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But let's actually do the calculations for this completely different scenario anyways. In the rest frame, we have no magnetic field, and an electric field vertical. To use your equations, we need the direction y to be vertical (positive up), sideways is x (positive right), and out of the page z. These equations were written with the assumption that positive v is to the right, but that's the velocity of the moving frame relative to the rest frame. You've actually got the frame moving to the left, so keep in mind that v is negative.
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OK, but what if the electron is already moving? Then you've got a vertical component of velocity, when you cross that with the B field you should get a sideways component for the force. Doesn't that make the electron deflect to the side?
No, it doesn't. And this is where things get really weird. If the electron is moving vertically, then in the moving frame its momentum is at an angle. And one of the weird aspects of special relativistic mechanics is that because momentum isn't linear with velocity anymore, the direction of any VELOCITY change doesn't need to be parallel to the direction of MOMENTUM change. Basically, to keep the electron moving to the right at the same velocity as it picks up speed vertically, we actually need to add momentum to the right as well. And how do we get that extra momentum to the right to maintain rightward velocity? From your magnetic field.
Thanks for this post!
Right, after the electric field is turned on and the electrons accelerate upwards, there is an electron velocity in the Y, Y' direction.
Where is the force pointing out from this upward velocity and the magnetic field?
Have you heard about spin orbit interaction?
This is where the relativity failed. It did not predict/expect spin orbit interaction.
The experiments/observations prove the drift is there.
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