A conducting square loop is placed in a magnetic field B with its plane perpendicular to the field. The sides of the loop start shrinking at a constant rate \(\alpha \) The induced emf in the loop at an instant when its side is 'a' is
A) \(2a\alpha B\)
B) \({{a}^{2}}\alpha B\)
C)\(2{{a}^{2}}\alpha B\)
D)\(a\alpha B\)