Practicing Success
A hemisphere of radius R is placed between two uniformly charged-thin infinite sheets of charge density $+σ$ and $-σ$. Flux through the curved surface of the hemisphere |
$\frac{σ}{2ε_0}(πR)$ $\frac{σ}{ε_0}(πR^2)$ $\frac{σ}{ε_0}(2πR^2)$ Zero |
$\frac{σ}{ε_0}(πR^2)$ |
The correct answer is Option (2) - $\frac{σ}{ε_0}(πR^2)$ |