Calculating E in a hemispherical shell using Coulomb's law

In summary, the conversation is discussing a problem involving the electric field generated by a ring along the axis of a hemisphere. The solution involves slicing the hemisphere into tiny rings and using the symmetry of the charge distribution to determine the electric field along the axis. The rest of the conversation involves providing a visual representation of the problem to better understand the solution.
  • #1
Lisa...
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My teacher worked out the following problem as shown below:

http://img116.imageshack.us/img116/7656/naamloos27mf.gif

The only thing is I don't really understand what he's doing, so could anybody please explain to me a bit more which steps he takes? I would be very greatful! (or maybe there's an easier way to solve it...)
 
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  • #2
Basically what he's doing is slicing the hemisphere into a whole bunch of tiny rings. Presumably equation 23-10 describes the electric field generated by a ring along the axis which runs through its center. Due to symmetry in x and y (there's just as much charge to one side of the ring as the other) the electric field along this axis must be entirely in z.

The rest of it is just some geometry on the surface of the sphere, unfortunately I don't have time to draw a picture and scan it just now. If nobody else has replied by the time I get back from class I'll see if I can whip something up for you.
 
  • #3
Hi Lisa,

I wrote up the problem and scanned it, hopefully this will help. I derived the E field from a ring of charge up near the top since I didn't have a handy reference. I then drew out the geometry on the surface of the sphere and used that to relate back to the field from the ring of charge. Hopefully this will help you see what's going on.

The file is http://www.warpenguin.com/~dice/hemisphere.jpg , it's huge though. I think you should be able to print it out and it should look okay, or you can just zoom out and read it on your monitor.

Let me know if you have any questions :smile:
 
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FAQ: Calculating E in a hemispherical shell using Coulomb's law

How is Coulomb's law used to calculate E in a hemispherical shell?

Coulomb's law is used to calculate the electric field (E) in a hemispherical shell by considering the distribution of charge on the surface of the shell. The law states that the electric field at a point in space is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance from the charge. By applying this law to the charge distribution on the surface of the hemispherical shell, the electric field at any point inside the shell can be calculated.

What is the equation for calculating E in a hemispherical shell using Coulomb's law?

The equation for calculating E in a hemispherical shell using Coulomb's law is E = (1/4πε0) * Q/R2, where ε0 is the permittivity of free space, Q is the total charge on the surface of the shell, and R is the distance from the center of the shell to the point where the electric field is being calculated.

Can Coulomb's law be used for any charge distribution on the surface of a hemispherical shell?

Yes, Coulomb's law can be used for any charge distribution on the surface of a hemispherical shell as long as the charge is uniformly distributed and the distance from the center of the shell to the point where the electric field is being calculated is known.

How does the magnitude of the charge affect the electric field in a hemispherical shell?

The magnitude of the charge has a direct effect on the magnitude of the electric field in a hemispherical shell. According to Coulomb's law, the electric field is directly proportional to the magnitude of the charge. This means that as the charge increases, the electric field also increases.

What is the significance of calculating E in a hemispherical shell using Coulomb's law?

Calculating E in a hemispherical shell using Coulomb's law is significant because it allows us to understand and predict the behavior of electric fields in real-world systems. This knowledge is crucial in various fields of science and engineering, such as electronics, telecommunications, and energy systems.

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