Difference between revisions of "Cyclotron motion"

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{{Def2|
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{{Final
Circular motion of a charged particle moving at velocity '''v''' in a magnetic field '''B''' that results from the force q'''v'''×'''B'''.}}
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|acronym=
 
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|def=Circular motion of a charged particle moving perpendicularly to the direction of a magnetic field that results from the [[wikipedia:Lorentz force|Lorentz force]]
== External links ==
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|ref=A. G. Marshall, C. L. Hendrickson, G. S. Jackson. Mass Spectrom. Rev. 17, 1 (1998). (http://dx.doi.org/10.1002/(SICI)1098-2787(1998)17:1%3C1::AID-MAS1%3E3.0.CO;2-K )
*[http://www.eh.doe.gov/ohre/roadmap/achre/glossary.html ACHRE Report Glossary]
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:'''[[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.
 
 
 
 
 
*[http://nobelprize.org/physics/laureates/1939/index.html E.O. Lawrence 1939 Nobel Prize in Physics]
 
 
 
*[http://education.jlab.org/glossary/cyclotron.html Jefferson Lab: Cyclotron]
 
 
 
*[http://en.wikipedia.org/wiki/Cyclotron Wikipedia:  Cyclotron]
 
 
 
  
 
[[Category:M/z Separation]]
 
[[Category:M/z Separation]]
{{DEFAULTSORT:Cyclotron Motion}}
 

Latest revision as of 19:54, 25 October 2013

IUPAC RECOMMENDATIONS 2013
Cyclotron motion
Circular motion of a charged particle moving perpendicularly to the direction of a magnetic field that results from the Lorentz force
Related Term(s):
Reference(s):

A. G. Marshall, C. L. Hendrickson, G. S. Jackson. Mass Spectrom. Rev. 17, 1 (1998). (http://dx.doi.org/10.1002/(SICI)1098-2787(1998)17:1%3C1::AID-MAS1%3E3.0.CO;2-K )

From Definitions of Terms Relating to Mass Spectrometry (IUPAC Recommendations 2013); DOI: 10.1351/PAC-REC-06-04-06 © IUPAC 2013.

Index of Recommended Terms