, aligning the peak inhalation times for all of the breaths, and determining the average time at each tidal volume, keeping inhalation and exhalation separate. Breathing motion trajectories were computed using a previously published five-dimensional lung tissue trajectory model which expresses the position of internal lung tissue, X, as: X(v, f : Xo) = X0 + a(Xo)v + fi(Xo)f, where Xo is the internal lung tissue position at zero tidal volume and zero airflow, the scalar values v and/are the measured tidal volume and airflow, respectively, and the vectors alpha and beta are fitted free parameters. In order to characterize the motion patterns, the trajectory elongations were examined throughout the subject's lungs. Elongation was defined here by generating a rectangular bounding box with one side parallel to the alpha: vector and the box oriented in the plane defined by the alpha and beta motion vectors. Hysteresis motion was defined as the ratio of the box dimensions aligned orthogonal to and parallel to the alpha vector. The 15th and 85th percentile of the elongation were used to characterize tissue trajectory hysteresis. Results: The 15th and 85th percentile bounding box elongations were 0.090 ± 0.005 and 0.083 ±0.013 in the upper left lung and 0.187 ± 0.037 and 0.203 ± 0.053, in the lower left lung. The 15th and 85th percentiles for the upper right lung were 0.092 ± 0.006 and 0.085 ±0.013, and 0.184 ± 0.038, and 0.196 ± 0.043 in the lower right lung. Both percentiles were calculated for tidal volume displacements between 5 and 15 mm. In the left lung, the average elongations in the upper and lower lung were zeta = 0.120 ± 0.064 and zeta = 0.090 ± 0.055, respectively. The average elongations in the upper and lower right lung were zeta = 0.107 ± 0.060 and £ = 0.082 ± 0.048, respectively. The elongation varied smoothly throughout the lungs. Conclusions: The hysteresis motion was relatively small compared to the volume-filling motion, contributing between 8% and 20% of the overall motion. Statistically significant differences were observed in the range of hysteresis contribution for upper and lower lung regions. The characteristic breath process provided an excellent method for defining an average breath. The characteristic breath had continuous tidal volume and airflow characteristics when the breath was continuously repeated, useful for generating patterns representative of realistic motion for breathing motion studies.
机译:目的:表征和量化自由呼吸的肺组织运动分布。方法:使用4DCT协议获取47个患者数据集,该协议包括在16层扫描仪上靠靠的卧榻位置进行25次电影扫描。每次扫描的潮气量通过同时获取肺活量测定仪和腹部气动风箱来测量。发展了特征性呼吸的概念来管理自然的呼吸模式变化。通过首先将呼吸轨迹从最大呼气到最大呼气划分为单个呼吸来发现特征性呼吸。假定为线性呼吸漂移模型,并且每次呼吸均消除漂移。在周期或幅度上超过一个标准偏差的呼吸将从进一步分析中删除。通过将每次呼吸归一化为一个共同的振幅,对齐所有呼吸的峰值吸气时间,并确定每个潮气量的平均时间,保持吸气和呼气分开,来定义特征性呼吸。使用先前发布的五维肺组织轨迹模型计算呼吸运动轨迹,该模型将内部肺组织的位置X表示为:X(v,f:Xo)= X0 + a(Xo)v + fi(Xo) f,其中Xo是在零潮气量和零气流下的内部肺组织位置,标量v和/分别是测得的潮气量和气流,并且向量alpha和beta是自由拟合的参数。为了表征运动模式,检查了整个受试者肺部的轨迹伸长。延伸率是通过生成矩形边界框来定义的,该边界框的一侧平行于alpha:向量,并且该框的方向是由alpha和beta运动向量定义的平面。磁滞运动定义为垂直于和平行于alpha矢量对齐的框尺寸的比率。伸长率的第15个百分数和第85个百分数用于表征组织轨迹滞后。结果:左上肺第15和第85个百分位框伸长分别为0.090±0.005和0.083±0.013,左下肺分别为0.187±0.037和0.203±0.053。右上肺的第15和第85个百分位数分别为0.092±0.006和0.085±0.013,以及右下肺的0.184±0.038和0.196±0.043。计算两个百分位的潮气量在5到15 mm之间。在左肺中,上肺和下肺的平均伸长率分别为zeta = 0.120±0.064和zeta = 0.090±0.055。右上肺和右下肺的平均伸长率分别为zeta = 0.107±0.060和£ = 0.082±0.048。整个肺的伸长率平滑变化。结论:滞后运动与体积填充运动相比相对较小,占整体运动的8%至20%。在上下肺区域的滞后作用范围内观察到统计学上的显着差异。独特的呼吸过程为定义平均呼吸提供了一种极好的方法。连续重复呼吸时,特征性呼吸具有连续的潮气量和气流特征,可用于代表呼吸运动研究生成代表真实运动的模式。

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