How can divF=0, but the volume integral of divF=/=0

Click For Summary
The discussion revolves around a divergence theorem problem where the divergence of a vector field \(\vec{F} = \nabla \frac{1}{r}\) is calculated to be zero, yet the volume integral of this divergence yields a non-zero result. The confusion arises because the vector field is not defined at the origin, violating the theorem's requirement for a continuously differentiable field in a neighborhood of the volume. Participants suggest that the Dirac delta function may provide insight into this discrepancy, particularly in relation to point charges in electrostatics. After further exploration, one participant realizes a calculation error in the right-hand side of the equation, impacting their understanding. The conversation emphasizes the importance of recognizing singularities in vector fields when applying the divergence theorem.
FaraDazed
Messages
347
Reaction score
2

Homework Statement


Basically, this is part C of a question where in part A we had to use the RHS of the divergence theorem below to calculate the LHS, and then in part B we had to calculate the divergene of F, which came to be 0. and part C asks us how can this be? Since in part A we used the LHS and shown that it does not equal 0.

For reference, although I doubt it matters, this was for a sphere centered at the origin, and \vec{F}=\nabla \frac{1}{r}

I had no issues calculating divF or the RHS but just cannot get my head around how divF equals 0, yet the volume integral of divF does not.

Homework Equations


<br /> \int \int \int_V \nabla \cdot \vec{F} dV =\int \int_S \vec{F} \cdot d \vec{S}<br />

The Attempt at a Solution


I had no issues calculating divF or the RHS but just cannot get my head around how divF equals 0, yet the volume integral of divF does not.

Is it simply because \vec{F}=\nabla \frac{1}{r} and so is not defined at (0,0,0) ? I have tried searching google and cannot find much. I am not sure if this post is in the right place, it does refer to a coursework question, but there's no math involved in this question.

Any help is much appreciated.
 
Physics news on Phys.org
Perhaps it would be more informative if you posted all parts of this problem you are working on. Right now, you have access to more information than we do.
 
Yes, that's pretty much it. The theorem only holds when you have a continuously differentiable vector field ##\vec{F}## defined on a neighborhood of ##V##. The vector field here isn't defined at ##\vec{r} = 0##, so it doesn't meet the requirements of the theorem.
 
vela said:
Yes, that's pretty much it. The theorem only holds when you have a continuously differentiable vector field ##\vec{F}## defined on a neighborhood of ##V##. The vector field here isn't defined at ##\vec{r} = 0##, so it doesn't meet the requirements of the theorem.
Right, I thought that was it. But because the RHS (in this case) equals 4 \pi R^4 is it mathmatically correct to say that \int \int \int_v \nabla \cdot \vec{F} dV = 4 \pi R^4 also? As that is what the question is essentially asking, that how can it be that the volume integral equals 4 \pi R^4 when \nabla \cdot \vec{F} = 0

Thanks!
 
Have you learned about the Dirac delta function?
 
vela said:
Have you learned about the Dirac delta function?

No not yet, I think he is covering something what he called "The Delta Function" on Tuesday. Maybe I should wait until then and then maybe I will get it?
 
Just a hint: Think about the Coulomb field of a point charge sitting in the origin of your coordinate system!
 
vela said:
Have you learned about the Dirac delta function?

We ended up covering the delta function yesterday and it was explained to us. I calculated the RHS wrong anyway as I had a silly exponent mistake with the R's, they canceled out and the answer was -4 \pi . I had actually met the delta function last year, but it was only very briefly and only covered it in one dimension.
 

Similar threads

  • · Replies 12 ·
Replies
12
Views
2K
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K