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MECHANICS of FLUIDS LABORATORY - Mechanical Engineering

MECHANICS of FLUIDS LABORATORY - Mechanical Engineering

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actual flow rate (measured in the laboratory).<br />

The ratio <strong>of</strong> actual to theoretical flow rate leads<br />

to the definition <strong>of</strong> a discharge coefficient: C o<br />

for<br />

the orifice meter and C n<br />

for the nozzle.<br />

rotor supported<br />

on bearings<br />

(not shown)<br />

to receiver<br />

h<br />

1 2<br />

flow<br />

straighteners<br />

turbine rotor<br />

rotational speed<br />

proportional to<br />

flow rate<br />

FIGURE 7.4. A schematic <strong>of</strong> a turbine-type flow<br />

meter.<br />

FIGURE 7.2. Cross sectional view <strong>of</strong> the orifice<br />

meter.<br />

h<br />

1 2<br />

FIGURE 7.3. Cross sectional view <strong>of</strong> the nozzletype<br />

meter, and a typical nozzle.<br />

For each and every measured actual flow<br />

rate through the orifice or nozzle-type meters, it<br />

is possible to calculate a theoretical volume flow<br />

rate, a Reynolds number and a discharge<br />

coefficient. The Reynolds number is given by<br />

Equation 7.2.<br />

The Turbine-Type Meter<br />

The turbine-type flow meter consists <strong>of</strong> a<br />

section <strong>of</strong> pipe into which a small “turbine” has<br />

been placed. As the fluid travels through the<br />

pipe, the turbine spins at an angular velocity<br />

that is proportional to the flow rate. After a<br />

certain number <strong>of</strong> revolutions, a magnetic pickup<br />

sends an electrical pulse to a preamplifier which<br />

in turn sends the pulse to a digital totalizer. The<br />

totalizer totals the pulses and translates them<br />

into a digital readout which gives the total<br />

volume <strong>of</strong> liquid that travels through the pipe<br />

and/or the instantaneous volume flow rate.<br />

Figure 7.4 is a schematic <strong>of</strong> the turbine type flow<br />

meter.<br />

The Rotameter (Variable Area Meter)<br />

The variable area meter consists <strong>of</strong> a tapered<br />

metering tube and a float which is free to move<br />

inside. The tube is mounted vertically with the<br />

inlet at the bottom. Fluid entering the bottom<br />

raises the float until the forces <strong>of</strong> buoyancy, drag<br />

and gravity are balanced. As the float rises the<br />

annular flow area around the float increases.<br />

Flow rate is indicated by the float position read<br />

against the graduated scale which is etched on<br />

the metering tube. The reading is made usually at<br />

the widest part <strong>of</strong> the float. Figure 7.5 is a sketch<br />

<strong>of</strong> a rotameter.<br />

freely<br />

suspended<br />

float<br />

outlet<br />

tapered, graduated<br />

transparent tube<br />

inlet<br />

FIGURE 7.5. A schematic <strong>of</strong> the rotameter and its<br />

operation.<br />

Rotameters are usually manufactured with<br />

one <strong>of</strong> three types <strong>of</strong> graduated scales:<br />

1. % <strong>of</strong> maximum flow–a factor to convert scale<br />

reading to flow rate is given or determined for<br />

the meter. A variety <strong>of</strong> fluids can be used<br />

with the meter and the only variable<br />

19

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