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Mechanics of Fluids

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54 Fluid statics<br />

Micro-manometers<br />

for a small value <strong>of</strong> p ∗ 1 − p∗ 2<br />

The interface between liquids <strong>of</strong> closely similar<br />

densities, however is very sensitive to changes in surface tension and therefore<br />

to traces <strong>of</strong> grease and other impurities. Air may be used as fluid B: it may<br />

be pumped through the valve V at the top <strong>of</strong> the manometer until the liquid<br />

menisci are at a suitable level. Then, <strong>of</strong> course, ϱB is negligible compared<br />

with ϱA.<br />

Certain practical considerations arise in the use <strong>of</strong> manometers. (1) Since<br />

the densities <strong>of</strong> liquids depend on temperature the temperature <strong>of</strong> the liquids<br />

should be known for accurate results. (2) Some liquids, otherwise suitable<br />

for use in manometers, give ill-defined menisci. (3) Fluctuations <strong>of</strong> menisci<br />

reduce accuracy; such movements may be reduced by restrictions in the<br />

manometer connections (e.g. lengths <strong>of</strong> small-diameter pipe) which, under<br />

equilibrium conditions, do not affect the pressure. (4) The density <strong>of</strong> the<br />

fluid in the connecting tubes must be uniform; for example, water must not<br />

contain air bubbles, nor must air contain ‘blobs’ <strong>of</strong> water. The layout <strong>of</strong><br />

the connecting tubes should be such as to minimize the possibility <strong>of</strong> trapping<br />

air bubbles, and means should be provided for flushing the connecting<br />

tubes through before the manometer is used. A valve by which the pressure<br />

difference may be reduced to zero and the zero reading thus checked<br />

is also desirable. (5) In tubes <strong>of</strong> less than about 15 mm diameter surface<br />

tension effects may be appreciable and the meniscus is either raised above<br />

or lowered below its ‘correct’ position. For example, for pure water in a<br />

clean, vertical, glass tube, 6 mm diameter, the capillary rise is about 5 mm.<br />

The corresponding depression for mercury is about 1.25 mm. Because <strong>of</strong><br />

the uncertain degree <strong>of</strong> cleanliness <strong>of</strong> tubes used in practice, however, it is<br />

difficult to allow for surface tension effects. Fortunately these effects can be<br />

nullified, for example in a U-tube manometer where the limbs are <strong>of</strong> equal<br />

diameter and cleanliness, or where measurements are made <strong>of</strong> the movement<br />

<strong>of</strong> a single meniscus in a uniform tube. Alcohol, being a solvent <strong>of</strong> grease, is<br />

less sensitive to the cleanliness <strong>of</strong> the tube and so is frequently preferred to<br />

water in manometers.<br />

For measuring very small pressure differences, a wide variety <strong>of</strong> special<br />

manometers has been developed. Several devices may be used to increase<br />

the accuracy <strong>of</strong> a reading. For example, a meniscus may be observed<br />

through a small telescope containing a horizontal cross-wire, and the<br />

assembly may be raised or lowered by a slow-motion screw with a micrometer<br />

scale. Or a scale floating on the surface <strong>of</strong> a liquid may be optically<br />

magnified.<br />

When an additional gauge liquid is used in a U-tube a large difference<br />

<strong>of</strong> meniscus level may be produced by a small pressure difference.<br />

One arrangement is illustrated in Fig. 2.11. The appropriate equilibrium<br />

equation is<br />

�<br />

p1 + ϱAg(h + �z) + ϱBg z − �z + y<br />

�<br />

2<br />

�<br />

= p2 + ϱAg(h − �z) + ϱBg z + �z − y<br />

�<br />

+ ϱCgy (2.10)<br />

2

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