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A comparison of modelling procedures used to estimate the power–exhaustion time relationship

机译:用来估计功率与功率消耗时间关系的建模程序的比较

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This study aimed to test the consistency of using the power required to elicit maximal oxygen uptake during incremental test (P t) to demarcate the range of power intensity in the modelling of the power–exhaustion time relationship. Different mathematical procedures were tested using data from ten subjects exercising on a cycle ergometer. After the determination of P t and the power at the ventilatory threshold, the subjects did six tests at constant power to exhaustion within 2–15 min. Estimates were obtained from a segmented model using two distinct equations of the anaerobic contribution to power below and above P t, respectively. This model fit the overall data with a better adequacy than the simple hyperbolic model (standard error of 29.2 ± 25.2 vs. 42.3 ± 25.2 s). The power asymptotes were 225.7 ± 27.3 W from the segmented model, 226.2 ± 27.3 and 283.3 ± 20.5 W from the simple model applied to data below and above P t, respectively. The estimates from the segmented model were strongly correlated with their analogues from the simple model applied only to data below P t (R = 1.00 for power asymptote and curvature coefficient). They were not correlated with their analogues from the simple model applied only to data above P t. These discrepancies between modelling procedures could arise from the method used to determine P t and the oversimplification of the oxygen uptake kinetics. These limitations could lead the segmented model to an overestimation of the anaerobic contribution which was around 15% of total energy expended at P t. Keywords Anaerobic metabolism - Performance - Critical power Communicated by Susan Ward.
机译:这项研究的目的是检验在功率消耗时间关系模型中使用增量试验(P t )中最大摄氧量所需功率来划分功率强度范围的一致性。使用来自在自行车测功机上锻炼的十名受试者的数据测试了不同的数学程序。在确定P t 和通气阈值下的力量后,受试者在2-15分钟内以恒定力量进行了六项测试,以进行力竭。使用两个不同的分别对P t 之上和之上的厌氧功率贡献的方程,从分段模型中获得估计值。与简单的双曲线模型相比,该模型更适合整体数据(标准误差为29.2±25.2 vs. 42.3±25.2 s)。分段模型的功率渐近功率为225.7±27.3 W,简单模型的功率渐近功率分别为P t 之上和之上的简单模型为226.2±27.3 W和283.3±20.5W。分割模型的估计值与简单模型的类似物密切相关,后者仅适用于P t 以下的数据(对于功率渐近线和曲率系数,R = 1.00)。它们与仅适用于P t 以上数据的简单模型中的类似物没有关联。建模过程之间的这些差异可能是由用于确定P t 的方法和过分简化的氧气吸收动力学引起的。这些局限性可能导致分割的模型高估了厌氧的贡献,大约占P t 消耗的总能量的15%。关键字无氧代谢-性能-临界功率由Susan Ward传达。

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