Potential at the edge of disc
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(c) 4σkR
Explanation : dV=kdqr
dq=σ(2rθ)dr
dV=14π∈0σ2rdrθr=σ2π∈0θdr
r=2Rcosθ
r=2Rcosθ
dr=−2Rsinθdθ
dr=−σ2π∈02Rθsinθdθ
V=∫0π2dV=σRπ∈0∫π20θsinθdθ
V=σRπ∈0=4kσR.
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