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Asked in GSEB Board March 2023 · Equipotential surfaces and V-r graphs
Idea: at a distance r much larger than the size of the collection, all the charges are at practically the same distance from the field point.
The potential is then V ≈ 1/(4πε₀)(Qₙₑₜ)/r, the same as for a single point charge Qₙₑₜ eq 0.
This V depends only on r, so V = constant means r = constant.
So the far-away equipotential surfaces are approximately spheres centred on the collection.
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