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handbook of modern sensors

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11.9 Drag Force Flow Sensors 377<br />

With a no-flow state, the tube vibrates identically at its inlet and outlet sides with<br />

the sine-wave motions with the zero phase shift between them. During flow, the tube<br />

twists in response to the flow, and the inlet and outlet sides vibrate differently with a<br />

phase shift between them (Fig. 11.17C). The main disadvantage <strong>of</strong> the Coriolis sensor<br />

its relatively high initial cost. However, the versatility <strong>of</strong> Coriolis <strong>sensors</strong> in handling<br />

multiple fluids makes them very useful for plants where the flow <strong>of</strong> multiple fluid<br />

types must be measured. There are also an increasing number <strong>of</strong> the gas applications<br />

for the Coriolis meters.<br />

11.9 Drag Force Flow Sensors<br />

When fluid motion is sporadic, multidirectional, and turbulent, a drag force flow<br />

sensor may be quite efficient. Application <strong>of</strong> such flowmeters include environmental<br />

monitoring, meteorology, hydrology, and maritime studies to measure the speed <strong>of</strong><br />

air or water flow and turbulence close to surface [11]. In the flowmeter, a solid object<br />

known as a drag element or target is exposed to the flow <strong>of</strong> fluid. The force exerted<br />

by the fluid on the drag element is measured and converted to a value for speed <strong>of</strong><br />

flow. An important advantage <strong>of</strong> the drag sensor is that it can be made to generate<br />

a measurement <strong>of</strong> flow in two dimensions, or even in three dimensions, as well as<br />

<strong>of</strong> flow speed. To implement this feature, the drag element must be symmetrical in<br />

the appropriate number <strong>of</strong> dimensions. These flowmeters have been used by industry,<br />

utilities, aerospace, and research laboratories to measure the flow <strong>of</strong> unidirectional<br />

and bidirectional liquids (including cryogenic), gases, and steam (both saturated and<br />

superheated) for almost half a century.<br />

The operation <strong>of</strong> the sensor is based on strain measurement <strong>of</strong> deformation <strong>of</strong> an<br />

elastic rubber cantilever, to which a force is applied by a spherical symmetrical drag<br />

element (Fig. 11.18). However, an ideal drag element is a flat disk [12], because this<br />

configuration gives a drag coefficient independent <strong>of</strong> the flow rate. Using a spherical<br />

drag element, which departs from the ideal <strong>of</strong> a flat disk, the drag coefficient may<br />

vary with flow speed, and, therefore, the gauge must be calibrated and optimized for<br />

the conditions <strong>of</strong> intended use. The strain measurement can be performed with strain<br />

gauges that should be physically protected from interaction with moving fluids.<br />

Fig. 11.18. Drag force sensor.

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