Let $P_1$ and $r_1$ be the pressure and radius of the bubble at the bottom of the tank, and $P_2$ and $r_2$ be the pressure and radius at the top surface. At the bottom, $P_1 = P_{atm} + \rho gh = 10 + 7.28 = 17.28$ m of water (where $\rho$ is the density of water and $h$ is the depth). At the top, $P_2 = P_{atm} = 10$ m of water. Since the temperature is constant, we can use Boyle's law: $P_1V_1 = P_2V_2$. $P_1(\frac{4}{3}\pi r_1^3) = P_2(\frac{4}{3}\pi r_2^3)$ $17.28 r_1^3 = 10 r_2^3$ $\frac{r_1^3}{r_2^3} = \frac{10}{17.28} = \frac{10}{10+7.28}$ $\frac{r_1}{r_2} = \sqrt[3]{\frac{10}{17.28}} = \frac{\sqrt[3]{10}}{2.579} \approx \frac{5}{6}$ If $P_{atm}=10$ m of water, and $h=7.28$ m, then $P_1 = 10\rho g + 7.28\rho g$ and $P_2=10 \rho g$. $P_1 V_1 = P_2 V_2$ so $(17.28 \rho g) (\frac{4}{3}\pi r_1^3) = (10\rho g)(\frac{4}{3}\pi r_2^3)$ $17.28 r_1^3 = 10r_2^3$ $\frac{r_1}{r_2} = \sqrt[3]{\frac{10}{17.28}} \approx 0.833 \approx \frac{5}{6}$.