Repulsion Forces Between Northern & Southern Hemisphere of Metal Sphere

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Homework Help Overview

The problem involves a metal sphere of radius R with a total charge Q, specifically examining the force of repulsion between its northern and southern hemispheres. The context is centered around electrostatics and the behavior of electric fields in conductors.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the implications of the electric field being zero inside the sphere and question how the hemispheres can exert forces on each other despite this. There is exploration of the nature of charge distribution and the resulting electric fields.

Discussion Status

The discussion is ongoing, with participants providing insights into the behavior of electric fields in conductors and the implications for charge distribution. Some guidance has been offered regarding the nature of the fields at the surface of the sphere, but no consensus has been reached on the original poster's question.

Contextual Notes

Participants are navigating assumptions about the behavior of electric fields within and around conductive materials, particularly in relation to the distribution of charge and the resulting forces between hemispheres.

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Homework Statement


A metal sphere of radius R carries a total charge Q. What is the force
of repulsion between the "northern" hemisphere and the "southern" hemisphere?

Homework Equations

The Attempt at a Solution


Since the sphere is metallic, its conducting and so the electric field inside the sphere is 0, and outside the sphere it is perpendicular to the surface and is radially outwards, and so, the force exerted by the northern hemisphere on the southern hemisphere should be 0. However, the answer appears to be other than zero. why?
 
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The net field inside is zero because the all the individual fields from the individual charges distributed around the sphere cancel each other out in the interior. That does not say that those same fields don't serve to push all the charges to the skin of the sphere, keeping them spread out evenly over the surface.

As far as the mutual repulsion of hemispheres goes, you've still got two charge distributions pushing on each other.
 
But those charge distributions have an electric field that is radially outwards, how can they push on each other?
 
Lea said:
But those charge distributions have an electric field that is radially outwards, how can they push on each other?
Each charge has a spherically symmetric field radiating outward around itself. Exterior to the sphere the net effect of summing all the fields leaves just the radially outward part. Within the sphere they all cancel. The overall effect is to be able to perceive no field in the interior of the sphere and a radially outward field exterior to the sphere.

At the surface where the charges reside, they are feeling the effects of the net radial field. This is what keeps those charges confined to the outer surface. The fields aren't mutually canceled from there outward, so each of the individual charges is "feeling" a net field that looks as if all the charge Q were placed as a point charge at the center of the sphere (and the conducting sphere is ignored).
 
Thank you! I understand now.
 

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