Calculating electric fields

In summary, the problem involves two concentric plastic spherical shells with uniformly distributed charges of Q on the inner shell and -Q on the outer shell. To find the electric field, we can use the equation integration(E * n)dA = (4pi) (k) (Qenclosed). By solving for E, we get E = kQ/pi r^2, where r is the distance from the center of the shells. For the charges outside the larger shell and inside the smaller shell, we use the same method but with different Gaussian surfaces. This method is valid because of symmetry.
  • #1
ibaraku
13
0

Homework Statement


Two concentric plastic spherical shells carry uniformly distributed charges, Q on the inner shell and -Q on the outer shell. Find the electric field (a)Inside the smaller shell, (b)between the shells, and (c) outside the larger shell

Homework Equations



integration(E * n)dA = (4pi) (k) (Qenclosed)

The Attempt at a Solution



In order to get hteh electric field between the shells, we can say that

[abs(E) * abs(n) cos delta](4pi) r^2 = (4pi) (k) (Qenclosed)

and working out the algebra it comes out to be

E = kQ/pi r^2

but what about for the charge outside the larger shell and the charge inside the smaller charge?
Is it safe to say that the we need to divide by 2 for the smaller shell and multiply by 2 for the large shell?
Thanks
 
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  • #2
ibaraku said:
[abs(E) * abs(n) cos delta](4pi) r^2 = (4pi) (k) (Qenclosed)

and working out the algebra it comes out to be

E = kQ/pi r^2
Yes that's right.
ibaraku said:
but what about for the charge outside the larger shell and the charge inside the smaller charge?
Is it safe to say that the we need to divide by 2 for the smaller shell and multiply by 2 for the large shell?
Thanks
You do this the same way as you did the above, except now the Gaussian surface for (a) cuts through the smaller sphere, and in (c) the Gaussian surface encloses both spheres. There isn't any way you can use the result obtained above to compute for the other two cases. The method used is still valid, though because of symmetry.
 
  • #3
for your question. For the charge outside the larger shell, the electric field can be found using the same equation, but with the enclosed charge being -Q instead of Q. So the electric field would be E = -kQ/pi r^2. As for the charge inside the smaller shell, we can use the same equation, but with the enclosed charge being 0, since there is no charge inside the smaller shell. So the electric field inside the smaller shell would be E = 0. It is not necessary to divide by 2 or multiply by 2 for these cases.
 

1. How do you calculate an electric field?

To calculate an electric field, you need to know the magnitude and direction of the electric charges involved and the distance between them. The formula for electric field is E = kQ/r^2, where k is the Coulomb's constant, Q is the electric charge, and r is the distance between the charges.

2. What is the unit of electric field?

The unit of electric field is newtons per coulomb (N/C) in the SI (International System of Units) system. In the CGS (Centimeter-Gram-Second) system, the unit of electric field is dynes per statcoulomb (dyn/esu).

3. Can you have a negative electric field?

Yes, electric field can be either positive or negative. A positive electric field indicates that the electric force on a positive charge is in the same direction as the field, while a negative electric field indicates that the electric force on a positive charge is in the opposite direction.

4. How does distance affect the electric field?

The electric field decreases as the distance from the source charge increases. This is because the electric force follows an inverse square relationship with distance, meaning that the force decreases as the distance squared increases. As a result, the electric field also decreases with distance.

5. Can you calculate the electric field at a point between two charges?

Yes, the electric field at a point between two charges can be calculated by taking into account the electric fields from both charges. You would use the principle of superposition, which states that the net electric field at a point is equal to the vector sum of the individual electric fields at that point.

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