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Match the following

P: Compressible flow

U: Reynolds number

Q: Free surface flow

V: Nusselt number

R: Boundary layer flow

W: Weber number

S: Pipe flow

X: Froude number

T: Heat convection

Y: Mach number

 

Z: Skin friction coefficient


1. P-U; Q-X; R-V; S-Z; T-W
2. P-W; Q-X; R-Z; S-U; T-V
3. P-Y; Q-W; R-Z; S-U; T-X
4. P-Y; Q-X; R-Z; S-U; T-V

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Best answer
Correct Answer - Option 4 : P-Y; Q-X; R-Z; S-U; T-V

Concept:

\({\rm{Mach\;Number}} = \frac{{Inertia\;force}}{{elastic\;force}} = \frac{{Inertia\;force}}{{Compressible\;force}}\)

Incompressible flow

  • M < 0.3
  • From the above point, it is clear that the compressibility effect can be treated as negligible when the Mach number is up to 0.2

 

Subsonic flow

0.3 < M < 1

Sonic flow

M = 1

Supersonic flow

1 < M < 5

Hypersonic flow

M > 5

 

Froude number

Froude number is the ratio of inertial force to the gravitation force.

\(\text{Froude }{ number}=\text{ }\!\!~\!\!\text{ }{\frac{\text{Inertia force }\!\!~\!\!\text{ }}{\text{Gravitational force }\!\!~\!\!\text{ }}}\)

Froude number has the following applications:

  • Used in cases of river flows, open-channel flows, spillways, surface wave motion created by boats
  • It can be used for flow classification

Skin friction coefficient

Skin friction drag is a component of profile drag that occurs differently depending on the type of flow over the lifting body

The local Skin friction coefficient for the boundary layer over a flat plate is given as

\({C_{fx}} = \frac{{0.664}}{{\sqrt {R{e_x}} }}\)

Reynolds number

Reynolds number is a dimensionless formula that is used to differentiate laminar flow from the turbulent flow.

Reynolds number is given by \(Re = \frac{{\rho \times V \times D}}{\mu }\)

In the case of pipe flow,

  • If Re ≤ 2000 then flow is laminar
  • 2000 ≤ Re ≤ 4000 then flow is transitional
  • Re ≥ 4000 then flow is turbulent

Nusselt number

It is the ratio of heat flow rate by convection process to the heat flow rate by the conduction process.

\(Nu = \frac{{{Q_{conv}}}}{{{Q_{cond}}}} = \frac{{hA{\rm{\Delta }}T}}{{\frac{{kA{\rm{\Delta }}T}}{L}}} = \frac{{hL}}{k}\)

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