Our stimulus consisted of a soccer ball (radius = 0.11 m) moving frontally along the three dimensions on parabolic trajectories. The ball was frontally and vertically aligned with the observer’s eye level at the beginning of each trial to account for posture changes during the experiment.
Flying time was set to 3 s for five out of six trials. However, in order to prevent observers from developing rhythmic responses, a second flight time of 3.5 s was randomly interleaved in a proportion of one out of six trials.
We explored the 10 different trajectories shown in
Figure 1A corresponding with a combination of five different initial positions in depth (
\(\text{Z}_{\text{init}}\) = [23.49, 24.23, 25.16, 26.24, 27.47] m) and two flight times (see inset within
Figure 1A). Each initial distance corresponds with a lateral final position relative to the observer (
\(\text{X}_{\text{end}}\) = [15.09, 12.53, 10.06, 7.71, 5.53] m either
left or
right) and depth position (
\(\text{Z}_{\text{end}}\) = [−4.53, −5.01, −5.03, −4.63, −3.87] m) both with a final height at eye level. Each trajectory was tailored to predict perfect accuracy by the GS model at different temporal moments corresponding to a [30, 40, 50, 60, 70] % of the flight time elapsed, that is, [0.9, 1.2, 1.5, 1.8, 2.1] s and [1.05, 1.4, 1.75, 2.1, 2.45] s for trajectories of 3 and 3.5 s of flight time, respectively.
A detailed scene was stereoscopically displayed providing cues for relative distance, retinal size (
\(\theta\)), and cardinal motion angles (horizontal:
\(\beta _{\text{ball}}\); vertical:
\(\gamma _{\text{ball}}\)). Note that from now on, we will use
\(\beta _{\text{ball}}\) and
\(\gamma _{\text{ball}}\) to denote the ball’s angular position in the horizontal and vertical axes with respect to the observer and ball’s initial position. See
Figure 3 for a combined representation of the ball’s angular position and gaze direction.
Figure 4 represents
\(\beta _{\text{ball}}\) and
\(\gamma _{\text{ball}}\) across time in our experimental trajectories. Note that horizontal angles larger than 90 degrees indicate that the ball is behind the observer under the initial frame of reference, assuming that the observer does not rotate. Gravitational acceleration was set at 1
g (
\(9.807\;\text{m}/\text{s}^2\), the standard at sea level). Complex dynamic effects such as air resistance and Magnus effects were neglected. Therefore, horizontal and depth movement remained constant during the same trial. No embedded rotation was simulated.