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Agilent Spectrum Analysis Basics - Agilent Technologies

Agilent Spectrum Analysis Basics - Agilent Technologies

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In a factory setting, there is often an in-house frequency standard available<br />

that is traceable to a national standard. Most analyzers with internal<br />

reference oscillators allow you to use an external reference. The frequency<br />

reference error in the foregoing expression then becomes the error of the<br />

in-house standard.<br />

When making relative measurements, span accuracy comes into play.<br />

For <strong>Agilent</strong> analyzers, span accuracy generally means the uncertainty in<br />

the indicated separation of any two spectral components on the display.<br />

For example, suppose span accuracy is 0.5% of span and we have two signals<br />

separated by two divisions in a 1 MHz span (100 kHz per division). The<br />

uncertainty of the signal separation would be 5 kHz. The uncertainty would<br />

be the same if we used delta markers and the delta reading would be 200 kHz.<br />

So we would measure 200 kHz ±5 kHz.<br />

When making measurements in the field, we typically want to turn our<br />

analyzer on, complete our task, and move on as quickly as possible. It is<br />

helpful to know how the reference in our analyzer behaves under short warm<br />

up conditions. For example, the <strong>Agilent</strong> ESA-E Series of portable spectrum<br />

analyzers will meet published specifications after a five-minute warm up time.<br />

Most analyzers include markers that can be put on a signal to give us<br />

absolute frequency, as well as amplitude. However, the indicated frequency<br />

of the marker is a function of the frequency calibration of the display, the<br />

location of the marker on the display, and the number of display points<br />

selected. Also, to get the best frequency accuracy we must be careful to<br />

place the marker exactly at the peak of the response to a spectral component.<br />

If we place the marker at some other point on the response, we will get a<br />

different frequency reading. For the best accuracy, we may narrow the span<br />

and resolution bandwidth to minimize their effects and to make it easier to<br />

place the marker at the peak of the response.<br />

Many analyzers have marker modes that include internal counter schemes<br />

to eliminate the effects of span and resolution bandwidth on frequency<br />

accuracy. The counter does not count the input signal directly, but instead<br />

counts the IF signal and perhaps one or more of the LOs, and the processor<br />

computes the frequency of the input signal. A minimum signal-to-noise ratio<br />

is required to eliminate noise as a factor in the count. Counting the signal<br />

in the IF also eliminates the need to place the marker at the exact peak of<br />

the signal response on the display. If you are using this marker counter<br />

function, placement anywhere sufficiently out of the noise will do. Marker<br />

count accuracy might be stated as:<br />

±[(marker freq x freq ref error) + counter resolution]<br />

We must still deal with the frequency reference error as previously discussed.<br />

Counter resolution refers to the least significant digit in the counter readout,<br />

a factor here just as with any simple digital counter. Some analyzers allow<br />

the counter mode to be used with delta markers. In that case, the effects of<br />

counter resolution and the fixed frequency would be doubled.<br />

57

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