Euler's Equations (rigid Body Dynamics) | Euler Equations (rigid Body Dynamics)

Euler's Equations (rigid Body Dynamics)

This page discusses rigid body dynamics. For other uses, see Euler function (disambiguation).

In classical mechanics, Euler's equations describe the rotation of a rigid body, using a rotating reference frame with its axes fixed to the body and parallel to the body's principal axes of inertia. In cartesian components, they are:

$\begin{align} I_1\dot{\omega}_{1}+(I_3-I_2)\omega_2\omega_3 &= M_{1}\\ I_2\dot{\omega}_{2}+(I_1-I_3)\omega_3\omega_1 &= M_{2}\\ I_3\dot{\omega}_{3}+(I_2-I_1)\omega_1\omega_2 &= M_{3} \end{align}$

where M_k are the components of the applied torques M, I_k are the principal moments of inertia I and ω_k are the components of the angular velocity ω along the principal axes.

Read more about Euler's Equations (rigid Body Dynamics): Motivation and Derivation, Torque-free Solutions, Generalizations

Famous quotes containing the word body:

“I think that if most guys in America could somehow get their fave-rave poster girl in bed and have total license to do whatever they wanted with this legendary body for one afternoon, at least 75 percent of the guys in the country would elect to beat her up.”
—Lester Bangs (1948–1982)