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Radar Technology for Level Gauging - Krohne

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6.7 Propagation along electric lines (TDR method)<br />

In the TDR method, waves are propagated not through the tank atmosphere but along an<br />

electric line (see chapters 4.4.1 to 4.4.4), shown in Fig. 29 by way of example with a rod or<br />

wire rope.<br />

An interference reflection is generally <strong>for</strong>med at the junction between measuring system and<br />

rod (see chapter 4.4.8).<br />

The propagation rate along the line is equal to the speed of light, independent of the type<br />

and dimensions of the line (see chapter 6.1.2). Line attenuation occurs with the finite conductivity<br />

of the metallic material, but this only becomes apparent in steel lines of more than<br />

10 m (32 ft) in length 26 .<br />

On the basis of the field patterns <strong>for</strong> single-wire, two-wire and coaxial cables shown in<br />

Fig. 30, it will be recognized that the possibility of interference from adjacent metal objects<br />

is the greatest with the single-wire system and non-existent with the coaxial system.<br />

26 As the skin effect is heavily dependent on the magnetic property µr, a completely non-magnetic (austenitic) steel is<br />

to be favoured. If in doubt, copper or aluminium should be used, both of which, moreover, have a conductivity that is<br />

approximately 40 and 25 times, resp., higher than steel.<br />

Distance<br />

Signal level<br />

Interference signal<br />

Useful signal<br />

Fig. 29:<br />

TDR arrangement<br />

with a rod<br />

<strong>Radar</strong> handbook 37<br />

6<br />

Fig. 30:<br />

Pattern of electric field<br />

lines in the plane<br />

across the line:<br />

a) single-wire,<br />

b) two-wire,<br />

c) coaxial cable.

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