Concept:
From Buckingham’s π – theorem,
\(\frac{F}{{\rho {U^2}{D^2}}} = \phi \left( {\frac{{\rho UD}}{\mu }} \right) = \phi \left( {Re} \right) = {C_F}\)
For dynamic similarity, Re1 = Re2
\(\frac{{{\rho _1}{U_1}{D_1}}}{{{\mu _1}}} = \frac{{{\rho _2}{U_2}{D_2}}}{{{\mu _2}}};\;{\rho _1} = {{\rm{\rho }}_2}\;\& \;{\mu _1} = {\mu _2}\)
U1D1 = U2D2
2 × 100 = U2 × 200
U2 = 1 m/s
\(\frac{{{F_1}}}{{{\rho _1}U_1^2D_1^2}} = \frac{{{F_2}}}{{{\rho _2}U_2^2D_2^2}} \Rightarrow \frac{{{F_1}}}{{U_1^2D_1^2}} = \frac{{{F_2}}}{{U_2^2D_2^2}} \Rightarrow \frac{{{F_1}}}{{{2^2} \times {{100}^2}}} = \frac{{{F_2}}}{{{1^2} \times {{200}^2}}}\)
F1 = F2
\({F_1} = {C_F} ~\rho _1U_1^2D_1^2 = 0.5 \times 1000 \times {2^2} \times {\left( {0.1} \right)^2}\)
F1 = 20 N ⇒ F2 = 20 N
Drag force on second sphere of 200 mm diameter is 20 N