Set-theoretic limit: Difference between revisions
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{{about|the rotation of an object around a single axis (a one-dimensional rotation)|the kinetic energy of an object that rotates in three dimensions|rigid rotor}} | |||
The '''rotational energy''' or '''angular kinetic energy''' is the [[kinetic energy]] due to the rotation of an object and is part of its [[Kinetic energy#Rotation in systems|total kinetic energy]]. Looking at rotational energy separately around an object's [[axis of rotation]], one gets the following dependence on the object's [[moment of inertia]]: | |||
:<math>E_\mathrm{rotational} = \frac{1}{2} I \omega^2 </math> | |||
where | |||
: <math> \omega \ </math> is the [[angular velocity]] | |||
: <math> I \ </math> is the [[moment of inertia]] around the axis of rotation | |||
: <math> E \ </math> is the [[kinetic energy]] | |||
The [[mechanical work]] required for / applied during rotation is the torque times the rotation angle. The instantaneous [[power (physics)|power]] of an angularly accelerating body is the torque times the angular velocity. For free-floating (unattached) objects, the axis of rotation is commonly around its [[center of mass]]. | |||
Note the close relationship between the result for rotational energy and the energy held by linear (or translational) motion: | |||
:<math>E_\mathrm{translational} = \frac{1}{2} m v^2 </math> | |||
In the rotating system, the [[moment of inertia]], ''I'', takes the role of the mass, ''m'', and the [[angular velocity]], <math> \omega </math>, takes the role of the linear velocity, ''v''. The ''rotational energy'' of a [[wheel|rolling]] [[cylinder (geometry)|cylinder]] varies from one half of the translational energy (if it is massive) to the same as the translational energy (if it is hollow). | |||
As an example, let us calculate the rotational kinetic energy of the Earth. As the Earth has a period of about 23.93 hours, it has an angular velocity of 7.29×10<sup>−5</sup> rad/s. The Earth has a moment of inertia, I = 8.04×10<sup>37</sup> kg·m<sup>2</sup>.<ref>[http://scienceworld.wolfram.com/physics/MomentofInertiaEarth.html Moment of inertia--Earth], Wolfram</ref> Therefore, it has a rotational kinetic energy of 2.138×10<sup>29</sup> J. | |||
Part of it can be tapped using [[tidal power]]. Additional friction of the two global tidal waves creates energy in a physical manner, infinitesimally slowing down Earth's angular velocity ''ω''. Due to [[Angular momentum#Conservation of angular momentum|conservation]] of [[angular momentum]] this process transfers angular momentum to the [[Moon]]'s [[orbit]]al motion, increasing its distance from Earth and its orbital period (see [[tidal locking]] for a more detailed explanation of this process). | |||
==See also== | |||
*[[Flywheel]] | |||
*[[List of energy storage projects]] | |||
*[[Rigid rotor]] | |||
*[[Rotational spectroscopy]] | |||
==References== | |||
{{reflist}} | |||
{{Footer energy}} | |||
{{DEFAULTSORT:Rotational Energy}} | |||
[[Category:Forms of energy]] | |||
[[Category:Rotation]] |
Revision as of 02:42, 7 March 2013
29 yr old Orthopaedic Surgeon Grippo from Saint-Paul, spends time with interests including model railways, top property developers in singapore developers in singapore and dolls. Finished a cruise ship experience that included passing by Runic Stones and Church.
The rotational energy or angular kinetic energy is the kinetic energy due to the rotation of an object and is part of its total kinetic energy. Looking at rotational energy separately around an object's axis of rotation, one gets the following dependence on the object's moment of inertia:
where
- is the angular velocity
- is the moment of inertia around the axis of rotation
- is the kinetic energy
The mechanical work required for / applied during rotation is the torque times the rotation angle. The instantaneous power of an angularly accelerating body is the torque times the angular velocity. For free-floating (unattached) objects, the axis of rotation is commonly around its center of mass.
Note the close relationship between the result for rotational energy and the energy held by linear (or translational) motion:
In the rotating system, the moment of inertia, I, takes the role of the mass, m, and the angular velocity, , takes the role of the linear velocity, v. The rotational energy of a rolling cylinder varies from one half of the translational energy (if it is massive) to the same as the translational energy (if it is hollow).
As an example, let us calculate the rotational kinetic energy of the Earth. As the Earth has a period of about 23.93 hours, it has an angular velocity of 7.29×10−5 rad/s. The Earth has a moment of inertia, I = 8.04×1037 kg·m2.[1] Therefore, it has a rotational kinetic energy of 2.138×1029 J.
Part of it can be tapped using tidal power. Additional friction of the two global tidal waves creates energy in a physical manner, infinitesimally slowing down Earth's angular velocity ω. Due to conservation of angular momentum this process transfers angular momentum to the Moon's orbital motion, increasing its distance from Earth and its orbital period (see tidal locking for a more detailed explanation of this process).
See also
References
43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro. Template:Footer energy
- ↑ Moment of inertia--Earth, Wolfram