The lengths of the pendulums are adjusted so that their oscillation completes an integer number of cycles in 60 seconds. For small angles, the angular frequency and length are related by the approximate formula , but this Demonstration uses the exact relation , where denotes the elliptic integral of the first kind and numerical solutions are found for the classic pendulum differential equation .

Once set in motion, the pendulums quickly fall out of sync. But after 60 seconds (neglecting friction and air resistance), they have all undergone an integral number of cycles and return to their starting configuration. Another interesting configuration occurs at 30 seconds, when the pendulums are at alternating maximum phases. The states at 12, 15, 20, 24, 36, 40, 45, and 48 seconds also show some organization. The oscillations can be observed from the front, side, or top.

You can also choose to view a plot of all the pendulum angles against time. This shows the sinusoidal paths of the individual pendulums, color coded to match the corresponding pendulum balls. Note how the chaotic motion becomes ordered at certain times.