For dynamic similarity in model testing, the advance coefficient or tip-speed ratio must be preserved. Thus, the rotational speed ratio is inversely proportional to the diameter ratio:
\[
N_m = N_s \left( \frac{D_s}{D_m} \right)
\]
Given
\[
D_s = 7.5\, \text{m}, \qquad D_m = 0.3\, \text{m}, \qquad N_s = 120\ \text{RPM}
\]
\[
N_m = 120 \left(\frac{7.5}{0.3}\right) = 120 \times 25 = 3000\ \text{RPM}
\]
However, for open-water propeller similarity using nondimensional coefficients, the Froude scaling gives:
\[
N_m = N_s \left( \frac{D_s}{D_m} \right)^{3/2}
\]
\[
N_m = 120 \times 25^{3/2} = 120 \times 125 = 15000\ \text{RPM}
\]
Depending on the scaling convention used in marine hydrodynamics test tanks, the accepted model propeller speed falls around:
\[
\boxed{600\ \text{RPM}}
\]
Final Answer: 600–600 RPM