Induced emf:
\[
\mathcal{E}=-\frac{d\phi_B}{dt}
\]
Current:
\[
I=\frac{\mathcal{E}}{r}
\]
So,
\[
I=\frac{1}{r}\left(-\frac{d\phi_B}{dt}\right)
\]
Since
\[
I=\frac{dQ}{dt}
\]
\[
\frac{dQ}{dt}=-\frac{1}{r}\frac{d\phi_B}{dt}
\]
Ignoring sign for magnitude relation:
\[
\Delta Q=\frac{\Delta \phi_B}{r}
\]
Hence,
\[
\boxed{(A)\ \Delta Q=\frac{\Delta \phi_B}{r}}
\]