Electrostatic force between a Half Cylinder and a Plate

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SUMMARY

The discussion centers on calculating the electrostatic force between a half cylinder and a dielectric plate, specifically using a half cylinder of radius R and length L, with charges Q and q uniformly distributed. The derived formula for the force is F = (qQ)/(8ε₀RL), with an alternative approach suggesting F = σΦ, where Φ is the flux through the plate. The total flux from the half cylinder is Φ_tot = Q/ε₀, and it is proposed that Φ = (1/4)Φ_tot passes through the plate. The problem originates from the book 'Advanced Problems in School Physics' by Cengage Publication.

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Terry Bing
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Homework Statement


(This is not a HW problem, but HW-type problem.)
A half cylinder of radius R and length L>>R is formed by cutting a cylindrical pipe made of an insulating material along a plane containing its axis. The rectangular base of the half cylinder is closed by a dielectric plate of length L and width 2R. A charge Q on the half cylinder and a charge q on the dielectric plate are uniformly sprinkled. Find the electrostatic force between the half cylinder and the dielectric plate.

Homework Equations


Flux through a closed surface S enclosing a charge q_{enc} is
\oint_S \vec{E} \cdot \vec{dA} \ =\frac{q_{enc}}{\epsilon _0}
Force \vec{dF} on a charged surface carrying a surface charge density \sigma due to an electric field \vec{E} is
\vec{dF}=\sigma \vec{E} dA, where dA is the area element (scalar, not vector).

The Attempt at a Solution


Brute force integration gave me
F=\frac{qQ}{8\epsilon_0 R L}
Since this problem is from a high school textbook, I think brute force double integration \int_S \vec{dF} is not the expected solution. So I tried the following:
For the flat plate which has uniform charge distribution,
\int_S \vec{dF}=\int_S\sigma \vec{E} dA
By symmetry of the problem, we know that resultant force will be normal to the plate. Hence we pick the normal component of \vec{E}. Let the magnitude of the net force be F
\lvert \int_S \vec{dF} \rvert=\sigma \int_SE_\perp dA
\implies F=\sigma \int_S \vec{E} \cdot \vec{dA}
\implies F=\sigma \, \Phi
where \Phi is the flux due to the half cylinder through the plate.
\implies F=\frac{q}{2RL} \, \Phi

Now, total flux emerging from the half cylinder is
\Phi_{tot} =\frac{Q}{\epsilon _0}
Out of this if \Phi=\frac{1}{4}\Phi_{tot} =\frac{Q}{4 \epsilon _0} passes through the plate, then we are done. But I don't see how I can show this.
Any help would be appreciated.
 
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Terry Bing said:
I don't see how I can show this.
What angle does the plate subtend at a point on the half pipe?
 
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haruspex said:
What angle does the plate subtend at a point on the half pipe?
Depends on the point we choose. For eg at a point adjacent to the plate it subtends zero angle.
The farthest point does subtend pi/2. If that was true for all points, then great. But that,s not true for all points, is it?
 
Terry Bing said:
Depends on the point we choose. For eg at a point adjacent to the plate it subtends zero angle.
No. The plate occupies a diameter of the half pipe. What angle does a diameter of a circle subtend at its circumference?
 
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haruspex said:
No. The plate occupies a diameter of the half pipe. What angle does a diameter of a circle subtend at its circumference?
Awesome! Thanks.
I was considering the extreme case of a point on the edge of the half pipe, on which the plate seems to subtend zero angle. I guess as a limit, it would still subtend pi/2.
 
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Terry Bing said:
Awesome! Thanks.
I was considering the extreme case of a point on the edge of the half pipe, on which the plate seems to subtend zero angle. I guess as a limit, it would still subtend pi/2.
Right.
 
What a nice problem!

@Terry Bing, This is from a high-school text? Interesting! Do you mind giving the title and author of the text?
 
TSny said:
What a nice problem!

@Terry Bing, This is from a high-school text? Interesting! Do you mind giving the title and author of the text?
Sorry, not a text, a problem book. 'Advanced Problems in school physics', by cengage publication. I think it is out of publication. Problems compiled by indian authors , I think mostly physics olympiad problems.
 
Terry Bing said:
Sorry, not a text, a problem book. 'Advanced Problems in school physics', by cengage publication. I think it is out of publication. Problems compiled by indian authors , I think mostly physics olympiad problems.
OK. Thank you.
 
  • #10
quite simple unitary method, 4pi angle enclosed means Q/Eo. Therefore, pi angle enclosed here which means Q/4Eo
 
  • #11
Terry Bing said:

Homework Statement


(This is not a HW problem, but HW-type problem.)
A half cylinder of radius R and length L>>R is formed by cutting a cylindrical pipe made of an insulating material along a plane containing its axis. The rectangular base of the half cylinder is closed by a dielectric plate of length L and width 2R. A charge Q on the half cylinder and a charge q on the dielectric plate are uniformly sprinkled. Find the electrostatic force between the half cylinder and the dielectric plate.

Homework Equations


Flux through a closed surface S enclosing a charge qenc is
∮SE→⋅dA→ =qencϵ0
Force dF→ on a charged surface carrying a surface charge density σ due to an electric field E→ is
dF→=σE→dA, where dA is the area element (scalar, not vector).

The Attempt at a Solution


Brute force integration gave me
F=qQ8ϵ0RL
Since this problem is from a high school textbook, I think brute force double integration ∫SdF→ is not the expected solution. So I tried the following:
For the flat plate which has uniform charge distribution,
∫SdF→=∫SσE→dA
By symmetry of the problem, we know that resultant force will be normal to the plate. Hence we pick the normal component of E→. Let the magnitude of the net force be F
|∫SdF→|=σ∫SE⊥dA
⟹F=σ∫SE→⋅dA→
⟹F=σΦ
where Φ is the flux due to the half cylinder through the plate.
⟹F=q2RLΦ

Now, total flux emerging from the half cylinder is
Φtot=Qϵ0
Out of this if Φ=14Φtot=Q4ϵ0 passes through the plate, then we are done. But I don't see how I can show this.
Any help would be appreciated.

 

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