Lorentz Transformations For Particle In Uniform Electromagnetic Field

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A charge q is released in a uniform electric field E and magnetic field B, with the electric field being zero in a moving frame S'. The velocity v of the moving frame is determined to be E_0/B_0, and the magnetic field in S' is found to be B'_x = B_0 / γ. The particle's motion in S' is circular, with a radius R given by R = mγ²v / (qB_0). The trajectory equations in the moving frame are derived, confirming that the path in the original frame follows the equation γ²(y - vt)² + (z - R)² = R². The problem is successfully solved, providing clarity on the particle's motion in both frames.
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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!
 
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Solved it.

For those interested:

It is indeed going in a circle in the zy-plane in S'. Since it starts at the origin in S' and goes clockwise, the equations of motion in terms of x', y', z' ,t' are:

x'=0
y'=-R Sin(\omega t')
z'=R(1-Cos(\omega t'))
Where \omega = v/R

Transform via usual lorentz transforms for boosts in y-axis:

t'=\gamma (t - \frac{v}{c^2} y)
y=\gamma (y' + v t')

Subbing in for the primed parameters in and following through etc,etc,etc,etc,etc,etc:

y= vt - \frac{R}{\gamma} Sin(\omega \gamma (t - \frac{v}{c^2}y))
z= R(1- \gamma R Cos(\omega \gamma (t - \frac{v}{c^2}y))

Using your favourite trig formula (no prizes for that one), we can see indeed:

\gamma^2(y-vt)^2 + (z-R)^2 = R^2

As required. I'll sleep easy tonight eh.
 

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