Step 1: Let the voltage at the node connected to the \(60\,\text{k}\Omega\) resistor (center node) be \(V_B\). By nodal analysis:
\[
\frac{V_B - V_1}{10k} + \frac{V_B - V_2}{20k} + \frac{V_B}{60k} = 0 .
\]
Multiplying by \(60k\) gives
\[
6(V_B - V_1) + 3(V_B - V_2) + V_B = 0
\Rightarrow 10V_B - 6V_1 - 3V_2 = 0.
\]
Hence,
\[
V_B = \frac{6}{10}V_1 + \frac{3}{10}V_2 = 0.3(2V_1 + V_2).
\]
Step 2: The power in the \(60\,\text{k}\Omega\) resistor is \(P = \dfrac{V_B^2}{60k}\), which is proportional to \(V_B^2\). Therefore,
\[
P \propto \big(0.3(2V_1+V_2)\big)^2 \propto (2V_1+V_2)^2.
\]
Thus, the required proportional expression is \(\boxed{(2V_1+V_2)^2}\).