Step 1: Use Reynolds number similarity.
For flow similarity, the Reynolds numbers for the model and the full-scale object must be the same. Reynolds number is given by:
\[
Re = \frac{\rho v D}{\mu},
\]
where \(\rho\) is density, \(v\) is velocity, \(D\) is diameter, and \(\mu\) is dynamic viscosity.
Step 2: Apply flow similarity.
For geometrically similar objects, the drag force ratio between the full scale and model is proportional to the Reynolds number ratio. For the model and full-scale object, the drag force \(F_d\) is related to the Reynolds number ratio as:
\[
\frac{F_{d,\text{full scale}}}{F_{d,\text{model}}} = \left( \frac{\rho_{\text{full scale}} \cdot v_{\text{full scale}} \cdot D_{\text{full scale}}}{\mu_{\text{full scale}}} \right) \div \left( \frac{\rho_{\text{model}} \cdot v_{\text{model}} \cdot D_{\text{model}}}{\mu_{\text{model}}} \right).
\]
Using the values provided, we calculate the drag for the full-scale object to be 644 N.