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Homer Hot Measurement and Tuning System - S-TEAM Lab

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Reflection coefficient modulus<br />

M<br />

M<br />

max<br />

min<br />

M u<br />

M u<br />

The formulas assume M > u. For M < u, M min = 0.<br />

Reflection coefficient phase angle<br />

<br />

<br />

where<br />

max<br />

min<br />

<br />

<br />

<br />

180<br />

<br />

u<br />

M<br />

is phase angle uncertainty in degrees. The formula derivation assumes M >> u. Clearly, given a value of u, the phase<br />

angle uncertainty grows when the reflection coefficient magnitude decreases. For M < u, phase angle loses meaning<br />

at all.<br />

Return loss R<br />

R<br />

R<br />

max<br />

min<br />

20log(<br />

M<br />

20log(<br />

M<br />

min<br />

max<br />

)<br />

)<br />

Voltage st<strong>and</strong>ing wave ratio V<br />

V<br />

V<br />

max<br />

min<br />

(1 M<br />

(1 M<br />

max<br />

min<br />

) /(1<br />

M<br />

) /(1<br />

M<br />

max<br />

min<br />

)<br />

)<br />

Effective directivity <strong>and</strong> test port (source) match<br />

Two independent quantities usually characterize heterodyne network analyzers. These are<br />

<br />

<br />

Effective directivity E D (critical for the measurement of small reflection coefficients)<br />

Effective test port (source) match E S (affecting primarily the measurement of high reflection coefficients)<br />

In the six-port reflectometer, effective directivity can be linked with the uncertainty circle radius u as<br />

E D<br />

20logu<br />

Effective test port match cannot practically be defined.<br />

See also Deembedded Reflection Coefficient Accuracy Considerations.<br />

<strong>Measurement</strong> Uncertainty Example<br />

An example of return loss uncertainty considerations is depicted in Figure 3. If, for instance, the uncertainty radius is<br />

u = 0.02 (E D = 34 dB) <strong>and</strong> the measured return loss is 20 dB (i.e. M = 0.1), then the true value lies somewhere<br />

between R min = 18.42 dB <strong>and</strong> R max = 21.94 dB.<br />

If you wish to be sure that the true return loss is greater than 20 dB, the measured value must be so that R min is at<br />

least 20 dB. The intersection of 20-dB horizontal graticule with the lower blue line (green circle) then shows that the<br />

measured return loss must be at least 22 dB.<br />

Mathematically, R min = 20 dB corresponds to M max = 0.1. Because, as stated above, M max = M + u, the measured<br />

reflection coefficient magnitude must not exceed the value M x = M max – u = 0.1 – 0.02 = 0.08, hence the measured<br />

return loss must be at least R x = -20 log(M x ) = -20 log(0.08) = 21.94 dB, which is approximately the 22 dB obtained<br />

from the graph.<br />

User's H<strong>and</strong>book <strong>Homer</strong> <strong>Hot</strong> <strong>Measurement</strong> <strong>and</strong> <strong>Tuning</strong> <strong>System</strong> Introduction 7

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