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Mechanics of Fluids

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28 Fundamental concepts<br />

rate <strong>of</strong> shear is (1/G)∂τ/∂t so the total rate <strong>of</strong> shear in the material is<br />

(τ/µ) + (1/G)∂τ/∂t.<br />

The fluids with which engineers most <strong>of</strong>ten have to deal are Newtonian,<br />

that is, their viscosity is not dependent on either the rate <strong>of</strong> shear or its<br />

duration, and the term mechanics <strong>of</strong> fluids is generally regarded as referring<br />

only to Newtonian fluids. The study <strong>of</strong> non-Newtonian liquids is termed<br />

rheology.<br />

1.6.6 Inviscid fluid<br />

An important field <strong>of</strong> theoretical fluid mechanics involves the investigation<br />

<strong>of</strong> the motion <strong>of</strong> a hypothetical fluid having zero viscosity. Such a fluid is<br />

sometimes referred to as an ideal fluid. Although commonly adopted in the<br />

past, the use <strong>of</strong> this term is now discouraged as imprecise. A more meaningful<br />

term for a fluid <strong>of</strong> zero viscosity is inviscid fluid.<br />

1.7 SURFACE TENSION<br />

Surface tension arises from the forces between the molecules <strong>of</strong> a liquid and<br />

the forces (generally <strong>of</strong> a different magnitude) between the liquid molecules<br />

and those <strong>of</strong> any adjacent substance. The symbol for surface tension is γ and<br />

it has the dimensions [MT −2 ].<br />

Water in contact with air has a surface tension <strong>of</strong> about 0.073 N · m −1 at<br />

usual ambient temperatures; most organic liquids have values between 0.020<br />

and 0.030 N · m −1 and mercury about 0.48 N · m −1 , the liquid in each case<br />

being in contact with air. For all liquids the surface tension decreases as<br />

the temperature rises. The surface tension <strong>of</strong> water may be considerably<br />

reduced by the addition <strong>of</strong> small quantities <strong>of</strong> organic solutes such as soap<br />

and detergents. Salts such as sodium chloride in solution raise the surface<br />

tension <strong>of</strong> water. That tension which exists in the surface separating two<br />

immiscible liquids is usually known as interfacial tension.<br />

As a consequence <strong>of</strong> surface tension effects a drop <strong>of</strong> liquid, free from all<br />

other forces, takes on a spherical form.<br />

The molecules <strong>of</strong> a liquid are bound to one another by forces <strong>of</strong> molecular<br />

attraction, and it is these forces that give rise to cohesion, that is, the tendency<br />

<strong>of</strong> the liquid to remain as one assemblage <strong>of</strong> particles rather than to behave<br />

as a gas and fill the entire space within which it is confined. Forces between<br />

the molecules <strong>of</strong> a fluid and the molecules <strong>of</strong> a solid boundary surface give<br />

rise to adhesion between the fluid and the boundary.<br />

If the forces <strong>of</strong> adhesion between the molecules <strong>of</strong> a particular liquid and<br />

a particular solid are greater than the forces <strong>of</strong> cohesion among the liquid<br />

molecules themselves, the liquid molecules tend to crowd towards the solid<br />

surface, and the area <strong>of</strong> contact between liquid and solid tends to increase.<br />

Given the opportunity, the liquid then spreads over the solid surface and<br />

‘wets’ it. Water will wet clean glass, but mercury will not. Water, however,<br />

will not wet wax or a greasy surface.

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