Electric field of charge distributions


by demonhunter19
Tags: charge, distributions, electric, field
demonhunter19
demonhunter19 is offline
#1
Sep12-08, 12:34 PM
P: 10
1. The problem statement, all variables and given/known data

A small, thin, hollow spherical glass shell of radius R carries a uniformly distributed positive charge +Q, as shown in the diagram above. Below it is a horizontal permanent dipole with charges +q and -q separated by a distance s (s is shown greatly enlarged for clarity). The dipole is fixed in position and is not free to rotate. The distance from the center of the glass shell to the center of the dipole is L.

The charge on the thin glass shell is +6e-09 coulombs, the dipole consists of charges of 4e-11 and -4e-11 coulombs, the radius of the glass shell is 0.15 m, the distance L is 0.45 m, and the dipole separation is 2e-05 m. Calculate the net electric field at the center of the glass shell. The x axis runs to the right, the y axis runs toward the top of the page, and the z axis runs out of the page, toward you.

E^^->_(net) = < , , > N/C

If the upper sphere were a solid metal ball with a charge +6e-09 coulombs, what would be the net electric field at its center?
E^^->_(net) = < , , > N/C

Which of the diagrams below best shows the charge distribution in and/or on the metal sphere?
A
B
C
D
E
F
G
H
J
K

2. Relevant equations
Electric Force of Dipole: (1/4*pi*epsilon_0)(q*s)/r^3
Electric Force of Sphere: (1/4*pi*epsilon_0)(Q/r^2)


3. The attempt at a solution

The question is kind of confusing to me, as it asks to calculate the net electric field at the CENTER of the glass shell. Right now I'm assuming that the electric field AT THE CENTER of the glass shell is zero (is this assumption not correct? since r<R inside the sphere) and that to answer this first part of the question, it would just be the electric field of the DIPOLE, which is <.000079,0,0>N/C.
Also, if I do calculate the electric field of the glass shell, from the center of the glass shell to the center of the dipole, whose distance is .45m, then I would obtain <0,266.667,>N/C.

I am really confused about this first part.

As for the second part, I would assume it would be the same values as when I calculate the net electric field at the center of the glass shell.

For the last part (multiple choice) I'm not entirely sure, but I'm leaning towards C.

HELP WOULD BE MUCH APPRECIATED, and thank you in advance.
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Irid
Irid is offline
#2
Sep14-08, 09:52 AM
P: 208
You solved the first part correctly. To find the total field, you must sum up the fields of the glass sphere and of the dipole (principle of superposition). Glass sphere gives zero because charge is distributed uniformly, dipole gives according to the formula.

In the second part, not that the field inside any conductor is always zero, i.e. the charge on the surface of the metal sphere distributes in such a way so as to cancel the field of the dipole inside the sphere.
demonhunter19
demonhunter19 is offline
#3
Sep14-08, 12:00 PM
P: 10
So, what you're saying for the second part is that the only electric field within this system is the metal sphere? Would the dipoles have any effect? If not, then the only net electric is to the negative y direction (as seen in the picture)? So then to calculate the electric field of just the metal sphere, it is 1/(4*pi*epsilon_0)*Q/A?

Irid
Irid is offline
#4
Sep14-08, 01:34 PM
P: 208

Electric field of charge distributions


Quote Quote by demonhunter19 View Post
So, what you're saying for the second part is that the only electric field within this system is the metal sphere? Would the dipoles have any effect? If not, then the only net electric is to the negative y direction (as seen in the picture)? So then to calculate the electric field of just the metal sphere, it is 1/(4*pi*epsilon_0)*Q/A?
I'm not saying that. All the charge in the surroundings contribute to the electric field, both the sphere and the dipole. However, the charge on the sphere distributes in such a way as to oppose the dipole and make the field zero inside the sphere. It's the nature of conductors. Under any circumstances the field inside the conductor is zero.


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