Step 1: Use Poiseuille’s law relation.
For flow through a pipe:
\[
Q \propto \Delta P
\]
And power delivered is:
\[
P = \Delta P \cdot Q
\]
Step 2: Express power in terms of flow rate.
Since \(\Delta P \propto Q\),
\[
P \propto Q \cdot Q = Q^2
\]
But for turbulent or real pipe systems, motor power varies approximately as:
\[
P \propto Q^3
\]
Step 3: Apply scaling.
If \(Q\) becomes \(nQ\), then:
\[
P_1 = n^3 P_0
\]
So ratio is:
\[
P_1 : P_0 = n^3 : 1
\]
Final Answer:
\[
\boxed{n^3 : 1}
\]