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Radar Technology for Level Gauging - Krohne

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The thinner the pipe, the slower are the waves propagated 21 . The propagation rate in the<br />

cylindrical waveguide (inside diameter D) is 22 :<br />

The diagram in Fig. 24 shows the correction factor as a function of the inside pipe diameter.<br />

The minimum diameter is dependent on the wavelength, or frequency.<br />

6.2 Transmission through dielectric windows<br />

The practical application of radar level gauging systems requires that the tank interior be<br />

separated from the tank exterior in order to provide separation of pressure, temperature and<br />

product. To this end, "windows" of a dielectric material (plastics, glass, ceramics) are used<br />

which <strong>for</strong> the microwaves should preferably be transparent and low reflecting.<br />

reflected<br />

wave<br />

incident wave transmitted wave<br />

The series of events can be imagined thus: a first (negative) reflection r 1 occurs at the left<br />

interface between air and dielectric and a second (positive) reflection r 2 at the right interface,<br />

which ideally cancel each other out (Fig. 25). It is reasonable to assume that the<br />

difference in the transit time of the waves must be a multiple of the wavelength inside the<br />

dielectric, divided up into incident wave and reflected wave. We there<strong>for</strong>e obtain the ideal<br />

thickness d of the window with material property ε r as:<br />

21 Relevant is the so-called group velocity, not the phase velocity of the waves<br />

dielectric<br />

window<br />

22 Group velocity; the <strong>for</strong>mula applies to the fundamental mode of the H11 waves; <strong>for</strong> other modes the factor 1.7 will<br />

change according to the table in section 4.4.5.<br />

Fig. 25:<br />

Reflection of waves<br />

from a dielectric<br />

window<br />

<strong>Radar</strong> handbook 31<br />

6

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