The Reynold’s number, used for critical velocity for turbulent flow of fluids, is given by the relation
The Reynolds number (Re) is a dimensionless quantity that helps predict flow patterns in different fluid flow situations. It is a crucial parameter in fluid dynamics, especially for determining when flow transitions from laminar to turbulent, or for characterizing fully turbulent flow. The question specifically mentions its use for critical velocity for turbulent flow of fluids.
The Reynolds number is fundamentally a ratio that compares the inertial forces to the viscous forces within a fluid. This ratio helps to characterize the relative importance of these two types of forces for given flow conditions.
It is expressed mathematically as:
\(\text{Re} = \dfrac{\rho u L}{\mu}\)
Where:
Alternatively, it can also be expressed using kinematic viscosity (\(\nu = \mu/\rho\)):
\(\text{Re} = \dfrac{u L}{\nu}\)
In fluid dynamics, two primary forces are often considered when analyzing the nature of flow, especially concerning the Reynolds number:
The Reynolds number is defined as the ratio of these two fundamental forces:
\(\text{Reynolds Number} = \dfrac{\text{Inertia Force}}{\text{Viscous Force}}\)
Let's consider why this ratio is so important for turbulent flow and critical velocity:
The transition from laminar to turbulent flow occurs at a specific range of Reynolds numbers, known as the critical Reynolds number, which corresponds to the critical velocity for a given system.
Let's evaluate the given options based on our understanding of the Reynolds number:
| Option | Analysis |
|---|---|
| \(\rm \dfrac{Pressure\;head}{Viscous \;force}\) | This ratio is not the definition of the Reynolds number. While pressure head is important in fluid flow, it is not part of the fundamental definition comparing inertia and viscous forces. |
| \(\rm \dfrac{Viscous \;force}{Mass\;density}\) | This ratio does not represent a dimensionless number like the Reynolds number, nor does it correctly relate the key forces involved in flow regimes. |
| \(\rm \dfrac{Viscous \;force}{Pressure\;head}\) | Similar to option 1, this ratio does not define the Reynolds number. It involves forces and pressure, but not in the standard dimensionless form for flow characterization. |
| \(\rm \dfrac{Inertia\;force}{Viscous \;force}\) | This option correctly represents the definition of the Reynolds number. It is the ratio of inertia force to viscous force, which determines the flow regime (laminar, transitional, or turbulent flow) and is directly linked to the concept of critical velocity. |
Therefore, the relation defining the Reynolds number for characterizing turbulent flow and critical velocity is the ratio of Inertia force to Viscous force.
Match the following and select the correct answer from the codes given below the lists
List I | List II | ||
A. | Steam Nozzle | 1. | Mach number |
B. | Compressible flow | 2. | Reaction turbine |
C. | Surface Tension | 3. | Biot number |
D. | Heat conduction | 4. | Nusselt number |
5. | Supersaturation | ||
6. | Weber number | ||
Reynolds number for non - circular cross-section is:
[V = mean velocity, ν = kinematic viscosity, P = ratio of cross-sectional area to the wetted perimeter]
A) \(V.\frac{{4P}}{v}\)
B) \(\frac{{V.P}}{v}\)
C) \(\frac{{V.2P}}{{4v}}\)
D) \(\frac{{V.P}}{{4v}}\)
When the Mach number is less than unity, the flow is
The only possible dimensionless group that combines velocity ‘V’, body size ‘L’, fluid density ‘ρ’ & surface tension ‘σ’