Electric field at tip of uniformly charged cone

AI Thread Summary
The discussion centers on calculating the electric field at the tip of a uniformly charged cone with surface charge density σ. It is noted that the electric field diverges at the tip, raising questions about the implications of treating charge as distributed over a surface rather than as a point charge. The derivation involves breaking the cone into differential hoops and calculating the contribution of each hoop to the electric field, leading to an integral that diverges as it approaches the tip. Participants acknowledge that while sharp tips can produce high electric fields, the scenario differs from conductors, where surface charge density increases significantly. The conversation concludes with an agreement that the behavior of electric fields at sharp tips is indeed complex and warrants further exploration.
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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