Since the process is isothermal and occurs in a vacuum, the pressure inside the soap bubbles is due to surface tension, and we can use the ideal gas law for the air inside the bubbles. The pressure inside a soap bubble is given by:
\[
P = \frac{4\sigma}{r}
\]
where \( \sigma \) is the surface tension, and \( r \) is the radius. However, in a vacuum, the external pressure is zero, so the pressure inside is entirely due to surface tension. The number of moles of air inside each bubble can be found using the ideal gas law \( PV = nRT \).
The volume of a bubble is \( V = \frac{4}{3} \pi r^3 \), so for the two bubbles:
- Bubble 1: \( V_1 = \frac{4}{3} \pi r_1^3 \), pressure \( P_1 = \frac{4\sigma}{r_1} \),
- Bubble 2: \( V_2 = \frac{4}{3} \pi r_2^3 \), pressure \( P_2 = \frac{4\sigma}{r_2} \).
The number of moles in each bubble:
\[
n_1 = \frac{P_1 V_1}{RT}, \quad n_2 = \frac{P_2 V_2}{RT}
\]
Substitute the pressures and volumes:
\[
n_1 = \frac{\left( \frac{4\sigma}{r_1} \right) \left( \frac{4}{3} \pi r_1^3 \right)}{RT} = \frac{16\sigma \pi r_1^2}{3RT}, \quad n_2 = \frac{\left( \frac{4\sigma}{r_2} \right) \left( \frac{4}{3} \pi r_2^3 \right)}{RT} = \frac{16\sigma \pi r_2^2}{3RT}
\]
Total moles in the new bubble:
\[
n = n_1 + n_2 = \frac{16\sigma \pi (r_1^2 + r_2^2)}{3RT}
\]
For the new bubble of radius \( r \), the pressure is \( P = \frac{4\sigma}{r} \), volume \( V = \frac{4}{3} \pi r^3 \), and moles:
\[
n = \frac{\left( \frac{4\sigma}{r} \right) \left( \frac{4}{3} \pi r^3 \right)}{RT} = \frac{16\sigma \pi r^2}{3RT}
\]
Equate the total moles:
\[
\frac{16\sigma \pi r^2}{3RT} = \frac{16\sigma \pi (r_1^2 + r_2^2)}{3RT}
\]
\[
r^2 = r_1^2 + r_2^2 \quad \Rightarrow \quad r = \sqrt{r_1^2 + r_2^2}
\]
So, the radius of the new soap bubble is \( \sqrt{r_1^2 + r_2^2} \).