Correct solution is option A ) \(2a\alpha B\)
Explaination:
"a" at any time "t" , the side of the square a= \((a_0-\alpha_t)\) , where \(\alpha_0\) side at t=0 .
at this instant , flux through the square
⇒\(\phi = BA\cos0^o = B(a_o-\alpha_t)^2 \)
⇒\(\therefore emf \ induced \ E= -\frac{d\phi}{dt}\)
⇒\(E=-B\times 2 (a_0-\alpha_t)\)
⇒E= \(2a\alpha B\)