Moment of inertia
Moment of inertia ([math]\displaystyle{ I }[/math]), also called "angular mass" (kg·m2),[1] is a body's resistance to angular acceleration or deceleration, equal to the product of the mass and the square of its radius measured perpendicularly to the axis of rotation.
Moments of inertia for a few objects
Moment Of Inertia Media
Tightrope walkers use the moment of inertia of a long rod for balance as they walk the rope. Samuel Dixon crossing the Niagara River in 1890.
Video of rotating chair experiment, illustrating moment of inertia. When the spinning professor pulls his arms, his moment of inertia decreases; to conserve angular momentum, his angular velocity increases.
Pendulums used in Mendenhall gravimeter apparatus, from 1897 scientific journal. The portable gravimeter developed in 1890 by Thomas C. Mendenhall provided the most accurate relative measurements of the local gravitational field of the Earth.
A 1920s John Deere tractor with the spoked flywheel on the engine. The large moment of inertia of the flywheel smooths the operation of the tractor.
Related pages
References
- ↑ Atkinson, P.. Feedback Control Theory for Engineers (2012)Springer Science & Business Media. p. 50. ISBN 978-1-4684-7453-4.
Other websites
- Angular momentum and rigid-body rotation in two and three dimensions Archived 2010-03-29 at the Wayback Machine
- A table of moments of inertia Archived 2008-07-01 at the Wayback Machine
- Parallels between rotation and translation HyperPhysics