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安静站立时平衡的刚度控制

Stiffness control of balance in quiet standing.

作者信息

Winter D A, Patla A E, Prince F, Ishac M, Gielo-Perczak K

机构信息

Department of Kinesiology, University of Waterloo, Ontario, Canada.

出版信息

J Neurophysiol. 1998 Sep;80(3):1211-21. doi: 10.1152/jn.1998.80.3.1211.

DOI:10.1152/jn.1998.80.3.1211
PMID:9744933
Abstract

Our goal was to provide some insights into how the CNS controls and maintains an upright standing posture, which is an integral part of activities of daily living. Although researchers have used simple performance measures of maintenance of this posture quite effectively in clinical decision making, the mechanisms and control principles involved have not been clear. We propose a relatively simple control scheme for regulation of upright posture that provides almost instantaneous corrective response and reduces the operating demands on the CNS. The analytic model is derived and experimentally validated. A stiffness model was developed for quiet standing. The model assumes that muscles act as springs to cause the center-of-pressure (COP) to move in phase with the center-of-mass (COM) as the body sways about some desired position. In the sagittal plane this stiffness control exists at the ankle plantarflexors, in the frontal plane by the hip abductors/adductors. On the basis of observations that the COP-COM error signal continuously oscillates, it is evident that the inverted pendulum model is severely underdamped, approaching the undamped condition. The spectrum of this error signal is seen to match that of a tuned mass, spring, damper system, and a curve fit of this "tuned circuit" yields omega n the undamped natural frequency of the system. The effective stiffness of the system, Ke, is then estimated from Ke = I omega n2, and the damping B is estimated from B = BW X I, where BW is the bandwidth of the tuned response (in rad/s), and I is the moment of inertia of the body about the ankle joint. Ten adult subjects were assessed while standing quietly at three stance widths: 50% hip-to-hip distance, 100 and 150%. Subjects stood for 2 min in each position with eyes open; the 100% stance width was repeated with eyes closed. In all trials and in both planes, the COP oscillated virtually in phase (within 6 ms) with COM, which was predicted by a simple 0th order spring model. Sway amplitude decreased as stance width increased, and Ke increased with stance width. A stiffness model would predict sway to vary as Ke-0.5. The experimental results were close to this prediction: sway was proportional to Ke(-0.55). Reactive control of balance was not evident for several reasons. The visual system does not appear to contribute because no significant difference between eyes open and eyes closed results was found at 100% stance width. Vestibular (otolith) and joint proprioceptive reactive control were discounted because the necessary head accelerations, joint displacements, and velocities were well below reported thresholds. Besides, any reactive control would predict that COP would considerably lag (150-250 ms) behind the COM. Because the average COP was only 4 ms delayed behind the COM, reactive control was not evident; this small delay was accounted for by the damping in the tuned mechanical system.

摘要

我们的目标是深入了解中枢神经系统如何控制和维持直立站姿,这是日常生活活动中不可或缺的一部分。尽管研究人员在临床决策中相当有效地使用了维持这种姿势的简单性能指标,但其中涉及的机制和控制原则尚不清楚。我们提出了一种相对简单的直立姿势调节控制方案,该方案能提供几乎即时的纠正反应,并降低对中枢神经系统的操作要求。推导并通过实验验证了该分析模型。针对安静站立开发了一个刚度模型。该模型假设肌肉起到弹簧的作用,使压力中心(COP)在身体围绕某个期望位置摆动时与质心(COM)同步移动。在矢状面中,这种刚度控制存在于踝跖屈肌,在额状面中则由髋外展肌/内收肌实现。基于压力中心 - 质心误差信号持续振荡的观察结果,很明显倒立摆模型严重欠阻尼,接近无阻尼状态。该误差信号的频谱与调谐质量、弹簧、阻尼器系统的频谱相匹配,对这个“调谐电路”的曲线拟合得出系统的无阻尼固有频率ωn。然后根据Ke = Iωn²估计系统的有效刚度Ke,并根据B = BW×I估计阻尼B,其中BW是调谐响应的带宽(单位为rad/s),I是身体绕踝关节的转动惯量。对10名成年受试者在三种站立宽度下安静站立时进行了评估:髋部间距的50%、100%和150%。受试者在每个位置睁眼站立2分钟;100%站立宽度的情况在闭眼时重复进行。在所有试验以及两个平面中,压力中心实际上与质心同相振荡(在6毫秒内),这由一个简单的零阶弹簧模型预测得出。摆动幅度随着站立宽度增加而减小,并且有效刚度Ke随着站立宽度增加而增大。刚度模型会预测摆动幅度随Ke -0.5变化。实验结果接近这一预测:摆动幅度与Ke(-⒈55)成正比。平衡的反应性控制不明显有几个原因。视觉系统似乎没有起到作用,因为在100%站立宽度下睁眼和闭眼的结果没有显著差异。前庭(耳石)和关节本体感觉的反应性控制被排除,因为必要的头部加速度、关节位移和速度远低于报道的阈值。此外,任何反应性控制都会预测压力中心会在质心之后相当大的延迟(150 - 250毫秒)。由于压力中心平均仅比质心延迟4毫秒,所以反应性控制不明显;这个小延迟是由调谐机械系统中的阻尼导致的。

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