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Agilent Spectrum Analysis Basics - Agilent Technologies

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These represent intermodulation distortion, the interaction of the two<br />

input signals with each other. The lower distortion product, 2ω 1 – ω 2 , falls<br />

below ω 1 by a frequency equal to the difference between the two fundamental<br />

tones, ω 2 – ω 1 . The higher distortion product, 2ω 2 – ω 1 , falls above ω 2 by the<br />

same frequency. See Figure 6-1.<br />

Once again, dynamic range is a function of the level at the input mixer. The<br />

internally generated distortion changes as the product of V 1 2 and V 2 in the<br />

first case, of V 1 and V 2 2 in the second. If V 1 and V 2 have the same amplitude,<br />

the usual case when testing for distortion, we can treat their products as<br />

cubed terms (V 1 3 or V 2 3 ). Thus, for every dB that we simultaneously change<br />

the level of the two input signals, there is a 3 dB change in the distortion<br />

components, as shown in Figure 6-1.<br />

This is the same degree of change that we see for third harmonic distortion<br />

in Figure 6-1. And in fact, this too, is third-order distortion. In this case,<br />

we can determine the degree of distortion by summing the coefficients<br />

of ω 1 and ω 2 (e.g., 2ω 1 – 1ω 2 yields 2 + 1 = 3) or the exponents of V 1 and V 2 .<br />

All this says that dynamic range depends upon the signal level at the<br />

mixer. How do we know what level we need at the mixer for a particular<br />

measurement? Most analyzer data sheets include graphs to tell us how<br />

dynamic range varies. However, if no graph is provided, we can draw<br />

our own 2 .<br />

We do need a starting point, and this we must get from the data sheet. We<br />

shall look at second-order distortion first. Let’s assume the data sheet says<br />

that second-harmonic distortion is 75 dB down for a signal –40 dBm at the<br />

mixer. Because distortion is a relative measurement, and, at least for the<br />

moment, we are calling our dynamic range the difference in dB between<br />

fundamental tone or tones and the internally generated distortion, we have<br />

our starting point. Internally generated second-order distortion is 75 dB<br />

down, so we can measure distortion down 75 dB. We plot that point on a<br />

graph whose axes are labeled distortion (dBc) versus level at the mixer<br />

(level at the input connector minus the input-attenuator setting). See<br />

Figure 6-2. What happens if the level at the mixer drops to –50 dBm? As<br />

noted in Figure 6-1, for every dB change in the level of the fundamental at<br />

the mixer there is a 2 dB change in the internally generated second harmonic.<br />

But for measurement purposes, we are only interested in the relative change,<br />

that is, in what happened to our measurement range. In this case, for every<br />

dB that the fundamental changes at the mixer, our measurement range also<br />

changes by 1 dB. In our second-harmonic example, then, when the level at<br />

the mixer changes from –40 to –50 dBm, the internal distortion, and thus our<br />

measurement range, changes from –75 to –85 dBc. In fact, these points fall<br />

on a line with a slope of 1 that describes the dynamic range for any input<br />

level at the mixer.<br />

2. For more information on how to construct a<br />

dynamic range chart, see the <strong>Agilent</strong> PSA<br />

Performance <strong>Spectrum</strong> Analyzer Series Product<br />

Note, Optimizing Dynamic Range for Distortion<br />

Measurements, literature number 5980-3079EN.<br />

72

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