Question about calculating electric field made by finite point charges

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SUMMARY

The discussion centers on calculating the electric field generated by finite point charges, specifically addressing the scenario where the observation point coincides with the location of one of the charges. The equation provided from "Introduction to Electrodynamics" is E(P) = (1/4πε₀)∑(qᵢ/rᵢ)âᵢ, where rᵢ represents the distance from each charge to point P. Participants conclude that at the location of a charge, the electric field becomes infinite, indicating that the electric field cannot be defined at that point. This leads to the understanding that Coulomb's law breaks down in such scenarios, necessitating consideration of other physical laws.

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  • Understanding of Coulomb's law and electric fields
  • Familiarity with point charge concepts in electrostatics
  • Basic knowledge of calculus, particularly integrals and singularities
  • Concept of electric field lines and their physical implications
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Homework Statement


Hi!
I have a question about calculating electric field made by finite point charges
q_{1},q_{2},..., q_{n}.
From the book "introduction to electrodynamics", you can see that the electric field E at a point P made by the finite point charges can be calculated by the below equation;
E(P) = \frac{1}{4\pi\epsilon_{0}}\sum^{n}_{i=1}\frac{q_{i}}{r_{i}}\hat{r_{i}} where r_{i}'s are the distances between a point charge and the point P.

I can see that above electric field makes sense if P is located at a different position from each point charge q_{i}.
However, what if P is located at one of those places at which the point charges are located? For example, what is the electric field at the position at which q_{1} is located?? As you can see, the electric field function has a singular point at the point, so that I think it is impossible to calculate it. Am I right?? Does it mean that the electric field doesn't exist at the point??



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The Attempt at a Solution

 
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Then you have an infinite electric field at that point :cry:

Really though, I don't think that this situation would be physically possible. The field is representative of the force that a charge would experience at a given location. Since that location is occupied, you can't put a charge there. At least that's my understanding.

I believe that if you put a charge infinitely close to another charge, the whole idea of coulombs law would break down, since now you are entering the domain of the nuclear force, and I am positive other laws apply.
 


QuarkCharmer said:
Then you have an infinite electric field at that point :cry:

Really though, I don't think that this situation would be physically possible. The field is representative of the force that a charge would experience at a given location. Since that location is occupied, you can't put a charge there. At least that's my understanding.

I believe that if you put a charge infinitely close to another charge, the whole idea of coulombs law would break down, since now you are entering the domain of the nuclear force, and I am positive other laws apply.

Thanks for your responding!

I actually asked you above one because of some equations.
I attach it here.
div.3.jpg

The divergence of E.jpg

Div.2.jpg


As you can check in the first equation, it represents the electric field at a point r occurred by continuously distributed electric charges.

Here's my question in the second picture...
It is said that because the charge density out of the electric charges is zero everywhere, the integral of the equation in the first picture can be extended over the whole space...
But, in this case, you can see that the integrand inevitably contains the singularity at r=r'. What does it mean? I can't understand the meaning of the integral;;
Furthermore, if r indicates a point within the volume of the distributed charges, it would be more complicating...
 

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