yusohard
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Homework Statement
A charge q is released from rest at the origin, in the presence of a uniform electric
field and a uniform magnetic field \underline{E} = E_0 \hat{z} and \underline{B} = B_0 \hat{x} in frame S.
In another frame S', moving with velocity along the y-axis with respect to S, the electric field is zero.
What must be the velocity v and the magnetic field in the frame S' ?
Show that the particle moves in S' in a circle of radius R=m\gamma^2 v / (q B_0) What are the equations in x', y', z, t' which describe the trajectory of the particle in the moving frame S' ?
By transforming from frame S’ show that the path of the particle in the original frame S is:
\gamma^2 (y-vt)^2 + (z-R)^2 = R^2
Homework Equations
Transformations of electric and magnetic fields for boosts in y-direction:
E'_x = \gamma (E_x + \beta c B_z)
E'_y = E_y
E'_z = \gamma (E_z - \beta c B_x)
B'_x = \gamma (B_x - (\beta / c) E_z )
B'_y = B_y
B'_z = \gamma (B_z + (\beta / c) E_x )
Lorentz Force:
\underline{F} = m \gamma \frac{d v}{d x} = m \gamma \frac{v^2}{R} = q \underline{B} \times \underline{v}
The Attempt at a Solution
Only the E field in the z-axis exists and, as stated in the problem, is zero:
E'_z = \gamma (E_0 - \beta c B_0) = 0 \rightarrow v=E_0/B_0
And similarly only the B field in the x-axis has a solution, and using the equation for v above:
B'_x = \gamma (B_0 - (\beta / c) E_0 ) = \gamma B_0 (1 - E^2_0/c^2 B^2_0 ) = B_0 / \gamma
Using the Lorentz force equation above:
m \gamma \frac{v^2}{R} = q B_0/\gamma \rightarrow R=m\gamma^2 v / (q B_0)
Now i doubt how to write equations in x', y', z, t' which describe the trajectory of the particle in the moving frame S'.
I think it should be:
(y'^2 + z'^2) = R^2
As it is in the yz-plane(right?)
If i transform back with y' = \gamma (y - vt) and z'=z I just get:
\gamma^2 (y - vt)^2 + z^2 = R^2
Missing the (z-R)^2 term.
Can anyone see where I've gone wrong or what I've missing?
Any help appreciated. Been driving me crazy.
Thanks in advance!