If a charge q is placed at the centre of a closed hemispherical non-conducting surface, the total flux passing through the flat surface would be :

1
zero
2
\(\rm \frac{q}{2 \varepsilon_{0}}\)
3
\(\rm \frac{{q}}{4 \varepsilon_{0}}\)
4
\(\rm \frac{q}{2 \pi \varepsilon_{0}}\)

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