Calculating Flux through a Uniform Electric Field Penetrating a Cone

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The discussion centers on calculating the electric flux through a cone in a uniform electric field. The correct formula for the flux entering the cone is identified as EhR, which raises questions about the absence of pi in the textbook answer, as the surface area of the cone's face typically involves pi. Participants clarify that the relevant area for flux calculation is the projection of the cone's surface onto a plane normal to the electric field, which simplifies to a triangular area. The conversation also touches on the concept of flux in relation to Gauss's law, emphasizing that only the flux entering the cone is considered, despite the electric field exiting the other side. Further examples are requested to clarify the concept of flux through various surfaces like hemispheres and frustums.
kaotak
Source: Physics and Scientists for Engineers, Ch. 24 #7

A cone of radius R and height h sits on a horizontal table. A uniform electric field parallel to the table penetrates the surface of the cone. What is the flux entering the cone?

Diagram:
(N.B. the dots in the cone are just to give it shape)

E
-->.../.\
-->../...\
-->./...\ <---- cone
-->/____\___________ <- table

The back of the book gives an answer of flux_entering=EhR, which I don't get. I don't see why there isn't a pi in that answer, since the surface area of the face of the cone that's being penetrated certainly does have a pi in it.

My attempt at a solution yields flux_entering=pi*E*h*r/3. Hah, it's close... but not.

EDIT: The field is uniform, I forgot to mention that.
 
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what is the integral equation and what does it equal? Need to see the steps of your attempt.
 
http://64.9.205.64/~andrew/images/latex/images/flux_def.gif

A is the area of the face of the cone that the electric field penetrates, which is half of the surface area of the cone excluding the bottom area. So

http://64.9.205.64/~andrew/images/latex/images/cone_solution.gif
 
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I'm pretty sure that is not the formula for the surface area of a cone. I'd double check it, something doesn't look right about it.
 
You're right. It's SA=pi*R*S (neglecting the base) where S is the slant height. But that still doesn't explain why there's no pi in the textbook solution.
 
You need to consider the perpendicular part as you're dealing with a dot product. So the surface area you should calculate is not that of half a cone but... what?

That was a bit confusing. Anyways
\int_S \mathbf{E}\cdot d\mathbf{A} = E\int_S dA
is wrong.
 
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OK actually you don't need the surface area of cone. You have to take the projection of the cone onto a plane normal to the electric field. That's the area you are interested in.
 
That's what I thought too but... by that logic can't you say that the shape of a surface doesn't matter when considering the flux?
 
I am probably missing something but isn't the flux going to be zero since you have the electric field entering on one side and exiting the cone on the other? The normal direction would be pointing outwards and thus the sign of the dot product would reverse from one side to the other?
 
  • #10
kaotak said:
That's what I thought too but... by that logic can't you say that the shape of a surface doesn't matter when considering the flux?

That is the point of flux really, and the mathematical formulation to achieve this is the dot product. Think of water flow, it really doesn't matter what shape you stick in there, the same amount of water will flow through. If you throw in a closed surface, the same amount of water that flows in, flows out, unless there happens to be a source or a drain inside the surface. In electromagnetism this is called Gauss's law, which you've probably encountered, or soon will.

bdrosd said:
I am probably missing something but isn't the flux going to be zero since you have the electric field entering on one side and exiting the cone on the other? The normal direction would be pointing outwards and thus the sign of the dot product would reverse from one side to the other?

Only the part going in was asked in the problem.
 
  • #11
Oh, I see, thanks. I thought that was only true for a gaussian surface enclosing a charge, but it's also true for the effects of an external charge on the flux entering a gaussian surface (whoo, that was a mouthful).
 
  • #12
Yes, you require to take only the projection of area of cone on a plane normal to electric field and it is a triangle for the cone. Area of the triangle = 1/2 * 2r * h = rh
Hence flux = Erh.
 
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  • #13
päällikkö said:
that is the point of flux really, and the mathematical formulation to achieve this is the dot product. Think of water flow, it really doesn't matter what shape you stick in there, the same amount of water will flow through. If you throw in a closed surface, the same amount of water that flows in, flows out, unless there happens to be a source or a drain inside the surface. In electromagnetism this is called gauss's law, which you've probably encountered, or soon will.



Only the part going in was asked in the problem.

i am still not able to get it....

I am messed up with this concept of projection of area of different surfaces and flux through different surfaces...

Please someone explain it with some examples such as -

1. Hemisphere
2. Frustum
3. Cone

we have to find flux through all these surfaces
 
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