Search

Loading [MathJax]/jax/output/HTML-CSS/jax.js

Filter Results
Location
- Campus Bookshelves (2)
Classification
- Article type
  - Book or Unit
  - Chapter
  - Section or Page
  - N/A
  - N/A
- Author
  - Jeremy Tatum
  - Lloyd Knox
  - OpenStax
  - Ben Crowell
  - Michael Fowler
  - Paul D'Alessandris
  - Malcolm McMillian
  - Jeffrey W. Schnick
  - Dina Zhabinskaya
  - Chris Impey
  - Douglas Cline
  - Paul Seeburger
  - Tom Weideman
  - Niels Walet
  - David Harrison
  - Boundless
  - Richard Fitzpatrick
  - Fred Jendrzejewski, Selim Jochim, & Matthias Weidemüller
  - Timon Idema
  - Lawrence Davis
  - Daniel Arovas
  - Daniel F. Styer
  - Ryan Martin et al.
  - UCD Physics 7 sans Dina
  - Julio Gea-Banacloche
  - John F. Cochran and Bretislav Heinrich
  - Daniel E. Barth
  - Lei Ma
  - Steven W. Ellingson
  - Michael Richmond
  - David H. Staelin
  - Johan Wevers
  - Peter Dourmashkin
  - Kyle Forinash and Wolfgang Christian
  - Jack C. Straton
  - Graeme Ackland
  - Paola Cappellaro
  - Kim Coble, Kevin McLin, Janelle Bailey, Anne Metevier, Carolyn Peruta, & Lynn Cominsky
  - László Tisza
  - Wolfgang Christian, Mario Belloni, Anne Cox, Melissa H. Dancy, and Aaron Titus, & Thomas M. Colbert
  - David J. Raymond
  - V. Parameswaran Nair
  - Howard Georgi
  - Y. D. Chong
  - Konstantin K. Likharev
  - Evan Halstead
  - Walter Fendt
  - Mihály Benedict
  - Pieter Kok
  - Sander Konijnenberg, Aurèle J.L. Adam, & H. Paul Urbach
  - Edwin F. Taylor & John Archibald Wheeler
  - James M. Fiore
  - Rob Knop
  - Ryan D. Martin, Emma Neary, Joshua Rinaldo, and Olivia Woodman
  - Ronald Kumon
  - Lumen Learning
  - Debra Fischer, Allyson Sheffield, Joshua Tan, and Lily Ling Zhao
- Embed Hypothes.is?
  - yes
- Embebbed CalcPlot3D?
  - yes
- Cover Page
  - yes
  - TOC Only
  - Compile but don't publish
- License
  - Public Domain
  - CC BY
  - CC BY-SA
  - CC BY-NC-SA
  - CC BY-ND
  - CC BY-NC-ND
  - GNU GPL
  - All Rights Reserved
  - CC BY-NC
  - GNU FDL
- Show TOC
  - yes
  - no
- Transcluded
  - yes
- OER program or Publisher
  - College of the Canyons - Zero Textbook Cost Program
  - ASCCC OERI Program
  - CK-12
  - OpenStax
  - GALILEO
  - OpenSUNY
  - MIT OpenCourseWare
  - Virginia Tech Libraries' Open Education Initiative
  - The Publisher Who Must Not Be Named
  - eCampusOntario
  - WAC Clearinghouse
  - BC Campus
  - Lumen
  - Open Oregon
  - OpenStax CNX
  - PDXOpen
  - Evergreen Valley College
- Student Analytics
  - yes
- Autonumber Section Headings
  - title with space delimiters
  - title with colon delimiters
  - title with dash delimiters
- License Version
  - 1.0
  - 2.0
  - 2.5
  - 3.0
  - 4.0
- Print CSS
- Screen CSS
  - default
  - Virginia Tech
  - Cosmology
- PrintOptions
  - No Header/Footer
  - No Title
  - No Header/Footer/Title
Include attachments
- Content Type
  - Document
  - Image
  - Other

7.8: Magnetic Force on a Current-Carrying Conductor
https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Introductory_Physics_II_(1112)/07%3A_Magnetism/7.08%3A_Magnetic_Force_on_a_Current-Carrying_Conductor
We can derive an expression for the magnetic force on a current by taking a sum of the magnetic forces on individual charges. (The forces add because they are in the same direction.) The force on an i...We can derive an expression for the magnetic force on a current by taking a sum of the magnetic forces on individual charges. (The forces add because they are in the same direction.) The force on an individual charge moving at the drift velocity $v_{d}$ is given by $F = qv_{d}B\sin \theta$ .
9.6: Magnetic Force on a Current-Carrying Conductor
https://phys.libretexts.org/Courses/Skyline/Survey_of_Physics/09%3A_Magnetism/9.06%3A_Magnetic_Force_on_a_Current-Carrying_Conductor
The magnetic force on current-carrying conductors is given by $F = \pi B sin \theta,$ where is the current, $l$ is the length of a straight conductor in a uniform magnetic field $B$ , and \...The magnetic force on current-carrying conductors is given by $F = \pi B sin \theta,$ where is the current, $l$ is the length of a straight conductor in a uniform magnetic field $B$ , and $\theta$ is the angle between $I$ and $B$ . The force follows RHR-1 with the thumb in the direction of $I$ .\

Search

Text Color

Text Size

Margin Size

Font Type

Support Center

How can we help?