In the figure, a very large plane sheet of positive charge is shown. P1 and P2 are two points at distance l and 2l from the charge distribution. If σ is the surface charge density, then the magnitude of electric fields Eand E2 and P1 and P2 respectively are

1
\(E_1=\frac{\sigma}{\varepsilon_0}, E_2=\frac{\sigma}{2 \varepsilon_0}\)
2
\(E_1=\frac{2 \sigma}{\varepsilon_0}, E_2=\frac{\sigma}{\varepsilon_0}\)
3
\(E_1=E_2=\frac{\sigma}{2 \varepsilon_0}\)
4
\(E_1=E_2=\frac{\sigma}{\varepsilon_0}\)
5
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