The continuum approach in fluid mechanics assumes that fluid properties such as density, pressure, and temperature vary smoothly and continuously throughout the flow. This approximation is valid when the mean free path of the molecules, which is the average distance a molecule travels before colliding with another molecule, is much smaller than the smallest significant length scale in the problem.
However, when the mean free path becomes comparable to the smallest significant length scale, the continuum assumption breaks down. This is because the fluid can no longer be accurately described as a continuous medium. In such cases, molecular effects become significant and must be accounted for using methods like statistical mechanics or molecular dynamics.
Therefore, the continuum approach breaks down when the mean free path of the molecules is:
Consider two identical tanks with a bottom hole of diameter \( d \). One tank is filled with water and the other tank is filled with engine oil. The height of the fluid column \( h \) is the same in both cases. The fluid exit velocity in the two tanks are \( V_1 \) and \( V_2 \). Neglecting all losses, which one of the following options is correct?

A pitot tube connected to a U-tube mercury manometer measures the speed of air flowing in the wind tunnel as shown in the figure below. The density of air is 1.23 kg m\(^{-3}\) while the density of water is 1000 kg m\(^{-3}\). For the manometer reading of \( h = 30 \) mm of mercury, the speed of air in the wind tunnel is _________ m s\(^{-1}\) (rounded off to 1 decimal place). 