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用于心脏多极分量逆恢复的表面积分和最小二乘法程序。

Surface integration and least-squares procedures for the inverse recovery of cardiac multipole components.

作者信息

Dubé B, Savard P, Guardo R, Gulrajani R M, Drouhard J P

出版信息

Ann Biomed Eng. 1985;13(1):43-58. doi: 10.1007/BF02371249.

Abstract

A simulation study was performed to evaluate different recovery procedures for computing the multipole components of the cardiac electrical activity. A series of dipolar potential distributions was first generated on a realistic numerical model of the human torso. Then, different procedures based on surface integration (SI) and least-squares (LS) minimization were used to compute the multipole components. The parameters of a single moving dipole (SMD) computed from the estimated multipoles were compared with those of the original dipole source. For a finite and homogeneous simulation as well as recovery medium, the results showed that SI employing the potentials over all 1216 surface elements of the torso model was not affected by the various numerical approximations used to perform the integration (e.g., rms error for the SMD position, p = 0.7 mm). By integrating the potentials with truncated capping surfaces at the neck and the waist, the recovery errors increased (p = 2.1 mm). Sampling the potentials at 63 sites, followed by interpolation over the rest of the torso surface, severely affected the SI results for the SMD (p = 6.4 mm), as compared with LS minimization using also 63 values (p = 0.9 mm). With lungs and intraventricular blood masses in the simulation medium but a finite and homogeneous recovery medium, SI was less effective (p = 10.8 mm) than LS (p = 8.6 mm). Adequate compensation for the effects of lungs was obtained by including regions of lower electrical conductivity in the recovery medium for LS, and by a correction matrix for SI. In general, LS gave better results than SI, but with a higher initial computation time.

摘要

进行了一项模拟研究,以评估计算心脏电活动多极分量的不同恢复程序。首先在逼真的人体躯干数值模型上生成一系列偶极电位分布。然后,使用基于表面积分(SI)和最小二乘(LS)最小化的不同程序来计算多极分量。将根据估计的多极计算出的单个移动偶极(SMD)的参数与原始偶极源的参数进行比较。对于有限且均匀的模拟以及恢复介质,结果表明,采用躯干模型所有1216个表面元素上的电位的SI不受用于执行积分的各种数值近似的影响(例如,SMD位置的均方根误差,p = 0.7毫米)。通过在颈部和腰部用截断的覆盖表面对电位进行积分,恢复误差增加(p = 2.1毫米)。与同样使用63个值的LS最小化(p = 0.9毫米)相比,在63个位点对电位进行采样,然后在躯干表面的其余部分进行插值,严重影响了SMD的SI结果(p = 6.4毫米)。在模拟介质中存在肺部和心室内血肿但恢复介质有限且均匀的情况下,SI的效果(p = 10.8毫米)不如LS(p = 8.6毫米)。通过在LS的恢复介质中包含较低电导率区域以及通过SI的校正矩阵,可以充分补偿肺部的影响。一般来说,LS比SI给出的结果更好,但初始计算时间更长。

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