Difference between revisions of "Cyclotron motion"
Jump to navigation
Jump to search
| Line 1: | Line 1: | ||
{{Def2| | {{Def2| | ||
Circular motion of a charged particle moving at velocity '''v''' in a magnetic field '''B''' that results from the force q'''v'''×'''B'''.}} | Circular motion of a charged particle moving at velocity '''v''' in a magnetic field '''B''' that results from the force q'''v'''×'''B'''.}} | ||
| + | |||
| + | {{Rev5| | ||
| + | Circular motion of a particle of charge q moving at velocity v in a [[magnetic flux densit]]y B that results from the [[Lorentz force]]. | ||
| + | | | ||
| + | #A. G. Marshall, C. L. Hendrickson, G. S. Jackson. Mass Spectrom. Rev. 17, 1 (1988). | ||
| + | }} | ||
{{asms| | {{asms| | ||
Revision as of 01:07, 12 April 2010
Obsolete Template
This template is no longer used.
External links
- Cyclotron
- A device that uses alternating electric fields to accelerate subatomic particles (a particle smaller than an atom, such as an alpha particle or a proton). When these particles strike ordinary nuclei, radioisotopes are formed. For his work in developing the cyclotron in the early 1930s, Ernest Lawrence of the University of California received the 1939 Nobel Prize in Physics.