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Basics of Fluid Mechanics, 2014a

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9.4. SUMMARY OF DIMENSIONLESS NUMBERS 317<br />

In this analysis, it is assumed that pressure is uniform in the cross section. This<br />

assumption is appropriate because only the secondary flows in the radial direction (to<br />

be discussed in this book section on pumps.). Hence, the ratio <strong>of</strong> power between the<br />

two pump can be written as<br />

Ẇ p<br />

= (PAU) p<br />

(9.XX.h)<br />

Ẇ m (P AU) m<br />

Utilizing equations above in this ratio leads to<br />

P p /P m<br />

A p /A m<br />

{ }} { { }} {<br />

( ) 2 ( ) { 2<br />

Ẇ p Dp Dp<br />

=<br />

Ẇ m D m D m<br />

U p /U m<br />

(<br />

Dp<br />

}} ) {<br />

=<br />

D m<br />

(<br />

Dp<br />

D m<br />

) 5<br />

(9.XX.i)<br />

End Solution<br />

Example 9.21:<br />

The flow resistance to flow <strong>of</strong> the water in a pipe is to be simulated by flow <strong>of</strong> air.<br />

Estimate the pressure loss ratio if Reynolds number remains constant. This kind <strong>of</strong> study<br />

appears in the industry in which the compressibility <strong>of</strong> the air is ignored. However, the<br />

air is a compressible substance that flows the ideal gas model. Water is a substance that<br />

can be considered incompressible flow for relatively small pressure change. Estimate the<br />

error using the averaged properties <strong>of</strong> the air.<br />

Solution<br />

For the first part, the Reynolds number is the single controlling parameter which affects<br />

the pressure loss. Thus it can be written that the Euler number is function <strong>of</strong> the<br />

Reynolds number.<br />

Eu = f(Re)<br />

(9.XXI.a)<br />

Thus, to have a similar situation the Reynolds and Euler have to be same.<br />

Re p = Re m Eu m = Eu p (9.XXI.b)<br />

Hence,<br />

U m<br />

U p<br />

and for Euler number<br />

ΔP m<br />

ΔP p<br />

and utilizing equation (9.XXI.c) yields<br />

= l p ρ μ p<br />

l m ρ m μ m<br />

= ρ m<br />

ρ p<br />

U m<br />

U p<br />

( ) 2 ( ) 2 ( )<br />

ΔP m lp μm ρp<br />

=<br />

ΔP p l m μ p ρ m<br />

(9.XXI.c)<br />

(9.XXI.d)<br />

(9.XXI.e)

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