Answer:
[tex]E = \frac{\lambda}{2\pi \epsilon_0 r}[/tex]
Explanation:
As we know that electric field due to long cylinder on a cylindrical Gaussian surface must be constant
so on the Gaussian surface we will have
[tex]\int E. dA = \frac{q_{en}}{\epsilon_0}[/tex]
now the electric field is passing normally through curved surface area of the cylinder
so we will have
[tex]E (2\pi rL) = \frac{q_{en}}{\epsilon_0}[/tex]
here enclosed charge in the cylinder is given as
[tex]q_{en} = \lambda L[/tex]
from above equation
[tex]E(2\pi rL) = \frac{\lambda L}{\epsilon_0}[/tex]
[tex]E = \frac{\lambda}{2\pi \epsilon_0 r}[/tex]