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2 votes
1 answer
74 views

How to derive $\partial^{\nu}F^{\mu\alpha} + \partial^{\alpha}F^{\nu\mu} + \partial^{\mu}F^{\alpha\nu}=0$ for the Electromagnetic field tensor? [closed]

The problem says to show that $$\partial_{[\mu}F_{\alpha\nu]}=F^{\mu\alpha, \nu} + F^{\nu\mu,\alpha} + F^{\alpha\nu,\mu}=0$$ stems from Maxwell equations. I haven't been able to find this anywhere on ...
TiredStudent's user avatar
4 votes
2 answers
578 views

Maxwell's equations with differential form formalism

I've been reading Sean Carroll's book on GR and I stumbled upon an exercise on EM using $p$-forms. I think I've solved the problem correctly but I am having problems with my answers. I'll provide the ...
user20046481's user avatar
2 votes
1 answer
189 views

Dot product of the electric and magnetic field as the contraction of the electromagnetic tensor and its dual

I've see in some examples, e.g. here, that $$-4i\vec{E}\cdot \vec{B}=\tilde{F}_{\mu\nu}F^{\mu\nu}$$ How would you show such a relation? By inserting terms by terms inside this equation I've seen it is ...
Salmon's user avatar
  • 941
1 vote
0 answers
54 views

Rewriting Maxwell Lagrangian [duplicate]

I'm having some problems with rewriting the Maxwell Lagrangian. The text states, \begin{align}\mathcal{L}&=-\dfrac{1}{4}F_{\mu\nu}F^{\mu\nu}-A_\mu J^\mu \\ &= -\dfrac{1}{2}(\partial_\mu A_\nu)^...
SMYK's user avatar
  • 11
2 votes
2 answers
2k views

Expressing Maxwell's equations in tensor form using Electromagnetic field strength tensor [closed]

I have yet another derivation question from Carroll's General Relativity textbook. Given the electromagnetic field strength tensor is of the form: $$ F_{\mu\upsilon} = \left( \begin{matrix} 0 & -...
Chidi 's user avatar
  • 187
2 votes
1 answer
1k views

Expressing Maxwell's equations in tensor notation

I've been teaching myself relativity by reading Sean Carroll's intro to General Relativity textbook, and in the first chapter he discusses special relativity and introduces the concept of tensors, ...
Chidi 's user avatar
  • 187
0 votes
2 answers
48 views

Index manipulation in Lorentz scalars

I have been trying to show that: $ \vec{B}^{2} - \vec{E}^{2} =\frac{1}{2} f^{\mu \nu }f_{\mu \nu}$ where $\vec{B}^{2}$ and $\vec{E}^{2}$ are the square of the magnitude of the magnetic field and ...
JFCastello's user avatar
-1 votes
1 answer
45 views

Tensor algebra identity [closed]

In our course we took the following formula: $$F^\mu{}_\lambda\partial_{\mu}F^{\lambda \nu}=\frac 1 2 F_{\mu \lambda}\partial^{\mu}F^{\lambda \nu} + \frac 1 2F_{\lambda \mu}\partial^{\lambda}F^{\mu \...
imbAF's user avatar
  • 1,398
0 votes
0 answers
88 views

How compute the expression of electromagnetic tensor explicitly as given here?

I am trying to understand how the second line arrives at the last line of this expression. For $F_{\mu\nu} = \partial_\mu A_\nu -\partial_\nu A_\mu$ And $F^{\mu\nu} = \partial^\mu A^\nu -\partial^\nu ...
Han's user avatar
  • 13
2 votes
0 answers
65 views

Starting with 1-form potential $A$, derive the relation $F_{\mu\nu}^{\nu}=A_{\nu,\mu}^{,\nu}-A_{\mu,\nu}^{,\nu}=4\pi J_\mu$ [closed]

First the problem in detail should be, "Starting with 1-form potential $\mathbf{A}$, derive the relation $F_{\mu\nu}^{\;\;\;,\nu}=A_{\nu,\mu}^{\;\;\;\;,\nu}-A_{\mu,\nu}^{\;\;\;\;,\nu}=4\pi J_\mu$...
Arafat Hossen's user avatar
2 votes
2 answers
106 views

Integration of tensor to find potential

I have question given as: $$\partial_k \varphi = -(C_k+ D_{jk}r_j)$$ where $C_k \,\&\, D_{jk}$ are constants and $D_{jk}$ is symmetric and traceless. I have to find $\varphi$. I am getting : $\...
shubham-sinha's user avatar
0 votes
1 answer
217 views

Problem 2.1(b) in Peskin and Schroeder's Introduction to QFT

In this exercise the author claims that adding $\partial_\sigma K^{\sigma \mu \nu}$ does not affect the divergence of $T^{\mu\nu}$. In other words the author claims that $\partial_\mu \partial_\sigma ...
user avatar
0 votes
1 answer
70 views

The variation of the Lagrangian density for the canonical energy-momentum tensor

I expanded the Lagrangian to this form $$ \mathcal{L} = -{1 \over 4} F^{\mu \nu} F_{\mu \nu} = ... = - {1 \over 2} (\partial^{\mu} A^{\nu} \partial_{\mu} A_{\nu} - \partial^{\mu} A^{\nu} \partial_{\nu}...
Chakalaka's user avatar
3 votes
3 answers
2k views

Simple derivation of the Maxwell's equations from the Electromagnetic Tensor

Lets start by considering the electromagnetic tensor $F^{\mu \nu}$: $$F^{\mu \nu}=\begin{bmatrix}0 & -E_x/c & -E_y/c & -E_z/c \\ E_x/c & 0 & -B_z & B_y \\ E_y/c & B_z & ...
Noumeno's user avatar
  • 4,577
2 votes
2 answers
446 views

How can we do this tensor product $F_{\mu \nu}F^{\mu \nu}$?

Iam Studying "Quantization of the electromagnetic field using Quantum Field Theory" by Lahiri and Pal. But I don't get how they computed action in equation $8.23$. $$A=-{1\over 4} \int d^4xF_{\mu \...
ROBIN RAJ's user avatar
  • 545

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