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handbook of modern sensors

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360 11 Flow Sensors<br />

(A)<br />

(B)<br />

Fig. 11.1. Tube <strong>of</strong> flow (A) and flow <strong>of</strong> a medium through a plane (B).<br />

Fig. 11.2. Pr<strong>of</strong>ile <strong>of</strong> the velocity <strong>of</strong> flow in a pipe.<br />

where v is the velocity <strong>of</strong> moving medium, which must be integrated over area A,<br />

and x is the displacement <strong>of</strong> volume V . Figure 11.2 shows that the velocity <strong>of</strong> a<br />

liquid or gas in a pipe may vary over the cross section. It is <strong>of</strong>ten convenient to define<br />

an average velocity<br />

∫<br />

vdA<br />

v a =<br />

A . (11.3)<br />

When measuring the velocity by a sensor whose dimensions are substantially<br />

smaller than the pipe size, one should be aware <strong>of</strong> the possibility <strong>of</strong> erroneous detection<br />

<strong>of</strong> either too low or too high velocity, whereas the average velocity, v a , is somewhere<br />

in between. A product <strong>of</strong> the average velocity and a cross-sectional area is called the<br />

flux or flow rate. Its SI unit is cubic meters per second. The U.S. Customary System<br />

unit is cubic feet per second. The flux can be found by rearranging Eq. (11.3):<br />

∫<br />

Av a = vdA. (11.4)<br />

What a flow sensor usually measures is v a . Thus, to determine the flow rate, the<br />

cross-section area <strong>of</strong> tube <strong>of</strong> flow A must be known, otherwise the measurement is<br />

meaningless.

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