How Does Gauss's Law Apply to Electric Fields at Points P2 and P3?

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Gauss's Law was applied to derive the electric field for a cylindrical charge distribution, resulting in E = (ρ * r) / (2ε₀) for points outside the cylinder. At Point 1 (P1), the electric field was determined to be 0 V/m due to the radial distance being zero at the surface. There was confusion regarding the electric field at Point 2 (P2), as it seemed counterintuitive for it to also be zero. The discussion shifted to calculating the electric field at Point 3 (P3) using the electric field equation for a charged disk, with integration suggested to find the total field. The consensus emphasized that Gauss's Law may not be applicable for finite-length cylinders, and integrating the derived electric field expression was the recommended approach.
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[SOLVED] Gauss and E-Field

Homework Statement


http://img443.imageshack.us/img443/9452/eletroof9.th.png

My main problem with this problem is finding the electric field at Point 2 (P2)

Homework Equations


The Attempt at a Solution



I derived the electric field using Gauss's Law for a cylindrical charge distribution.
E (2\pi rL ) = \rho(\pi r^2 L) / \varepsilon_0
E = \frac{\rho * r}{2\varepsilon_0}
So I found E at P1 to be 0 V/m

Now onto finding E at P2, according to my equation, it would seem that E is 0, since the radial distance is 0, however that seems strange to me, if the point is at the surface of the charged volume cylinder, wouldn't there be some charge, I know it's not a conductor but still I would think that there would be some charge?And since I've got it all out here, is the E field at P3 just the integral [3/2L, L/2] of a charged disk?
 
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The gausses law won't help you much here.
Try working with Ex = k*q*x/r^3.
 
Thanks for your reply,

I can't use Gauss's Law for finding any of the points? I know usually the cylinder is an infinite length if you want to find E, but even for Point 1 I can't use it?
 
Basically not in or outside finite length cylinder the tangential forces will cancel only at the midpoints. Try finding E on axis of a charged disc first.
 
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Ok so I've got the equation for a charged disk
2\pi k \rho (1 - \frac{x}{\sqrt{x^2+a^2} ) } how do I integrate that over the length (L) to get the electric field of the cylinder?

Would I say that dE = 2\pi k \rho (1 - \frac{x}{\sqrt{x^2+a^2} ) } and then integrate dE from 0 to L or do I need to differentiate Edisk before I do that?
 
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Just integrate it form 0 to L, since ddQ = 2*pi*rho*a*da*dx and u integrated it along a then your equation should still contain dx.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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