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handbook of modern sensors

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364 11 Flow Sensors<br />

(A)<br />

(B)<br />

Fig. 11.4. Thermoanemometer. (A) a basic two-sensor design; (B) cross-sectional view <strong>of</strong> a<br />

temperature detector.<br />

closer to the R s detector, that detector will register a higher temperature. When the<br />

medium flows, heat dissipation increases due to forced convection. The higher the<br />

rate <strong>of</strong> flow, the higher the heat dissipation and the lower the temperature that will be<br />

registered by the R s detector. Heat loss is measured and converted into the flow rate<br />

<strong>of</strong> the medium.<br />

A fundamental relationship <strong>of</strong> thermoanemometry is based on King’s law [2]<br />

( √ )<br />

2πρc dv<br />

Q = kl 1 +<br />

(T s − T 0 ) , (11.12)<br />

k<br />

where k and c are the thermal conductivity and specific heat <strong>of</strong> a medium at a given<br />

pressure, ρ is the density <strong>of</strong> the medium, l and d are the length and diameter <strong>of</strong> the<br />

sensor, respectively, T s is the surface temperature <strong>of</strong> the sensor, T 0 is the temperature<br />

<strong>of</strong> the medium away from the sensor, and v is the velocity <strong>of</strong> the medium. Collis and<br />

Williams experimentally proved [3] that King’s theoretical law needs some correction.<br />

For a cylindrical sensor with l/d ≫ 1, a modified King’s equation yields the velocity<br />

<strong>of</strong> the medium:<br />

v = K ( ) dQ 1 1.87<br />

, (11.13)<br />

ρ dt T s − T 0<br />

where K is the calibration constant. It follows from the above that to measure a flow,<br />

a temperature gradient between the sensor and the moving medium and the dissipated<br />

heat must be measured. Then, velocity <strong>of</strong> the fluid or gas becomes, although nonlinear,<br />

a quite definitive function <strong>of</strong> thermal loss (Fig. 11.5A).<br />

To maintain the R s detector at T s and to assure a sufficient thermal gradient with<br />

respect to T 0 , heat loss must be compensated for by supplying the appropriate power<br />

to the heating element.Also, we may consider a flow sensor without a separate heating<br />

element. In such a sensor, the R s detector operates in a self-heating mode; that is, the<br />

electric current passing through its resistance generates enough Joule heat to elevate<br />

its temperature to T s . At that temperature, the second detector has resistance R s .<br />

Assuming that conductive heat loss through connecting wires and sensor’s enveloping

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