A point charge ‘q’ is placed at the centre of one of the faces of cuboid PQRS as shown in the figure. If ∫E→. d s→ is electric flux through area ds. If value of ∫E→. d s→ over the surface QRUT is qkε0 and value of ∫E→. d s→ over the surface of PQRS is Nqε0 , then

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A point charge ‘q’ is placed at the centre of one of the faces of cuboid PQRS as shown in the figure. If $\int \vec{E} . d \vec{s}$ is electric flux through area ds. If value of $\int \vec{E} . d \vec{s}$ over the surface QRUT is $\frac{q}{k ε_{0}}$ and value of $\int \vec{E} . d \vec{s}$ over the surface of PQRS is $\frac{N q}{ε_{0}}$ , then

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