Lorentz Invariants and Field Strength Tensor Fuv

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Homework Help Overview

The discussion revolves around the Lorentz invariance of quantities derived from the field strength tensor Fuv, specifically focusing on the expressions E² - c²B² and cE·B. Participants are tasked with expressing these quantities as invariant contractions using the tensors Fuv and εuvab.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the meaning of writing expressions as invariant contractions and discuss the requirements for Lorentz invariance, including the need for no free indices.
  • There is a focus on forming contractions from Fuv and εμνab, with some participants questioning the correctness of their expressions and seeking clarification on the relationships between E, B, and the components of Fuv.
  • Some participants attempt to relate the components of Fuv to the electric and magnetic fields, while others express uncertainty about their progress and the correctness of their formulations.

Discussion Status

The discussion is ongoing, with participants actively questioning their understanding and the validity of their approaches. Some have identified potential invariant expressions, while others are still grappling with the correct formulations. There is no explicit consensus, but guidance has been offered regarding the relationships between the quantities involved.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. There is a noted confusion regarding the proper use of indices and the definitions of the tensors involved.

jc09
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Homework Statement



The Field strength tensor Fuv encodes the electric and magnetic fields via:
Ei=-cF0i, Bi=-1/2 eijkFjk, i=1,2,3 Show that E^2-c^2B^2 and cE.B are invariant under lorentze transformations, by writing them explicitly as invariant contractions using the tensors Fuv and euvab

Homework Equations





The Attempt at a Solution


What does write the explicitly as invariant contractions mean?
 
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jc09 said:

The Attempt at a Solution


What does write the explicitly as invariant contractions mean?

A Lorentz invariant quantity can't have any free index. A quantity like A_{\mu\nu\rho}v^\mu}B^{\nu\rho} would be invariant, but A_{\mu\nu\rho}B^{\nu\rho} would not.
 
ok so for the first one E^2-c^2B^2 how would I start the problem. I know the equation for E and B are given in terms of the metric tensor so I would write them out but what would be the next step
 
Well what sort of contractions can you form from F^{\mu\nu} and \epsilon_{\mu\nu ab}? Note that the quantities you're supposed to obtain are quadratic in the fields.
 
I know I can contract FuvUb=Va but not sure how to proceed at all
 
jc09 said:
I know I can contract FuvUb=Va but not sure how to proceed at all

The expression you've written has free indices \mu, \nu and b on the LHS and an index a on the RHS, so it is incorrect. Also U and V are undefined and have nothing to do with the question. You do not need any other tensors other than F^{\mu\nu} and \epsilon_{\mu\nu ab}. Try to form contractions that have no free indices. For example, \epsilon_{\mu\nu ab} \epsilon^{\mu\nu ab} is a Lorentz invariant, but it's not one of the ones you're looking for.
 
so does euvxy=euvexy make more sense? are these correct? I know these are still not what I used in the question but is the idea right here. Then FuvFuv
 
jc09 said:
so does euvxy=euvexy make more sense? are these correct? I know these are still not what I used in the question but is the idea right here. Then FuvFuv

sorry that isn't right I think maybe this is euveuvexyexy
 
\epsilon^{\mu\nu a b} is the Levi-Civita symbol, you might want to brush up on what it means here: http://en.wikipedia.org/wiki/Levi-Civita_symbol You can't write \epsilon^{\mu\nu a b} =\epsilon_{\mu\nu} \epsilon_{ a b} for any definition of \epsilon_{\mu\nu}, the RHS does not have all of the symmetries that the LHS does.

I wrote the expression with 2 \epsilon's to illustrate a Lorentz-invariant combination, don't get hung up on trying to rewrite that. You mentioned F^{\mu\nu}F_{\mu\nu}. Why don't you try writing that in terms of E and B?
 
  • #10
hi so if I write FuvFuv in terms of E and B I get FuvFuv=FolFol+FijFij=cE.B is this correct?

Then to get the other one I can write 1/2euvxyFuvFxy in terms of E and B
 
  • #11
jc09 said:
hi so if I write FuvFuv in terms of E and B I get FuvFuv=FolFol+FijFij=cE.B is this correct?

No, that's not right. Remember that Ei=-cF0i, Bi=-1/2 eijkFjk, i=1,2,3.

Then to get the other one I can write 1/2euvxyFuvFxy in terms of E and B

That's one of the invariants that you need. You should see what expression that gives in terms of E and B.
 
  • #12
fzero said:
No, that's not right. Remember that Ei=-cF0i, Bi=-1/2 eijkFjk, i=1,2,3.



That's one of the invariants that you need. You should see what expression that gives in terms of E and B.

So for the first bit if I write FuvFuv=F0iF0i+FjkFjk is that better. sorry I'm having quite a lot of trouble with these
 
  • #13
jc09 said:
So for the first bit if I write FuvFuv=F0iF0i+FjkFjk is that better. sorry I'm having quite a lot of trouble with these

That part was fine, the part that was wrong was what you wrote for the E and B expression. You should use the relationships between E, B and the components of Fuv to explicitly compute that, don't just try to guess.
 
  • #14
so for F0iF0i does that equal -2/c E.B then to finish I add on the second part of it?
 
  • #15
ah wait sorry I see the error of my ways I had written down the second matrix wrong so I had B's where there were meant to be E's etc. Think I have the first one now.
 

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