Force of one distribution of charge on another

AI Thread Summary
The discussion revolves around calculating the total force exerted by a uniformly charged ring on a segment of uniformly distributed positive charges along its axis. The initial approach involved determining the electric field at a point on the segment and integrating to find the force. A key correction was made regarding the direction of the force, emphasizing the need to account for the cosine component due to the geometry of the setup. The final expression for the force incorporates this correction, leading to a more accurate calculation. The conversation highlights the importance of considering symmetry and the correct components when dealing with electric fields and forces.
archaic
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Homework Statement


I need help on solving this exercise :
We have a ring of radius = ##a## uniformly charged (total charge = ##Q##) and on its axis a segment ##OA## (length = ##a## also) of uniformly distributed positive electric charges with the charge density ##\lambda'## and of total charge = ##Q## (the same as the ring).

Zwcu3.png


I'm asked to determine the total force ##\vec{F}## that the ring's distribution is exerting on the segment's distribution.

Homework Equations


##\vec{F}=q.\vec{E}##

The Attempt at a Solution


First of all we have, for a point ##M## of ##OA## :
##\vec{F}_{Ring/M}=k\frac{Q.\lambda'dz}{a^2+z^2}\vec{u_z}## with ##k\frac{Q}{a^2+z^2}\vec{u_z}=## the electric field created at ##M##.
##\Rightarrow \vec{F}_{Ring/OA} = kQ\lambda'\int_0^a \frac{dz}{a^2+z^2}\vec{u_z} = kQ\lambda'\frac{\pi}{4a}\vec{u_z}##
Where have I gone wrong?
Thank you!
 

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I believe that the result must have the following shape
$$\mathrm{Const}\cdot\int_0^\pi \int_0^a\frac{zdzd\varphi}{(z^2+a^2)^{3/2}}$$
where ##\varphi## is the angle on the circle
 
archaic said:
Where have I gone wrong?
You need just the component of the field in the z direction.
 
haruspex said:
You need just the component of the field in the z direction.
So multiply by a cosine? But shouldn't that be already taken into account since we're given the charge of the ring? I mean we're supposing that each point of the ring is creating a force.
 
archaic said:
So multiply by a cosine? But shouldn't that be already taken into account since we're given the charge of the ring? I mean we're supposing that each point of the ring is creating a force.
But what direction is the force from a small element of the ring? Is it along the z axis?
 
haruspex said:
But what direction is the force from a small element of the ring? Is it along the z axis?
Yes, considering symmetries
 
archaic said:
Yes, considering symmetries
No, that's the overall result. What are the magnitude and direction of the force from a small element of the ring? What component of that is along the z axis?
 
haruspex said:
No, that's the overall result. What are the magnitude and direction of the force from a small element of the ring? What component of that is along the z axis?
That would be ##\vec{F}=k\frac{dq_{ring}.dq_M}{a^2+z^2}cos\theta .\vec{u_z}##
 
Well the force of the whole ring on a point M would be $$\vec{F}_{Ring/M}=k\frac{Q.\lambda'dz}{a^2+z^2}\cos{\theta}.\vec{u_z}$$ then substitute the cosine with ##\frac{z}{\sqrt{a^2+z^2}}## and so $$\vec{F}_{Ring/OA} = kQ\lambda'\int_0^a \frac{z.dz}{(a^2+z^2)^{3/2}}\vec{u_z}$$
I guess that's it, thank you!
 
  • #10
What made me rethink using the cosine here is the fact that we're given the total charge of the ring, in my mind I was literally picturing myself looking from "a charge on the ring" point of view and I was imagining lines from all the other charges, as well as the one I'm looking from, moving towards a point M and naturally the electric field at that point was in the ##\vec{u_z}## direction, so I thought maybe we ought to directly express the field as ##E=k\frac{Q}{a^2+z^2}\vec{u_z}##
 
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