1. \(d\phi=\overrightarrow E.d \overrightarrow s\)
2. Gauss’s law:
Guass’s law states that total flux over a closed surface is 1/s0 times net charge enclosed by the surface.
3. Field due to A uniformly charged infinite plane sheet:

Consider an infinite thin plane sheet of change of density σ.
To find electric field at a point P (at a distance ‘r’ from sheet), imagine a Gaussian surface in the form of cylinder having area of cross section ‘ds’.
According to Gauss’s law we can write,
\(\int\overrightarrow E.d\overrightarrow s=\frac{1}{\varepsilon_0}q\)
\(E\int ds=\frac{\sigma ds}{\varepsilon_0}\)(Since q = σds)
But electric field passes only through end surfaces ,so we get ∫ds = 2ds
i.e. E2ds = \(\frac{\sigma ds}{\varepsilon_0}\)
\(E = \frac{\sigma ds}{2ds\varepsilon_0}\), \(E = \frac{\sigma }{2\varepsilon_0}\)
E is directed away from the charged sheet, if σ is positive and directed towards the sheet if σ is negative.