Two general approaches were used by most of the students.
Approach A: Spread the students out every 10 meters or so. The students each start their stopwatches as the runner starts and measure the time for the runner to reach their positions.
Analysis variant 1: Make a position vs. time graph. Fit the parabolic and linear parts of the graph and establish the position and time at which the parabola makes the transition to the straight line.
Analysis variant 2: Use the position and time measurements to determine a series of average velocities (vavg = ∆x/∆t ) for the intervals. Graph these velocities vs. time to obtain a horizontal line and a line with positive slope. Establish the position and time at which the sloped and horizontal lines intersect.
Analysis variant 3: Use the position and time measurements to determine a series of average accelerations (∆x = v0t + 1/2at2). Graph these accelerations vs. time to obtain two horizontal lines, one with a nonzero value and one at zero acceleration. Establish the position and time at which the acceleration drops to zero.
Approach B: Concentrate the students at intervals at the end of the run, in order to get a very precise value of the constant speed vf, or at the beginning in order to get a precise value for a. The total distance D is given by a = ½ atu2 + vf(T – tu), where T is the total measured run time. In addition vf = atu These equations can be solved for a and tu(if vf is measured directly) or vf and tu(if a is measured directly). Students may have also defined and used distances, speeds, and times for the accelerated and constant-speed portions of the run in deriving these relationships.