Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Lorentz force
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
== Trajectories of particles due to the Lorentz force == {{Main|Guiding center}} [[File:charged-particle-drifts.svg|upright=1.4|thumbnail|right|Charged particle drifts in a homogeneous magnetic field. (A) No disturbing force. (B) With an electric field, {{math|'''E'''}}. (C) With an independent force, {{math|'''F'''}} (e.g. gravity). (D) In an inhomogeneous magnetic field, {{math|grad '''H'''}}.]] In many cases of practical interest, the motion in a [[magnetic field]] of an [[electric charge|electrically charged]] particle (such as an [[electron]] or [[ion]] in a [[Plasma (physics)|plasma]]) can be treated as the [[Quantum superposition|superposition]] of a relatively fast circular motion around a point called the '''guiding center''' and a relatively slow '''drift''' of this point. The drift speeds may differ for various species depending on their charge states, masses, or temperatures, possibly resulting in electric currents or chemical separation.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)