Difference between revisions of "Forest UCM PnCP"

From New IAC Wiki
Jump to navigation Jump to search
Line 18: Line 18:
  
  
:<math>\vec{F} = m \vec{a} = q \vec{v} \times \vec{B} =  \left ( ˆiˆjˆkvxvy000B
\right )</math>  
+
:<math>\vec{F} = m \vec{a} = q \vec{v} \times \vec{B} =  \left ( \begin{matrix} \hat i  & \hat j & \hat k \\ v_x  & v_y &0 \\ 0 &0 & B  \end{matrix} \right )</math>  
  
  
 
[[Forest_Ugrad_ClassicalMechanics]]
 
[[Forest_Ugrad_ClassicalMechanics]]

Revision as of 12:07, 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.

v=vxˆi+vyˆj
B=Bˆk


Lorentz Force
F=qE+qv×B
Note
the work done by a magnetic field is zero if the particle's kinetic energy (mass and velocity) don't change.
W=ΔK.E.

No work is done on a charged particle force to move in a fixed circular orbit by a magnetic field (cyclotron)


F=ma=qv×B=(ˆiˆjˆkvxvy000B)


Forest_Ugrad_ClassicalMechanics