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Mechanics of Fluids

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592 Fluid machines<br />

derives essentially from changes <strong>of</strong> the volume occupied by the fluid within<br />

the machine. This type is most commonly exemplified by those machines,<br />

such as reciprocating pumps and engines, in which a piston moves to and fro<br />

in a cylinder (a suitable arrangement <strong>of</strong> valves ensures that the fluid always<br />

moves in the direction appropriate to either a pump or an engine). Also in this<br />

category are diaphragm pumps, in which the change <strong>of</strong> volume is brought<br />

about by the deformation <strong>of</strong> flexible boundary surfaces (an animal heart is an<br />

example <strong>of</strong> this form <strong>of</strong> pump), and gear pumps in which two rotors similar<br />

to gear wheels mesh together within a close-fitting housing. Although hydrodynamic<br />

effects may be associated with a positive-displacement machine, the<br />

operation <strong>of</strong> the machine itself depends only on mechanical and hydrostatic<br />

principles. This is not to say that such a machine is easy to design, but since<br />

few principles <strong>of</strong> the mechanics <strong>of</strong> fluids are involved our consideration <strong>of</strong><br />

positive-displacement machines in this book will be very brief.<br />

13.1.4 Rotodynamic machines<br />

All rotodynamic machines have a rotor, that is, a rotating part through<br />

which the fluid passes. In a turbine this rotor is called the runner, for a<br />

pump the term impeller is more <strong>of</strong>ten used. The fluid has a component <strong>of</strong><br />

velocity and therefore <strong>of</strong> momentum in a direction tangential to the rotor,<br />

and the rate at which this tangential momentum is changed corresponds<br />

to a tangential force on the rotor. In a turbine there is a reduction <strong>of</strong> the<br />

tangential momentum <strong>of</strong> the fluid in the direction <strong>of</strong> movement <strong>of</strong> the rotor;<br />

thus energy is transferred from the fluid to the rotor and hence to the output<br />

shaft. In a pump, energy from the rotor is used to increase the tangential<br />

momentum <strong>of</strong> the fluid; subsequent deceleration <strong>of</strong> the fluid produces a rise<br />

in pressure.<br />

Rotodynamic machines have several advantages over the positivedisplacement<br />

type. The flow from most positive-displacement machines is<br />

unsteady whereas, for normal conditions <strong>of</strong> operation, that from a rotodynamic<br />

machine is essentially steady. Most positive-displacement machines<br />

require small clearances between moving and stationary parts, and so are<br />

unsuited to handling fluids containing solid particles; in general, rotodynamic<br />

machines are not restricted in this way. If discharge from a<br />

positive-displacement pump is prevented – for example, by the closing <strong>of</strong><br />

a valve – the pressure within the pump rises and either the pump stops or<br />

some part <strong>of</strong> the casing bursts; if the discharge valve <strong>of</strong> a rotodynamic pump<br />

is closed, however, the rotating impeller merely churns the fluid round, and<br />

the energy consumed is converted to heat. Moreover, for dealing with a given<br />

overall rate <strong>of</strong> flow a rotodynamic machine is usually less bulky than one <strong>of</strong><br />

positive-displacement type.<br />

13.2 RECIPROCATING PUMPS<br />

From the point <strong>of</strong> view <strong>of</strong> mechanics <strong>of</strong> fluids a positive-displacement<br />

machine holds interest principally because <strong>of</strong> the unsteady nature <strong>of</strong> the

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