Potential energy of an hemispheric shell

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Homework Help Overview

The problem involves calculating the electric potential at points along the z-axis due to a hemispherical shell with a uniform surface charge distribution. The original poster attempts to set up the integral for potential using surface integrals and spherical coordinates.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss breaking the problem into smaller pieces using trigonometric angles and surface elements. There are questions about the correct setup for the vector difference R-R' and the surface element ds. Some participants suggest using the Law of Cosines and reconsidering the angles used in the setup.

Discussion Status

The discussion is ongoing, with participants providing guidance on visualizing the problem and clarifying the setup. There is an exchange of ideas about the correct expressions for the vectors and surface elements, but no consensus has been reached on the final approach.

Contextual Notes

Participants are working under the constraint of a uniform charge distribution and are exploring different coordinate systems to simplify the integral. There is mention of potential confusion regarding the angles used in the spherical coordinate system.

BSJ90
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Homework Statement


Given that the hemisphere has a charge +Q distributed through its surface with radius a. Find the electric potential on any point on z axis (the plane of the hemisphere is oriented in positive z direction).

Homework Equations


\phi = \int\frac{kQ}{|R-R'|}*ds
(surface integral)

The Attempt at a Solution


So i decided to break this problem into little pieces of the surface using some trig.

I made a angle θ from the plane of the hemisphere around the cross section (so there is semi circles) and then an angle \varphi on the xy-plane.

I found ds to be a^{2}d\varphid\theta (using the arc lengths of my angles and radii).

Now my problem is finding an equation for the vector R-R'. I tried making it a function of \theta (i.e. i got (sqrt(z^{2} + a^{2}sin^{2}(\theta)
but the integral was not a nice one and it lead me to believe that it wasn't correct. if someone can help me along that would be great!
 
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Is the charge evenly distributed on the surface?

Make a picture and indicate R and R'!


ehild
 
oh yeah evenly distributed on surface. I made a paint object to help clarify. R' is to the ds and R is to the point on the z axis. I know R has to be z but I am having a problem figuring out R'. Thanks for this and the last problem you help me with.
 

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Nice picture! :smile: You need the magnitude of the vector difference of R-R'. What about using the Law of Cosines?
To make your task more clear I draw an other picture with Paint (using the option to draw circle, ellipse, straight line )

ehild
 

Attachments

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    hemisphere.JPG
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ok so should my theta be from the z axis and i think that changes my whole set up oh wait i can use 90 + theta and it would work. Ok thanks time to go to work on it. Plus i only really care about the z direction.
 
I get my |R- R'| = \sqrt{ a^2 +z^2 + 2azsin(θ)}. look right? Umm this isn't turning out to be a easy integral. I am thinking mabye go back to Cartesian.
 
Last edited:
Last edited:
I just need to add 90 degrees to my theta so it restricts it to my hemisphere not a whole sphere. The ds stays the same except for that sin(θ) term which i added.
 
It will not be sin(theta) in the surface element of your special spherical system of coordinates.

ehild
 

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