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These symbols in the technical data show the operating ranges of microsonic ultr<strong>as</strong>onic sensors.<br />

The attenuation of sound in the air<br />

depends on the temperature and pressure of the air <strong>as</strong> well <strong>as</strong> its relative humidity. The physical relationships are complex<br />

and have different effects at different ultr<strong>as</strong>onic frequencies. For simplicity we can say that the attenuation in the air incre<strong>as</strong>es<br />

with rising temperature and rising humidity. This necessitates a reduction in the size of the detection zones.<br />

With a lower relative humidity and falling temperatures, the attenuation in the air decre<strong>as</strong>es and the detection zones enlarge<br />

accordingly.<br />

The reduction in the size of the detection zone is essentially compensated for by the sensor's operating reserves. And at<br />

temperatures below 0 °C some sensors can operate over distances certainly twice <strong>as</strong> large <strong>as</strong> those given here.<br />

As the pressure of the air rises, so the attenuation in the air drops considerably. This <strong>as</strong>pect should be taken into account for<br />

applications involving overpressure. Sound propagation is impossible in a vacuum.<br />

0,15 m<br />

20 mm blind zone<br />

150 mm operating range<br />

250 mm maximum range<br />

f = 380 kHz, λ = 0.9 mm<br />

Used in the following product groups:<br />

zws ucs sks<br />

0,24 m<br />

50 mm blind zone<br />

240 mm operating range<br />

350 mm maximum range<br />

f = 500 kHz, λ = 0.7 mm<br />

Used in the following product groups:<br />

zws ucs<br />

::: Detection zones :::

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