Electric field at centre o of semicircle of radius a having linear charge density is given as
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consider a small element of length dl and charge = dq = λ dl , at which point the radius makes an angle θ with the vertical through the center of geometry of the semi circle.
K = 1/(4πε)
dE = K dq/a² , makes an angle θ with the vertical.
The components along the y axis (vertical) add up. The limits are θ = -π/2 to π/2.
dl = a dθ
dE_y = (K λ /a) Cos θ dθ
integrating, E = (K λ / a) [sinθ ] from θ = -pi/2 to pi/2
E = 2 K λ/a
K = 1/(4πε)
dE = K dq/a² , makes an angle θ with the vertical.
The components along the y axis (vertical) add up. The limits are θ = -π/2 to π/2.
dl = a dθ
dE_y = (K λ /a) Cos θ dθ
integrating, E = (K λ / a) [sinθ ] from θ = -pi/2 to pi/2
E = 2 K λ/a
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