a non conducting ring of radius r = 10 cm has linear charge density lambda = 2cos(0/2)*10^-10c/m as shown in figure the potential at the ring in volt is
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Consider two small elements of length dl=Rdθ symmetrically at angle θ on both sides as shown in the figure. Here, dE
1 =dE
2
and sin component cancel out each other. Charge on the element , dq=λdl=(λ 0cosθ)Rdθ
Net field at center due to both elements , dE=2dE 1 cosθ=2( 4πϵ 0 R 2 dq )cosθ= 4πϵ 0 R λ 0 2cos 2 θdθ
or
E= 4πϵ 0 R λ 0 ∫ 0 π (1+cos2θ)dθ= 4πϵ 0 R λ 0 [(π−0)+ 2 1 (sin2π−sin0)]= 4ϵ 0 R λ 0
thus, x=4
Therefore the potential of the ring in volt is 4.
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