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