Difference between revisions of "Forest UCM PnCP"
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:<math>\dot{v}_y = - \omega v_x</math> | :<math>\dot{v}_y = - \omega v_x</math> | ||
− | + | ==determine the velocity as a function of time== | |
let | let | ||
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:<math>\Rightarrow</math> | :<math>\Rightarrow</math> | ||
::<math>v^* = Ae^{-i\omega t}</math> | ::<math>v^* = Ae^{-i\omega t}</math> | ||
+ | |||
+ | the complex variable solution may be written in terms of <math>\sin</math> and <math>\cos</math> | ||
+ | |||
+ | :<math>v_x +i v_y = A \left ( \cos(\omega t) - i \sin ( \omega t) \right )</math> | ||
+ | |||
+ | |||
+ | ==Determine the position as a function of time== | ||
http://hep.physics.wayne.edu/~harr/courses/5200/f07/lecture10.htm | http://hep.physics.wayne.edu/~harr/courses/5200/f07/lecture10.htm |
Revision as of 11:25, 27 August 2014
Charged Particle in uniform B-Field
Consider a charged particle moving the x-y plane in the presence of a uniform magnetic field with field lines in the z-dierection.
- Lorentz Force
- Note
- the work done by a magnetic field is zero if the particle's kinetic energy (mass and velocity) don't change.
No work is done on a charged particle force to move in a fixed circular orbit by a magnetic field (cyclotron)
Apply Newton's 2nd Law
- Motion in the z-direction has no acceleration and therefor constant (zero) velocity.
- Motion in the x-y plane is circular
Let
- = fundamental cyclotron frequency
Then we have two coupled equations
determine the velocity as a function of time
let
- = complex variable used to change variables
the complex variable solution may be written in terms of
and
Determine the position as a function of time
http://hep.physics.wayne.edu/~harr/courses/5200/f07/lecture10.htm
http://www.physics.sfsu.edu/~lea/courses/grad/motion.PDF
http://physics.ucsd.edu/students/courses/summer2009/session1/physics2b/CH29.pdf
http://cnx.org/contents/77faa148-866e-4e96-8d6e-1858487a520f@9