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Double pendulum
From Wikipedia, the free encyclopedia
In horology, a double pendulum is a system of two simple pendulums on a common mounting which move in anti-phase.
In mathematics, in the area of dynamical systems, a double pendulum is a pendulum with another pendulum attached to its end, and is a simple physical system that exhibits rich dynamic behavior. The motion of a double pendulum is governed by a set of coupled ordinary differential equations. Above a certain energy its motion is chaotic. Also see pendulum (mathematics).
The double pendulum consists of two thin rods (moment of inertia, 
) connected by a pivot and the end of one rod suspended from a pivot. It is natural to define the coordinates to be the angle between each rod and the vertical. These are denoted by θ1 and θ2. The position of the centre of mass of the two rods may be written in terms of these coordinates. If the origin of the Cartesian coordinate system is assumed to be at the point of contact of the wall and the first pendulum, then the centre of mass is located at:
and
This is enough information to write out the Lagrangian.
The Lagrangian is given by
where the first term is the kinetic energy of the bodies, the second term is the kinetic energy of the center of mass of each rod, and the last term is the potential energy of the bodies in a uniform gravitational field.
Plugging in the coordinates above and doing a bit of algebra gives
![L = \frac{1}{6} m \ell^2 \left [ {\dot \theta_2}^2 + 4 {\dot \theta_1}^2 + 3 {\dot \theta_1} {\dot \theta_2} \cos (\theta_1-\theta_2) \right ] + \frac{1}{2} m g \ell \left ( 3 \cos \theta_1 + \cos \theta_2 \right ).](../../../math/8/1/8/818a9a6d0e001cf64b3f05aedd29fe97.png)
There is only one conserved quantity (the energy), and no conserved momenta. The two momenta may be written as
![p_{\theta_1} = \frac{\partial L}{\partial {\dot \theta_1}} = \frac{1}{6} m \ell^2 \left [ 8 {\dot \theta_1} + 3 {\dot \theta_2} \cos (\theta_1-\theta_2) \right ]](../../../math/5/d/2/5d2ce3773944fc8800e86b10d97cdb87.png)
and
![p_{\theta_2} = \frac{\partial L}{\partial {\dot \theta_2}} = \frac{1}{6} m \ell^2 \left [ 2 {\dot \theta_2} + 3 {\dot \theta_1} \cos (\theta_1-\theta_2) \right ].](../../../math/6/7/4/6745f6cfa73911f28f6525b38aa1ef63.png)
These expressions may be inverted to get
and
The remaining equations of motion are written as
![{\dot p_{\theta_1}} = \frac{\partial L}{\partial \theta_1} = -\frac{1}{2} m \ell^2 \left [ {\dot \theta_1} {\dot \theta_2} \sin (\theta_1-\theta_2) + 3 \frac{g}{\ell} \sin \theta_1 \right ]](../../../math/d/f/5/df57a7c7102f358e6c77b9a85df778b1.png)
and
![{\dot p_{\theta_2}} = \frac{\partial L}{\partial \theta_2} = -\frac{1}{2} m \ell^2 \left [ -{\dot \theta_1} {\dot \theta_2} \sin (\theta_1-\theta_2) + \frac{g}{\ell} \sin \theta_2 \right ].](../../../math/7/f/2/7f2414e33d60ca9bb057b81e6099a77b.png)
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 100 (red), 1000 (purple) or 10000 (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:
Within the region defined by this curve, that is if
then it is energetically impossible for either pendulum to flip. Outside this region, the pendulums can flip but this is different from determining when they will flip.
- Eric W. Weisstein, Double pendulum (2005), ScienceWorld. (Contains details of the complicated equations involved.)
- Peter Lynch, Double Pendulum, (2001). (Java applet simulation.)
- Northwestern University, Double Pendulum, (Java applet simulation.)
- Theoretical High-Energy Astrophysics Group at UBC, Double pendulum, (2005).
- Meirovitch, Leonard (1986). Elements of Vibration Analysis, 2nd edition, McGraw-Hill Science/Engineering/Math. ISBN 0-07-041342-8.