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In the given figure, calculate the total flux of the electrostatic field through the sphere S1 and S2. The wire AB, as shown here, has a linear charge density λ given by λ = kx, where x is the distance measured along the wire, from the end A.

electrostatic field

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Since linear charge density λ (λ = kx) depends on distance, so it is not constant. Thus consider a small element dx having charge dq, then

dq = λ dx = kx dx

∴ q = λdq = k \(\int_0^1 xdx=\frac{kl^2}{2}\)

Electric flux through Gaussian surface is:

\(\phi_1= ∮ \vec E. \vec{dS}= \frac{q}{ɛ_o} = 0\) (∵ q = 0 inside s1)

Electric flux through Gaussian surface S2 is:

\(\phi_2= ∮ \vec E. \vec{dS}= \frac{q}{ɛ_o} = \frac{kl^2}{2ɛ_o}\) (∵ q = \(\frac{kl^2}{2}\))

Total electric flux thorugh the spheres S1 and S2

Φ = Φ1 + Φ2

or Φ = 0 + \(\frac{kl^2}{2}\) = \(\frac{kl^2}{2ɛ_o}\)

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