A full description of the parameters measured, as well as their statistical significance, can be found in
Table 1 and
Table 2. Statistically significant differences in performance emerged with the addition of all types of peripheral refractive errors.
For the lenses with spherical defocus, the total crossing time increased with respect to the plano lenses as the power of the superimposed error increased: +6.2%, +7.6%, +19.2%, and +29.6% for the −2 D, +2 D, −4 D, and +4 D lenses, respectively (P < 0.05 in all the cases, except the −2 D lens). Ascent and descent times followed the same trend, with ascent being more affected by superimposed peripheral errors: +2.3%, +4.7%, +8.4%, and +15.8% for the −2 D, +2 D, −4 D, and +4 D lenses, respectively (P < 0.05 for all cases, except the −2 D lens). The number of steps taken on the elevated platform also increased slightly with power, with some subjects taking up to two more steps.
When analyzing mean ascent and descent trajectories, a similar behavior can be observed for the trajectories with all the types of refractive error (even though cylindrical lenses exhibited a less pronounced change in performance): starting and landing positions, as well as maximum foot elevation were generally reduced with respect to the plano lens (
Fig. 4). Foot clearances slightly increased with the superimposed peripheral refractive error at ascent and decreased at descent. For ascent, the starting position was especially reduced in the case of −4 D lenses (−20.8% of reduction in distance,
P = 0.005). During descent, both −4 D and +4 D defocus lenses behaved similarly, being the change with respect to the plano lenses significant for the negative lenses (
P = 0.02). The position of the foot on the intermediate step was affected by the sign of the defocus: whereas the distance to the bottom of the step increased for high-power positive defocus lenses (+122.2%,
P = 0.02) it decreased for high-power negative defocus lenses (−50%,
P = 0.15). Performance differences were more subtle with low power lenses.
For the leading foot, the ascent to the elevated platform (second step) showed the greatest reduction in peak speed. The mean speed for both ascent and descent trajectories were also reduced by superimposing the peripheral errors (see
Table 1).
The parameters associated with the following foot were less affected by the superimposed peripheral errors (see
Table 2), as few statistically significant differences were found. Still, some differences in the placement of the following foot emerged depending on the type of superimposed peripheral error (
Fig. 5). Ascent and descent starting distances decreased (compared to the plano lenses) by −52.2% and −83.3% for −4 D of defocus, respectively, whereas for +4 D of defocus, the differences in starting distance decreased −2.5% at ascent and increased +233.3% at descent. That is, on average, the following foot was placed closer to the steps with negative lenses and further away with positive lenses.