A hemisphere of radius r is charged uniformly with surface charge density sigma, what will be the potential at the centre?
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Given details:
Radius of the hemisphere is 'r'.
Surface charge density is 'σ'
Solution:
In the hemisphere, let us consider a small element of angle θ.
Potential due this small element will be dV = σ r / 2 ε * (sin θ dθ)
Now, let us integrate dV with respect to θ in the interval 0 to π/2,
So, at the centre of the hemisphere, potential will be given by V = σ r / 2 ε
Hope it helps. Thank You!
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