Double Pendulum - Chaotic Motion

Chaotic Motion

The double pendulum undergoes chaotic motion, and shows a sensitive dependence on initial conditions. The image to the right shows the amount of elapsed time before the pendulum "flips over," as a function of initial conditions. Here, the initial value of θ1 ranges along the x-direction, from −3 to 3. The initial value θ2 ranges along the y-direction, from −3 to 3. The colour of each pixel indicates whether either pendulum flips within (green), within (red), (purple) or (blue). Initial conditions that don't lead to a flip within are plotted white.

The boundary of the central white region is defined in part by energy conservation with the following curve:


3 \cos \theta_1 + \cos \theta_2 = 2. \,

Within the region defined by this curve, that is if


3 \cos \theta_1 + \cos \theta_2 > 2, \,

then it is energetically impossible for either pendulum to flip. Outside this region, the pendulum can flip, but it is a complex question to determine when it will flip.

The lack of a natural excitation frequency has led to the use of double pendulum systems in seismic resistance designs in buildings, where the building itself is the primary inverted pendulum, and a secondary mass is connected to complete the double pendulum.

Read more about this topic:  Double Pendulum

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