Antisymmetry of the electromagnetic field tensor

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SUMMARY

The discussion focuses on the antisymmetry of the electromagnetic field tensor, specifically the exercise involving the differentiation of the tensor components with respect to momentum variables ##p_\alpha## and ##p_\beta##. Participants emphasize that the tensor ##F^{\mu\nu}## can be expressed as a sum of symmetric and antisymmetric components, leading to the conclusion that only the antisymmetric components remain after contraction with the symmetric tensor ##p_\mu p_\nu##. The hint regarding ignoring the constraint ##p^\alpha p_\alpha = m^2c^2## is clarified as a means to simplify the problem, allowing for a focus on the antisymmetric nature of the tensor.

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  • Understanding of tensor calculus, specifically electromagnetic field tensors.
  • Familiarity with the concepts of symmetric and antisymmetric tensors.
  • Knowledge of differentiation techniques in the context of physics.
  • Basic understanding of the implications of the mass-energy equivalence principle, ##E=mc^2##.
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Students and professionals in theoretical physics, particularly those focusing on electromagnetism and tensor analysis, will benefit from this discussion. It is also valuable for anyone seeking to deepen their understanding of the mathematical foundations of physics.

shinobi20
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Homework Statement
Show that the electromagnetic field tensor is antisymmetric from the fact that ##p_\mu p_\nu F^{\mu \nu} = 0##.
Relevant Equations
##p_\mu p_\nu F^{\mu \nu} = 0##
where ##p_\mu## is the 4-momentum and ##F^{\mu \nu}## is the EM field tensor
1.png

I am trying to answer exercise 5 but I am not sure I understand what the hint is implying, differentiate with respect to ##p_\alpha## and ##p_\beta##, I have done this but nothing is clicking. Also, what is the relevance of the hint "the constraint ##p^\alpha p_\alpha = m^2c^2## can be ignored ..."? Please help me clarify what the author wants me to think or do in accordance to the hint.
 
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##p_\mu p_\nu## is a symmetric tensor.
 
try writing F^{\mu\nu} as a sum of symmetric and anti symmetric pieces then do the contraction with the p^\alpha to show that the components cancel.

or try writing F^{\mu\nu} using its definition in terms of A^\mu and \partial^\nu
 
Dr Transport said:
try writing F^{\mu\nu} as a sum of symmetric and anti symmetric pieces then do the contraction with the p^\alpha to show that the components cancel.

or try writing F^{\mu\nu} using its definition in terms of A^\mu and \partial^\nu

I cannot figure out what you want me to do, but then I want to follow the hint given in OP.

My attempt, differentiating with respect to ##p_\alpha## and ##p_\beta##,

##\delta^\mu_\alpha p_\nu F^{\mu\nu} + p_\mu \delta^\nu_\alpha F^{\mu\nu} = 0 \quad \rightarrow \quad p_\nu F^{\alpha\nu} + p_\mu F^{\mu\alpha} = 0##

##\delta^\mu_\beta p_\nu F^{\mu\nu} + p_\mu \delta^\nu_\beta F^{\mu\nu} = 0 \quad \rightarrow \quad p_\nu F^{\beta\nu} + p_\mu F^{\mu\beta} = 0##

Multiplying both sides of the first equation by ##p^\mu##

##p^\mu p_\nu F^{\alpha\nu} + m^2 c^2 F^{\mu\alpha} = 0##

Multiplying both sides of the second equation by ##p^\nu##

##m^2 c^2 F^{\beta\nu} + p^\nu p_\mu F^{\mu\beta} = 0##

From these last two equations, I think there are only a few steps before I get the answer, but I cannot see it.

**I may be wrong by multiplying ##p^\nu## in the second equation, maybe it should also be ##p^\mu##, but the flow is as above.
 
(Further to post #2)
p_\mu p_\nu F^{\mu \nu}=p_\mu p_\nu (S^{\mu \nu}+A^{\mu \nu})
where S is symmetric and A is anti-symmetric components of F.
Contract of symmetric tensor, here ##p_\mu p_\nu##, and anti-symmetric tensor, here ##A^{\mu \nu}##, is always zero.
p_\mu p_\nu A^{\mu \nu}=0
This and
p_\mu p_\nu F^{\mu \nu}=0
give
p_\mu p_\nu S^{\mu \nu}=0
S^{\mu \nu}=0
So ##F^{\mu \nu}## has only anti-symmetric components.
 
shinobi20 said:
I cannot figure out what you want me to do, but then I want to follow the hint given in OP.

My attempt, differentiating with respect to ##p_\alpha## and ##p_\beta##,

##\delta^\mu_\alpha p_\nu F^{\mu\nu} + p_\mu \delta^\nu_\alpha F^{\mu\nu} = 0 \quad \rightarrow \quad p_\nu F^{\alpha\nu} + p_\mu F^{\mu\alpha} = 0##
Try differentiating this result with respect to ##p_\beta##.
 
vela said:
Try differentiating this result with respect to ##p_\beta##.
😑😑😑
I don't consider myself stupid, but there are some days where I think I am one. It is like having a snake in front of me but still don't notice it. The hint given in OP is very clear, you just restated what it said but in a different way.

What is your advice on this? Is this just a physics thing that can be improved within physics? o_O
 
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shinobi20 said:
😑😑😑
I don't consider myself stupid, but there are some days where I think I am one. It is like having a snake in front of me but still don't notice it. The hint given in OP is very clear, you just restated what it said but in a different way.

What is your advice on this? Is this just a physics thing that can be improved within physics? o_O
I think everyone has had moments like these, and then we feel like idiots for not seeing what's right in front of us. The best advice I can give is to be aware of the possibility of tunnel vision so you can break out of a rut sooner rather than later.
 
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