Participants
Ten adult males (mean ± standard deviation (SD) age: 22.6 ± 1.5 years, height: 1.70 ± 0.05 m, body mass: 64.6 ± 6.0 kg) participated in this study. All participants reviewed and signed an informed consent form. All participants were asked to review and sign an informed consent form prior to participating in the study. The study protocol was conducted in accordance with the guidelines proposed in the Declaration of Helsinki and was reviewed and approved by the Institutional Review Board at Ritsumeikan University, Biwako-Kusatsu Campus in Japan.
Data collection
The participants were instructed to walk continuously and run on a 20 m circuit runway five times while maintaining their preferred speed. Three-dimensional position data of the lower extremities along a straight distance of 5 m of the runway (from a 2.5–7.5 m section of the runway) during the third lap in each trial were recorded using a 24-camera-motion capture system at 250 Hz (MAC3D, Motion Analysis Corporation, California, USA). A total of 26 reflective markers were placed on each participant’s body at the anatomical landmarks to measure the three-dimensional positions of the segments 7.
Data analysis
Three linked rigid body models with different DOF represented the lower extremities in each trial. These models have 9 (9-DOF model), 18 (18-DOF model), and 22 DOFs (22-DOF model). The 9-DOF model is planar in the sagittal plane and has often been used as a simple model in human locomotion analysis 3,8,9. The 18-DOF model has been widely used in the three-dimensional musculoskeletal computer simulations of human locomotion 1,2. The 22-DOF model was constructed as the most complex model under the experimental conditions in this study. The DOFs of each model are listed in Table 1.
Table 1
Joints and their degrees of freedom implemented in the models.
Segment | | Joint | | Movements | | DOF |
| | | 9-DoF | 18-DoF | 22-DoF |
Pelvis | | GCS | | x (Anterior-posterior direction) | | 〇 | 〇 | 〇 |
| | | | y (Vertical direction) | | 〇 | 〇 | 〇 |
| | | | z (Medio-lateral direction) | | | 〇 | 〇 |
| | | | Rotation about the medio-lateral axis | | 〇 | 〇 | 〇 |
| | | | Rotation about the anterior-posterior axis | | | 〇 | 〇 |
| | | | Rotation about the vertical axis | | | 〇 | 〇 |
Right Thigh | | Right Hip | | Flexion/Extension | | 〇 | 〇 | 〇 |
| | | | Internal/External Rotation | | | 〇 | 〇 |
| | | | Adduction/Abduction | | | 〇 | 〇 |
Right Shank | | Right Knee | | Flexion/Extension | | 〇 | 〇 | 〇 |
| | | | Internal/External Rotation | | | | 〇 |
| | | | Adduction/Abduction | | | | 〇 |
Right Foot | | Right Ankle | | Dorsi/Plantar Flexion | | 〇 | 〇 | 〇 |
| | | | Inversion/Eversion | | | 〇 | 〇 |
Left Thigh | | Left Hip | | Flexion/Extension | | 〇 | 〇 | 〇 |
| | | | Internal/External Rotation | | | 〇 | 〇 |
| | | | Adduction/Abduction | | | 〇 | 〇 |
Left Shank | | Left Knee | | Flexion/Extension | | 〇 | 〇 | 〇 |
| | | | Internal/External Rotation | | | | 〇 |
| | | | Adduction/Abduction | | | | 〇 |
Left Foot | | Left Ankle | | Dorsi/Plantar Flexion | | 〇 | 〇 | 〇 |
| | | | Inversion/Eversion | | | 〇 | 〇 |
A local coordinate system was defined for each rigid-body segment. The position data of the markers in each local coordinate system were transformed using a simultaneous transformation matrix (STM). A set of parameters for the STM at each frame was determined using a nonlinear optimization algorithm (fmincon in the MATLAB optimization toolbox) to minimize the sum of squares of the Euclidian distance for all pairs of the empirical and modeled data (Fig. 1) 10,11.
As the AIC tends to select models with a larger number of parameters when the sample size is small, bias-corrected AIC (cAIC) was used 12. The cAIC values for each model are calculated as follows:
$$\text{c}\text{A}\text{I}\text{C} \text{v}\text{a}\text{l}\text{u}\text{e}=-2 \times \left(MLL\right)+ 2 \times DOF+ \frac{2DOF\left(DOF+1\right)}{N-DOF-1}, (\text{E}\text{q}.1)$$
where MLL, N, and DOF indicate the maximized logarithmic likelihood, the number of reflective markers placed on the lower extremity (i.e., twenty-six in this study), and the DOF for each model, respectively. The MLL is calculated as follows:
$$MLL=-\frac{1}{2{\sigma }^{2}}\sum _{i=1}^{N}{\left({\text{P}\text{E}}_{i}\right)}^{2}- \frac{N}{2}log2\pi {\sigma }^{2}, (\text{E}\text{q}.2)$$
where PE denotes the distance for a pair of the empirical and modeled data, and \({\sigma }^{2}\) denotes the variance of the PEs. The frame in which the sum of the PEs for M1 reached its maximum during the stride was used to calculate the MLL for each model. As the cAIC value decreases with increasing MLL (i.e., goodness-of-fit of the model) and decreasing number of DOFs (i.e., complexity of the model), the model with the smallest cAIC value is considered the best model, assuming that the goodness-of-fit and simplicity are better balanced than those of the other models.
Statistical analysis
A two-way repeated-measures ANOVA with two factors—model (9-, 18-, and 22-DOF models) and condition (walking and running)—was used to examine the main and interaction effects on the cAIC and MLL values. When the sphericity assumption was violated, the Greenhouse–Geisser correction was applied. A Bonferroni’s post hoc multiple comparison test was performed if a significant main effect was observed. Indices of effect size (Hedge’s g for pairwise comparisons, partial eta squared \({{\eta }_{p}}^{2}\) for ANOVA) were reported with p-values. A significance level of p < 0.05 was used for all comparisons. Statistical analyses were performed using IBM SPSS Statistics for Windows, version 23 (IBM Corporation, Armonk, NY, USA).