Difference between revisions of "Forest UCM PnCP"
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(Created page with " Forest_Ugrad_ClassicalMechanics") |
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+ | =Charged Particle in uniform B-Field= | ||
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+ | Consider a charged particle moving the x-y plane in the presence of a uniform magnetic field with field lines in the z-dierection. | ||
+ | |||
+ | :\vec{v} = v_x \hat i + v_y \hat j | ||
+ | :\vec{B} = B \hat k | ||
+ | |||
+ | |||
+ | ;Lorentz Force | ||
+ | |||
+ | :\vec{F} = q \vec{E}q\vec{v} \times \vec{B} | ||
+ | |||
+ | ;Note: the work done by a magnetic field is zero if the particle's kinetic energy (mass and velocity) don't change. | ||
+ | :W = \Delta K.E. | ||
+ | |||
+ | No work is done on a charged particle force to move in a fixed circular orbit by a magnetic field (cyclotron) | ||
[[Forest_Ugrad_ClassicalMechanics]] | [[Forest_Ugrad_ClassicalMechanics]] |
Revision as of 11:57, 25 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.
- \vec{v} = v_x \hat i + v_y \hat j
- \vec{B} = B \hat k
- Lorentz Force
- \vec{F} = q \vec{E}q\vec{v} \times \vec{B}
- Note
- the work done by a magnetic field is zero if the particle's kinetic energy (mass and velocity) don't change.
- W = \Delta K.E.
No work is done on a charged particle force to move in a fixed circular orbit by a magnetic field (cyclotron)