Electric field at tip of uniformly charged cone

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Homework Help Overview

The problem involves calculating the electric field at the tip of a uniformly charged cone with a specified surface charge density. The original poster expresses confusion regarding the divergence of the electric field at the tip, questioning the implications of treating charge as distributed over a surface rather than concentrated at a point.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the method of breaking the cone into differential hoops to calculate the electric field contribution from each hoop. There is also a consideration of how the electric field diverges at the tip and the implications of this divergence.

Discussion Status

Some participants confirm the original poster's derivation and explore the nature of electric fields at sharp tips, noting that while the question may seem unusual, it raises interesting points about the behavior of electric fields in relation to surface charge density and curvature.

Contextual Notes

Participants note the distinction between uniformly charged surfaces and conductors, questioning how the principles might differ in these contexts. The discussion includes references to the physical characteristics of sharp tips and their effect on electric fields.

musemonkey
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1. Find the electric field at the tip of a cone of height and radius R with uniform surface charge density \sigma.

I get that the field diverges at the tip, which is puzzling because it's not as though there's a point charge at the tip. I thought this sort of thing can't happen when you treat charge as smeared over a surface.


2. Homework Equations

The field from a hoop of radius z, charge q, at height z above the hoop center is

E_{hp} = \frac{q}{4\pi\epsilon_0} \frac{1}{2\sqrt{2}z^2}.

The Attempt at a Solution



I break the cone into hoops of variable radius. Because it's a right cone, the distance from the tip to each differential hoop equals the radius -- very convenient. The charge on each hoop is

dq = 2\pi z \sigma ds = 2\pi z \sigma \sqrt{2} dz

where ds = \sqrt{2} dz is a differential arc length along the side of the cone.

Each hoop contributes to the field

dE = \frac{dq}{4\pi\epsilon_0} \frac{1}{2\sqrt{2}z^2}

= \frac{2\pi z \sigma \sqrt{2} dz}{4\pi\epsilon_0} \frac{1}{2\sqrt{2}z^2}

= \frac{\sigma}{4\epsilon_0} \frac{dz}{z},

and the field is then

\int dE = \int_0^R \frac{\sigma}{4\epsilon_0} \frac{dz}{z} = \left . \frac{\sigma}{4\epsilon_0} \ln z \right |_R^0,

which blows up at 0.

Correct? If so, what to make of it? Special surfaces can mimic point charges?
 
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Your derivation looks fine to me.

From what I remember, electric fields do diverge for sharp tips. In practice, a real "tip" will be rounded off, even if at the molecular scale. The actual field depends on the radius-of-curvature for the tip.

Still it seems a rather odd question to ask, which is essentially show that E is infinite for a particular sharp tipped object.
 
I've read that high fields arise at sharp tips of charged conductors because the surface charge density is much greater there. But since this is not a conductor but a uniformly charged surface, I'm not sure the two cases are actually related.

Your point about curvature is very interesting. I'll look into that. Thanks and thank you for checking my derivation!
 
check Jackson pg 104
 
musemonkey said:
But since this is not a conductor but a uniformly charged surface, I'm not sure the two cases are actually related.
That is correct. However, a sharp tip is still a sharp tip, and the electric field will basically be pointing away from the surface, so it must spread out from that point.

I agree, this is a strange question to ask.
 

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