$\Rightarrow K \frac{Q_{1}}{r_1}=K \frac{Q_{2}}{r_{2}}$
$\Rightarrow \frac{Q_{1}}{r_{1}}=\frac{Q_{2}}{r_{2}}$
The ratio of electric fields
$\frac{E_{1}}{E_{2}}=\frac{K \frac{Q_{1}}{r_{1}^{2}}}{K \frac{Q_{2}}{r_{2}^{2}}}=\frac{Q_{1}}{r_1^{2}} \times \frac{r_{2}^{2}}{Q_{2}}$
$\Rightarrow \frac{E_{1}}{E_{2}}=\frac{r_{1} \times r_{2}^{2}}{r_1^{2} \times r_{2}}$
$ \Rightarrow \frac{E_{1}}{E_{2}}=\frac{r_{2}}{r_{1}}=\frac{2}{1}$
since the distance between the spheres is large as compared to their diameters, the induced effects may be ignored.
Reason : In a hollow spherical shield, the electric field inside it is zero at every point.

Note: $V_{1,2,3,4}$ are the potential differences across $C_{1,2,3,4}$ and $Q_{1,2,3,4}$ are the final charges stored in $C_{1,2,3,4}$ respectively.
