Step 1: In vacuum and under isothermal conditions, volume is conserved when two bubbles combine.
\[
\text{Let the radius of each original bubble be } r = 2\, \text{cm}
\]
Step 2: Volume of each bubble = \(V = \frac{4}{3}\pi r^3\)
Total volume of two bubbles:
\[
V_{\text{total}} = 2 \times \frac{4}{3} \pi r^3 = \frac{8}{3} \pi r^3
\]
Let \(R\) be the radius of the new bubble. Then:
\[
\frac{4}{3} \pi R^3 = \frac{8}{3} \pi r^3 \Rightarrow R^3 = 2r^3 \Rightarrow R = r . \sqrt[3]{2}
\]
This is correct for general isothermal processes. However, in this particular question, **surface energy in vacuum** is also conserved (assuming ideal condition), and **pressure difference** inside bubble is considered. Hence, **pressure-volume** product is conserved due to **isothermal process**:
\[
P_1V_1 + P_2V_2 = P_fV_f
\]
For small soap bubbles under vacuum, the relation reduces to:
\[
R = \sqrt[3]{R_1^3 + R_2^3}
\]
Step 3: Since \(R_1 = R_2 = 2\, \text{cm}\), we get:
\[
R = \sqrt[3]{2^3 + 2^3} = \sqrt[3]{16} = 2 \sqrt[3]{2}
\]
But in case of isothermal expansion of **gas** inside ideal soap bubbles (in vacuum), using pressure relation:
\[
P \propto \frac{1}{R},
PV = \text{constant} \Rightarrow \frac{1}{R} . R^3 = \text{constant} \Rightarrow R^2 = \text{constant}
\Rightarrow R = \sqrt{R_1^2 + R_2^2}
\]
Final Calculation:
\[
R = \sqrt{2^2 + 2^2} = \sqrt{8} = 2\sqrt{2}
\]
% Final Answer
\[
\boxed{2\sqrt{2} \, \text{cm}}
\]