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Mechanics of Fluids

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168 Physical similarity and dimensional analysis<br />

from fluid motion. These can be broadly classified as pressure coefficients,<br />

force coefficients and friction coefficients, respectively. Amongst the force<br />

coefficients are the lift and drag coefficients, <strong>of</strong> fundamental importance<br />

in aircraft aerodynamics. The friction coefficients include amongst their<br />

number the friction factor associated with pipe flow, and the skin friction<br />

coefficient used to describe in a dimensionless form the surface shear stresses<br />

<strong>of</strong> external fluid flow. Examples <strong>of</strong> dimensionless groups which fall outside<br />

these named categories are the Strouhal number, which arises in the treatment<br />

<strong>of</strong> cyclical phenomena, and the mass flow parameter, which is a useful<br />

concept when dealing with compressible flows in pipes. Apart from the pressure<br />

coefficients, which will be discussed explicitly, albeit briefly, all other<br />

dimensionless groups will be considered as they arise.<br />

5.5.1 The pressure coefficient and related coefficients<br />

Pressure forces are always present and are therefore represented in any<br />

complete description <strong>of</strong> fluid flow. When expressed in dimensionless form,<br />

the ratio <strong>of</strong> pressure forces to other types <strong>of</strong> forces appears. For example,<br />

the ratio<br />

|Pressure force|<br />

|Inertia force|<br />

is proportional to �p∗l2 ϱl2 �p∗<br />

=<br />

u2 ϱu2 where �p∗ represents the difference in piezometric pressure between two<br />

points in the flow. In fluid dynamics, it has become normal practice to use<br />

the ratio �p∗ / 1<br />

2ϱu2 , the 1<br />

2 being inserted so that the denominator represents<br />

kinetic energy divided by volume or, for an incompressible fluid, the dynamic<br />

pressure <strong>of</strong> the stream (see Section 3.7.1). This latter form is usually known<br />

as the pressure coefficient, denoted by the symbol Cp.<br />

Several other similar coefficients are, in essence, variants <strong>of</strong> the pressure<br />

coefficient. Amongst these are the static and total pressure loss coefficients,<br />

widely used to describe the dissipation <strong>of</strong> mechanical energy that occurs in<br />

internal fluid flows, and the pressure recovery coefficient more specifically<br />

used to describe the properties <strong>of</strong> diffusers. Also in this category are the<br />

corresponding head loss coefficients.<br />

5.5.2 The discharge coefficient<br />

The discharge coefficient is an important dimensionless parameter which<br />

relates the flow rate through a differential-pressure flow-metering device,<br />

such as an orifice plate, nozzle or venturi tube, to the pressure distribution<br />

the flow generates. It was first introduced in Chapter 3, where it was<br />

used to adjust theoretical values <strong>of</strong> mass flow rate (or volumetric flow rate),<br />

derived from simplistic mathematical models <strong>of</strong> fluid motion which ignored<br />

the effects <strong>of</strong> viscosity, to yield improved comparisons with the behaviour<br />

<strong>of</strong> real flows. The method <strong>of</strong> dimensional analysis provides a more rigorous<br />

justification for the use <strong>of</strong> the discharge coefficient, since, from the outset,<br />

the analysis takes full account <strong>of</strong> the viscous nature <strong>of</strong> real fluids.

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