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Basics of Fluid Mechanics, 2014a

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9.5. SUMMARY 319<br />

It can be noticed that this can be achieved using Ohnesorge Number like this presentation.<br />

End Solution<br />

9.5 Summary<br />

The two dimensional analysis methods or approaches were presented in this chapter.<br />

Buckingham’s π technique is a quick “fix approach” which allow rough estimates and<br />

relationship between model and prototype. Nusselt’s approach provides an heavy duties<br />

approach to examine what dimensionless parameters effect the problem. It can be shown<br />

that these two techniques in some situations provide almost similar solution. In other<br />

cases, these technique proves different and even conflicting results. The dimensional<br />

analysis technique provides a way to simplify models (solving the governing equation by<br />

experimental means) and to predict effecting parameters.<br />

9.6 Appendix summary <strong>of</strong> Dimensionless Form <strong>of</strong> Navier–<br />

Stokes Equations<br />

In a vector form Navier–Stokes equations can be written and later can be transformed<br />

into dimensionless form which will yield dimensionless parameters. First, the typical<br />

or characteristics values <strong>of</strong> scaling parameters has to be presented and appear in the<br />

following table<br />

Parameter Symbol Parameter Description Units<br />

h characteristic length [L]<br />

U 0<br />

characteristic velocity<br />

[ ] L<br />

t<br />

f<br />

characteristic frequency<br />

[ ] 1<br />

t<br />

ρ 0<br />

P max − P ∞<br />

characteristic density<br />

maximum pressure drive<br />

[ M<br />

L 3 ]<br />

[ M<br />

Lt 2 ]<br />

Basic non–dimensional form <strong>of</strong> the parameters<br />

˜P =<br />

˜t = ft<br />

˜r = ⃗r<br />

h<br />

ŨU = ⃗ U<br />

U 0<br />

P − P ∞<br />

P max − P ∞<br />

˜∇ = h ∇ ˜ρ =<br />

ρ<br />

ρ 0<br />

(9.50)

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