Step 1: Identify the type of fluid motion.
Fluid motion can be categorized by how smoothly the fluid particles move.
In laminar flow, the fluid travels in well-defined, parallel layers, and there is no intermixing between adjacent layers.
Step 2: Introduce Reynolds number.
The nature of flow is commonly determined using the Reynolds number, a dimensionless parameter defined as:
\[ Re = \frac{\rho v D}{\mu} \]
where:
Step 3: Classify flow regimes in a pipe.
For flow through a circular pipe, experimental observations give the following ranges:
Since the question asks specifically about laminar flow, we focus on the region where viscous forces dominate and the motion remains stable.
Step 4: Final conclusion.
Fluid flow is considered laminar when the Reynolds number is:
\[ \boxed{Re < 2000} \]
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). 
Consider a velocity field \( \vec{V} = 3z \hat{i} + 0 \hat{j} + Cx \hat{k} \), where \( C \) is a constant. If the flow is irrotational, the value of \( C \) is (rounded off to 1 decimal place).