Coplanar Double Pendulum

Tag: LnL_1.5.1

Source:

Textbook: Landau and Lifshitz, Mechanics, 3rd Edition

Chapter: 1 The Equations of motion

Section: 5 The Lagrangian for a system of particles

Problem: 1 Coplanar Double Pendulum

Description: This problem involves: a) identifying the appropriate Degrees of Freedom or generalized coordinates and their relation to cartesian coordinates

b) and using them to write down the Lagrangian for

a coplanar double pendulum made up of two point masses $m_1$ and $m_2$. Mass $m_1$ is attached to the pivot and $m_2$ is attached to $m_1$ via strings of length $l_1$ and $l_2$ respectively.

Solution:

The Cartesian coordinates $(x_1, y_1)$ for mass $m_1$ and $(x_2, y_2)$ for mass $m_2$ can be expressed in terms of the two angles $\phi_1$ and $\phi_2$ made by the strings with the vertical: $$ \begin{aligned} x_1 &= l_1\sin\phi_1\ y_1 &= -l_1\cos\phi_1\ x_2 &= l_1\sin\phi_1 + l_2\sin\phi_2\ y_2 &= -l_1\cos\phi_1 - l_2\cos\phi_2 \end{aligned} $$

b) The Lagrangian is obtained by writing down the kinetic and potential energies first in terms of cartesian coordinates and their time derivates and then substituting the coordinates and derivatives with transformations obtained in a) :

$$\mathcal{L} = T_1 + T_2 - V_1 - V_2$$ where $T$ denotes the kinetic energy and $V$ the potential energy $$ \begin{aligned} T_1 &= \tfrac{1}{2}m_1(\dot{x}_1^2 + \dot{y}_1^2) = \tfrac{1}{2}m_1 l_1^2\dot{\phi}_1^2\ V_1 &= m_1 g y_1 = -m_1 g l_1\cos\phi_1\ T_2 &= \tfrac{1}{2}m_2(\dot{x}_2^2 + \dot{y}_2^2) = \tfrac{1}{2}m_2\bigl(l_1^2\dot{\phi}_1^2 + l_2^2\dot{\phi}_2^2 + 2l_1 l_2\dot{\phi}_1\dot{\phi}_2\cos(\phi_1 - \phi_2)\bigr)\ V_2 &= m_2 g y_2 = -m_2 g\bigl(l_1\cos\phi_1 + l_2\cos\phi_2\bigr) \end{aligned} $$

so that the Lagrangian becomes: $$ \mathcal{L} = \tfrac{1}{2}(m_1 + m_2)l_1^2\dot{\phi}_1^2 + \tfrac{1}{2}m_2 l_2^2\dot{\phi}_2^2+ m_2 l_1 l_2\dot{\phi}_1\dot{\phi}_2\cos(\phi_1 - \phi_2)+ (m_1 + m_2)g l_1\cos\phi_1 + m_2 g l_2\cos\phi_2 $$

The configuration space of the coplaner double pendulum.