用3个惯性测量单元估算跑步过程中的垂直地面反作用力

Bouke L. Scheltinga, Hazal Usta, J. Reenalda, J. Buurke
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引用次数: 2

摘要

-量化生物力学负荷对于深入了解导致跑步相关损伤的机制至关重要。地面反作用力(GRF)可以深入了解生物力学载荷,然而,测量GRF仅限于步态实验室。惯性传感器技术的发展使得在实验室之外的跑步者自己的环境中测量分段加速度和方向成为可能。本研究的主要目的是利用基于牛顿第二定律的通用算法估计三个惯性测量单元的垂直GRF。当使用牛顿第二定律时,已知加速度对应的质量分布和加速度信号的滤波设置确实对估计的力有影响。因此,本研究对过滤设置和片段质量进行了优化。为了将牛顿第二定律应用于整个物体,必须知道每个部分的加速度和质量。然而,这需要bbb10个传感器。通过将段的数量减少到三个,可以创建一个不那么引人注目的设置。12名后脚冲击(RFS)跑步者在仪器跑步机上以三种不同的速度(10,12和14km/h)和三种不同的步频(低,首选,高)进行了九次试验。惯性测量单元放置在胸骨、骨盆、小腿、胫骨和足部。通过优化,找到了最优的传感器配置。将估计的GRF与实测GRF之间的均方根误差(RMSE)作为优化的损失函数。采用RMSE、有源峰误差和Pearson相关系数作为算法的性能指标。在胫骨和骨盆上安装传感器效果最好,平均RMSE为0.179体重,峰值误差为3.6%,Pearson相关系数为0.98。通过留一个主体的交叉验证,表明该算法在RFS跑者群体中是可推广的。模型性能随速度的增加而降低,随步频的增加而增加。该算法的主要误差出现在姿态阶段的前25%,然而,总体性能与当前文献中描述的相当或更好。
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Estimating Vertical Ground Reaction Force during Running with 3 Inertial Measurement Units
- Quantification of biomechanical load is crucial to gain insights in the mechanisms causing running related injuries. Ground reaction forces (GRF) can give insights into biomechanical loading, however, measuring GRF is restricted to a gait laboratory. Developments in inertial sensor technology make it possible to measure segment accelerations and orientations outside the lab in the runners’ own environment. The main objective of this study is to estimate vertical GRF with three inertial measurement units using a generic algorithm based on Newtons second law. When using Newton’s second law, it is known that the mass distribution per corresponding acceleration and filtering settings of the acceleration signal do have an influence on the estimated force. Therefore, filtering settings and the mass of the segments were optimized in this study. To apply Newton’s second law to the full body, the accelerations and masses of every segment should be known. However, this requires >10 sensors. By minimizing the number of segments to three, a setup is created that is less obtrusive. Twelve rear foot strike (RFS) runners performed nine trials at three different velocities (10, 12 and 14km/h) and three different stride frequencies (low, preferred, high), on a instrumented treadmill. Inertial measurement units were placed at sternum, pelvis, upper legs, tibias and feet. An optimization was performed to find the optimal sensor configuration. The root mean squared error (RMSE) between the estimated GRF and measured GRF was used as loss function in the optimization. As performance measure of the algorithm, RMSE, active peak error and Pearson’s correlation coefficient were used. The setup with sensors on the tibia and pelvis showed the best result, with an average RMSE of 0.179 bodyweight, peak error of 3.6% and Pearson’s correlation coefficient of 0.98. Using leave-one-subject-out cross validation, it is shown that the algorithm is generalizable within the population of RFS runners. Model performance decreases with velocity but increases with stride frequency. The main error of the algorithm is seen in the first 25% of the stance phase, however, the general performance is comparable or better than what is described in current literature.
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