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Cyclotron resonance : ウィキペディア英語版
Cyclotron resonance
Cyclotron resonance describes the interaction of external forces with charged particles experiencing a magnetic field, thus already moving on a circular path. It is named after the cyclotron, a cyclic particle accelerator that utilizes an oscillating electric field tuned to this resonance to add kinetic energy to charged particles.
The ''cyclotron frequency'' or ''gyrofrequency'' is the frequency of a charged particle moving perpendicular to the direction of a uniform magnetic field ''B'' (constant magnitude and direction). Since that motion is always circular,〔Physics by M. Alonso & E. Finn, Addison Wesley 1996.〕 the cyclotron frequency is given by equality of centripetal force and magnetic Lorentz force
:\frac = qBv
with the particle mass ''m'', its charge ''q'', velocity ''v'', and the circular path radius ''r'', also called gyroradius.
By substitution for the circulation frequency f = \frac which defines the cyclotron frequency, this leads to
:f = \frac,
or the angular frequency
:\omega = 2 \pi f = \frac.
It is notable that the cyclotron frequency is independent of the radius and velocity and therefore independent of the particle's energy.
== See also ==

* Ion cyclotron resonance
* Electron cyclotron resonance
* (Calculate Cyclotron frequency with Wolfram Alpha )

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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