Gauss' Law -- How did he come up with it?

In summary, Gauss's law, which states that the flux Φ is equal to the net charge Qenc inside a gaussian surface, was developed through a combination of Faraday's experiment and Gauss's mathematical sophistication. To fully understand how Gauss came up with this law, one must have a deep understanding of Maxwell's equations and the divergence theorem. This was mostly a theoretical work and involved the use of the coulomb force equation and the concept of divergence.
  • #1
amjad-sh
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How did Gauss came out with his law εΦ=Qenc,where Φ is the flux and Qenc is the net charge inside the gaussian surface?Was it an experimental work or just a theoretical one? thanks.
 
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amjad-sh said:
How did Gauss came out with his law εΦ=Qenc,where Φ is the flux and Qenc is the net charge inside the gaussian surface?Was it an experimental work or just a theoretical one? thanks.

It is unclear how far back do you want to start here. First of all, do you know the differential form of Gauss's Law, which is one of the 4 equations that are collectively known at "Maxwell Equations"?

If you do, then do you know the Divergence Theorem that allows you to go from the differential form into the integral form?

Zz.
 
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  • #4
ZapperZ said:
It is unclear how far back do you want to start here. First of all, do you know the differential form of Gauss's Law, which is one of the 4 equations that are collectively known at "Maxwell Equations"?

If you do, then do you know the Divergence Theorem that allows you to go from the differential form into the integral form?
OK.Yes I know Maxwell's equations and the divergence theorem but i didn't go deep to them.I just know them.
So do you mean that to understand deeply how Guass makes his law I need to grasp Maxwell's equations and the divergence theorem? and it is mostly a theoretical work?
 
  • #5
One of the most important formulas you get out of electromagnetism is the coulomb force F = kQq/r^2 where k = 1/(4πε0), from that fact we define the electric field to be E = kQ/r^2, where you can notice the inverse square, 1/r^2 if you sketck the electric field R/r^3, it seems to be just divergent in any point but, when applying the formula of divergence, you'll be shocked that it's exactly zero, by the time the delta function was born it became widely known that this isn't quite true and ∇.(R/r^3) = δ3(r), r is the position, so ∇.E = 4πδ3(r)*kQ, by the definition of k ∇.E = Qδ3(r)/ε0, so ∫∫∫∇.EdV = ⊂∫∫⊃E.dS, this is the gauss's famous divergence theorem, ∫∫∫∇.E dV = Q/ε0*∫∫∫δ3(r)dV = Q/ε0*1, so the flux Φ = ⊂∫∫⊃E.dS = Q/ε0,Cheers
 
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1. What is Gauss' Law and why is it important?

Gauss' Law is a fundamental law in the study of electromagnetism that relates the electric flux through a closed surface to the charge enclosed within that surface. It is important because it allows us to find the electric field at any point in space and understand the behavior of electric charges and fields.

2. How did Gauss come up with this law?

Gauss' Law was first formulated by the German mathematician and physicist Carl Friedrich Gauss in the early 19th century. He developed the law based on his mathematical studies of electric and magnetic fields and their relationship to electric charges.

3. What is the mathematical equation for Gauss' Law?

The mathematical equation for Gauss' Law is ∮E⃗ · dA = Q/ε0, where E⃗ is the electric field, dA is the differential area element, Q is the enclosed charge, and ε0 is the permittivity of free space.

4. What are the applications of Gauss' Law?

Gauss' Law has many applications in various fields of science and engineering, including circuit analysis, electrostatics, and electromagnetic radiation. It is also fundamental in understanding the behavior of electric fields in conductors, insulators, and other materials.

5. Are there any limitations to Gauss' Law?

Like any scientific law, Gauss' Law has its limitations. It is only valid for static electric fields and does not account for changing magnetic fields. Additionally, it assumes that the electric field is continuous and differentiable, which may not always be the case in real-world scenarios.

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