Electric Field in a Hemisphere

AI Thread Summary
The discussion focuses on calculating the electric field at the center of curvature of a nonconducting hemispherical cup with a uniform charge distribution. Initial calculations yield an electric field of kQ/R², but the expected answer is kQ/3R². Participants clarify that the x and y components of the electric field cancel due to symmetry, leaving only the z-component. Further integration leads to a derived electric field of kQ/2R², which still does not match the book's answer. The consensus is that the book's answer may be incorrect unless the hemispherical cup is closed, which would alter the surface area and the resulting electric field calculation.
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Homework Statement



A nonconducting hemispherical cup of inner Radius R has a total charge Q spread uniformly over its inner surface. Find the electric field at the center of curvature.

Homework Equations



\sigma = \frac{Q}{2piR^{2}}

dq = \sigma dA = \sigma R^{2}Sin\thetad\thetad\phi
k = \frac{1}{4\pi\epsilon_{}0}

The Attempt at a Solution



dE = \frac{kdq}{R^{2}}
dE = \frac{k \sigma R^{2} Sin\theta d\theta d\phi}{R^{2}} = k \sigma Sin \theta d \theta d \phi

E = k \sigma \int^{2 \pi}_{0} \int^{\frac{\pi}{2}}_{0} Sin \theta d \theta d \phi
E = k \sigma 2 \pi = k \frac{Q}{R^{2}}

But for some reason, the answer is listed as k \frac{Q}{3R^{2}}. I have no idea why my answer is factor of 3 larger. Any help would be appreciated.
 
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Do not forget that the electric field is a vector quantity, so is dE. You can add the contributions as vectors: Determine the x, y and z components of dE and integrate.

ehild
 
Alright, so the x and y components of the field will cancel by symmetry correct? Therefore, only the z-component dEz = dECos\theta will remain.

Ez = k \sigma \int^{2 \pi}_{0} \int^{\frac{\pi}{2}}_{0} Sin \theta Cos \theta d \theta d \phi
Ez = k \sigma \int^{2 \pi}_{0} \frac{1}{2} [Sin^{2} \theta]^{\frac{\pi}{2}}_{0} d \phi
Ez = k \sigma \int^{2 \pi}_{0} \frac{1}{2} d \phi
Ez = k \sigma \pi = k \frac{Q}{2 R^{2}}

This still seems to be off from the correct answer unless I did this wrong.
 
It looks correct to me. I don't know why the answer is listed differently...
 
So the correct answer is k \frac{Q}{2 R^{2}} ?
 
Yes, that's what I get the answer to be.
 
My definition of the center of curvature is correct right? It would be the center of the bottom of the hemisphere? If so, I guess the book's answer is wrong.
 
Yes, I would have thought the centre of curvature was the centre of the bottom of the hemisphere. (since this point is equidistant from any point on the curve).

It seems to me that the book is wrong. This does happen sometimes. (Rarely, though).
 
If the cup is closed (with a cover), it adds /pi r^2 to the surface and the book's answer is correct.
 
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