Stick Pendulum Via Lagrangian Mechanics by Frank Owen, 23 May 2014 © All Rights Reserved

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Stick Pendulum Via Lagrangian Mechanics by Frank Owen, 23 May 2014 © All Rights Reserved

Alpha Omega Engineering, Inc. 872 Toro Street, San Luis Obispo, CA 93401 – (805) 541 8608 (home office), (805) 441 3995 (cell) Stick pendulum via Lagrangian mechanics by Frank Owen, 23 May 2014 © All rights reserved Note: The following development follows from other developments shown for pendula via Lagrange mechanics to be found at www.aoengr.com/Dynamics. Unlike the simple pendulum, which consists of a massless link holding a point mass without any resistance to rotation, a stick pendulum is a link of length l with mass m and a rotational inertia about its mass center of Figure 1 shows a stick pendulum. Figure 1 – Stick pendulum Lagrangian formulation For the Lagrangian formulation we need expressions for the kinetic energy T and the potential energy U of the pendulum. The kinetic energy consists of the movement of the pendulum’s mass center and also the rotational energy of the stick itself. ̇ 1 The mass center moves with a speed ̇ Thus ̇ ̇ ̇ The potential energy is purely gravitational and is similar to that of the simple pendulum except that the mass center only rises half as much as it does for a mass mounted at the pendulum end. Thus it is half that of a simple pendulum. ( ) where y is the distance of the mass center above its lowest position at = 0. Thus the Lagrangian is ̇ ( ) Like the simple pendulum there is just one equation of motion, where q1 = . The Lagrange formulation is ( ) ̇ Now let’s get the parts and pieces from the Lagrangian. ̇ ̇ Taking the time derivative of this ( ) ̈ ̇ Then Putting these parts together, we get the equation of motion. ( ) ̈ ̇ ̈ 2 Or ̈ 3 .

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