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Mechanics of Fluids

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in eqn 6.24 we obtain<br />

�<br />

D<br />

Vp<br />

2<br />

�<br />

+ c = c3<br />

�<br />

F + W<br />

6µl πD2 �<br />

− ρgl<br />

/4<br />

Steady laminar flow between moving planes 209<br />

(6.26)<br />

The clearance c is normally small compared with the radius <strong>of</strong> the piston D/2,<br />

so the left-hand side <strong>of</strong> eqn 6.26 may be simplified to VpD/2. Rearrangement<br />

then gives<br />

F + W − ρglπD 2 /4 = 3<br />

4 πµl<br />

� �3 D<br />

Vp<br />

(6.27)<br />

c<br />

The term ρglπD 2 /4 represents the buoyancy <strong>of</strong> the piston, and in some<br />

instances this is negligible compared with F. This, however, is not always so<br />

and the buoyancy term should not be omitted without investigation.<br />

For upward movement <strong>of</strong> the piston the signs <strong>of</strong> F and Vp are <strong>of</strong> course<br />

changed.<br />

Equation 6.27 is a formula commonly used, but even for steady conditions<br />

it is only approximate. The clearance c has been assumed small in comparison<br />

with the radius <strong>of</strong> the piston; the shear force on the piston has been<br />

neglected; the circumferences <strong>of</strong> piston and cylinder are not exactly equal;<br />

end effects have been neglected. It may be shown, however, that the accuracy<br />

is much improved if the mean diameter 2(D/2 + c/2) = (D + c) is used in<br />

eqn 6.27 in place <strong>of</strong> the piston diameter D.<br />

In a dashpot <strong>of</strong> this kind the piston has to be maintained concentric with<br />

the cylinder by external means. If it is free to move laterally the piston tends<br />

to move to one side <strong>of</strong> the cylinder and, having once touched the side <strong>of</strong> the<br />

cylinder, is reluctant to leave it. Under such conditions the relation between<br />

the load on the piston and the rate at which oil flows through the clearance<br />

space is drastically altered and the effectiveness <strong>of</strong> the dashpot in restraining<br />

the movement <strong>of</strong> the piston is greatly reduced. Three buttons, equally spaced<br />

round the circumference <strong>of</strong> the piston, are sometimes used to maintain its<br />

concentricity with the cylinder.<br />

Many other forms <strong>of</strong> dashpot are in use, but an account <strong>of</strong> these is beyond<br />

the scope <strong>of</strong> this book.<br />

Example 6.4 A simple dashpot consists <strong>of</strong> a piston <strong>of</strong> diameter<br />

50 mm and length 130 mm positioned concentrically in a cylinder <strong>of</strong><br />

50.4 mm diameter. If the dashpot contains oil <strong>of</strong> specific gravity 0.87<br />

and kinematic viscosity 10 −4 m 2 · s −1 , determine the velocity <strong>of</strong> the<br />

dashpot if the difference in pressures �p ∗ is 1.4 MPa.<br />

Solution<br />

Clearance: c = (50.4 − 50)/2 = 0.2 mm<br />

Dynamic viscosity:<br />

µ = ρν = (0.87 × 10 3 ) kg · m −3 × 10 −4 m 2 · s −1<br />

= 0.087 kg · m −1 · s −1

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