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184_notes:dist_charges [2021/02/13 19:20] – [Conducting Sphere of Charge] bartonmo | 184_notes:dist_charges [2021/02/13 19:26] (current) – [Insulating Cylinder of Charge] bartonmo | ||
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where Q is the total charge on the ball and →r points from the center of the sphere to the observation location. | where Q is the total charge on the ball and →r points from the center of the sphere to the observation location. | ||
- | However, what would happen to the electric field inside the sphere? We know that all of the charges should be located on the surface of the metal ball. When inside the sphere, there will always be a contribution to the electric field from the electrons on one side of the sphere that opposes the electric field contribution from the electrons on the other side of sphere. This means that on the inside, the electric field from the electrons on the surface perfectly cancels out, leaving a net field of zero. | + | However, what would happen to the electric field inside the sphere? We know that all of the charges should be located on the surface of the metal ball. When inside the sphere, there will always be a contribution to the electric field from the electrons on one side of the sphere that opposes the electric field contribution from the electrons on the other side of sphere. This means that on the inside, the electric field from the electrons on the surface perfectly cancels out,** leaving a net field of zero.** |
→Einside=0 | →Einside=0 | ||
This is actually the primary idea behind shielding sensitive electronics (also referred to as a [[https:// | This is actually the primary idea behind shielding sensitive electronics (also referred to as a [[https:// | ||
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Just like with the sphere, if we are outside the cylinder, the electric field will look the same as if the cylinder were a conductor (as long as it has the same amount of charge). Namely that it points radially away from the positively charged cylinder, expect near the ends of the cylinder. | Just like with the sphere, if we are outside the cylinder, the electric field will look the same as if the cylinder were a conductor (as long as it has the same amount of charge). Namely that it points radially away from the positively charged cylinder, expect near the ends of the cylinder. | ||
- | Inside the insulating cylinder, the electric field would be non-zero. The contributions to the electric field from the charges in the middle of the cylinder do not completely cancel out, leaving an electric field that points away from the center of the cylinder for a positive charge (it would point towards the center for a negative charge). The electric field inside will be strongest at the edge of the cylinder and will be smallest (or exactly zero) in the center. | + | Inside the insulating cylinder, the electric field would be non-zero. The contributions to the electric field from the charges in the middle of the cylinder do not completely cancel out, leaving an electric field that points away from the center of the cylinder for a positive charge (it would point towards the center for a negative charge). |
[{{184_notes: | [{{184_notes: |