Lorentz boost to obtain parallel E and B fields?

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SUMMARY

This discussion focuses on determining the conditions under which a Lorentz transformation can yield parallel electric (\vec{E}) and magnetic (\vec{B}) fields in different inertial frames. The equations governing the transformation of these fields under a Lorentz boost along the x_1-direction are provided, specifically detailing how the components of \vec{E} and \vec{B} change. The key insight is that the scalar quantity F_{\rho \sigma}\tilde{F}^{\rho\sigma} = -4 \vec{B}\cdot \vec{E} remains invariant across frames, indicating that if \vec{E} is parallel to \vec{B} in one frame, they cannot be orthogonal in any other frame. The discussion emphasizes the importance of finding the appropriate Lorentz boost to achieve this configuration.

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Xavier1900
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Homework Statement


Suppose given an electric field \vec{E} and a magnetic field \vec{B} in some inertial frame. Determine the conditions under which there exists a Lorentz transformation to another inertial frame in which \vec{E} || \vec{B}

Homework Equations


If we give a Lorentz boost along x_1-direction, then in the boosted frame, electric and magnetic fields are given by
E_1&#039; = E_1\\<br /> E_2&#039; = \gamma (E_2 - \beta B_3)\\<br /> E_3&#039; = \gamma (E_3 + \beta B_2)
And similar for components of B fields.

The Attempt at a Solution


I started with a frame in which the fields are parallel and see what kind of fields I can obtain after the transformation. The case where the boost is along the direction of E//B fields is trivial. Then I consider the case where I boost in the direction perpendicular to the E//B fields. By the equations I listed I find that I can produce E and B fields with some angle depending on \beta. But I am not seeing how I can go further from here. Am I in the right direction? Or should I try some other approach?
 
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One way to approach problems like these is to construct invariants - i.e quantities that are the same in all frames. For example, given a four-vector A, the quantity A^\mu A_\mu has the same value in all frames. It turns out there are two invariants that can be constructed from the electromagnetic field tensor F^{\mu \nu}, and hence from E and B. Try to discover what these are - this will help answer the question.
 
phyzguy said:
One way to approach problems like these is to construct invariants - i.e quantities that are the same in all frames. For example, given a four-vector A, the quantity A^\mu A_\mu has the same value in all frames. It turns out there are two invariants that can be constructed from the electromagnetic field tensor F^{\mu \nu}, and hence from E and B. Try to discover what these are - this will help answer the question.

Thanks for the hint. I realize that F_{\rho \sigma}\tilde{F}^{\rho\sigma} = -4 \vec{B}\cdot \vec{E}, which is a scalar. That means if E//B in one frame, \vec{E}\cdot \vec{B} \neq 0 in all frames. Thus I just need to find the right Lorentz boost for systems like that. I will try and see what I can find.
 

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