You are viewing an old version of this page. View the current version.

Compare with Current View Page History

« Previous Version 33 Next »

Unknown macro: {table}
Unknown macro: {tr}
Unknown macro: {td}
Error formatting macro: live-template: java.lang.NullPointerException
Unknown macro: {td}

Description and Assumptions

This model is [generally applicable], but mathematically very complicated. In introductory mechanics it will only be used to describe the motion of a gyroscope.

Problem Cues

Only used in problems involving a gyroscope.


Page Contents

Prerequisite Knowledge

Prior Models

Vocabulary

  • [torque (one-dimensional)]
  • [angular momentum (one-dimensional)]

Compatible Systems

Technically, any number of rigid bodies. In practice, only used in analyzing gyroscopes (single rigid body with a fixed pivot point).

Relevant Interactions

Only external torques need be considered. Internal torques do not change the system's angular momentum.

Model

Definitions

Gyroscopic Approximation


Unknown macro: {latex}

\begin

Unknown macro: {large}

[ \vec

Unknown macro: {L}

\approx \vec

Unknown macro: {omega}

I]\end

(I is the moment of inertia of the gyroscope about the spin axis

Unknown macro: {latex}

$\hat

Unknown macro: {omega}

$

)


Angular Frequency of Gyroscopic Precession


Unknown macro: {latex}

\begin

Unknown macro: {large}

[\displaystyle \Omega = \frac{\displaystyle \left(\frac

Unknown macro: {dL}
Unknown macro: {dt}

\right)}

Unknown macro: {L}

]\end

Law of Change

Differential Form


Unknown macro: {latex}

\begin

Unknown macro: {large}

[\sum_

Unknown macro: {rm system}

\frac{d\vec{L}}

Unknown macro: {dt}

= \sum_

Unknown macro: {rm external}

\vec

Unknown macro: {tau}

]\end


Diagrammatic Representations

Relevant Examples

None yet.


Unknown macro: {search-box}



Error formatting macro: live-template: java.lang.NullPointerException
  • No labels