About the derivation of Lorentz gauge condition

In summary, the Lorentz condition ∂µAµ = 0 can be expressed as d* A = 0, where A is the four-potential and * is the Hodge star, and d is the exterior differentiation. The Lorentz gauge potential is different from the actual Lorentz condition due to a sign difference. The indices should be "upstairs" in this case and the name should be corrected to Lorenz instead of Lorentz.
  • #1
QuantumRose
11
1
The question:
Show that the Lorentz condition ∂µAµ =0 is expressed as d∗ A =0.
Where A is the four-potential and * is the Hodge star, d is the exterior differentiation.


In four-dimensional space, we know that the Hodge star of one-forms are the followings.
0c95a67c2cdabbfc965b8475ec01a96f4bce3af9


3. My attempt
Since the four potential one-form is
png.png

Therefore we have
png.png

Then d*A = 0 is equivalent of saying
png.png
(Where
png.png
)

However, the actual Lorentz gauge potential is
png.png
(Where
png.png
)

I don't know why there is a sign difference?
 

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  • #2
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  • #3
George Jones said:
Aren't the indices "upstairs", here?
Opps, such a silly mistake... thank you!
 
  • #4
The correct name is Lorenz, not Lorentz. Please, tell that to your instructor, too.
 

1. What is the Lorentz gauge condition?

The Lorentz gauge condition is a mathematical constraint used in the theory of electromagnetism to describe the behavior of electric and magnetic fields. It is based on the principle of gauge invariance, which states that the equations used to describe physical phenomena should not change under a certain mathematical transformation. In the case of the Lorentz gauge condition, this transformation is a gauge transformation that ensures the equations are consistent with the principles of special relativity.

2. How is the Lorentz gauge condition derived?

The Lorentz gauge condition is derived by applying the principle of gauge invariance to the equations of electromagnetism, specifically Maxwell's equations. This involves making a mathematical transformation to the equations that ensures they are consistent with the principles of special relativity. The resulting equations are then simplified to arrive at the Lorentz gauge condition.

3. What is the physical significance of the Lorentz gauge condition?

The Lorentz gauge condition has physical significance because it is a mathematical constraint that ensures the equations of electromagnetism are consistent with the principles of special relativity. This means that the equations accurately describe the behavior of electric and magnetic fields in the context of moving observers and reference frames.

4. How does the Lorentz gauge condition affect the behavior of electric and magnetic fields?

The Lorentz gauge condition has no direct effect on the behavior of electric and magnetic fields. Instead, it is a constraint on the equations used to describe their behavior. The resulting equations, which include the Lorentz gauge condition, accurately describe the behavior of electric and magnetic fields in the context of moving observers and reference frames.

5. What are the implications of violating the Lorentz gauge condition?

If the Lorentz gauge condition is violated, it means that the equations used to describe the behavior of electric and magnetic fields are not consistent with the principles of special relativity. This could lead to incorrect predictions and interpretations of experimental results. Therefore, it is important to use the Lorentz gauge condition in the appropriate context to ensure accurate and consistent results.

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