A long charged cylinder of linear charge density \(\lambda\) is surrounded by a hollow coaxial conducting cylinder. The magnitude of electric field in the space between the two cylinders at a distance \(R\) from the common axis of the cylinders is
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For an infinitely long line charge,
\[
\boxed{
E=\frac{\lambda}{2\pi\varepsilon_0r}.
}
\]
The surrounding conducting cylinder does not alter the electric field in the empty region between the two cylinders; only the enclosed charge matters in Gauss' law.