Pre Amps....some Measurement thoughts.

 

Nearly every VHF/UHF/SHF meeting now includes the infamous and good fun 'Noise Figure Measuring Contest'.

I will attempt to explain and illustrate that a simple list of results in a table showing only gain and NF of the devices under test (DUT) should not be considered as a 'definitive result'.

I believe the majority of participants just want to know "where they are" with respect to what they have just built and/or are using. Most people simply do not have frequent access to good test equipment, which is prohibitively expensive to be dedicated to 'amateur' applications/situations.

In recent years, where I have been involved in the measuring processes, I have attempted to try and broaden the view from that of a 'contest' into one of information exchange and education. Rather than simply grabbing a device out of the collection box, measuring it, scribbling a number on it, and then chucking it back in the box. It is much more productive for everyone present to look inside, fiddle with it, poke it, look at the techniques used ( with the owners permission ) and share the collective groups experience to suggest possible improvements that could be adopted.

The simple measuring of a noise figure and the associated tables constructed do contribute positively to the ongoing struggle/race to improve peoples receivers. But it is clear that the process of measurement, the results obtained, and the accuracy of the results are eithe r; not clearly understood, or, at least not acknowledged.

I have repeatedly stated in various discussions at these events I have attended, and in emails ;

"if the measurment indicates that you broke the laws of either physics or common sense then it's the measurement that's broke and not the laws"

This is an over simplified statement and could be improved to; "if the measurement indicates that you broke the laws of physics or common sense then you should try to quantify the possible range of accuracy/uncertainty of the measurement and then go on to try and investigate the apparent anomoly"

I am repeatedly seeing NF. claims of 0.16 dB and 0.18 dB at UHF/SHF. Manufacturers data for the devices used and even a primitive session in any decent simulation software shows that even a genuine 0.3 dB is highly improbable at bands higher than 144 Mhz, using room temperature techniques, so perhaps it's time for a reality check.

I'm also repeatedly told; "ok we cannot say that these measurements are absolute, we accept that, but we can say that all DUTs measured on our test setup can be compared to each other equally, so this is a good relative comparison result"

.......well, it can be......

If the data provided by test equipment manufacturers is considered properly, it is readily seen that the noise figures we are now attempting to measure with modern devices are, in many cases, lower than the margin of error, or "uncertainty" , in the equipment being used + uncertainties introduced by parameters of the DUT that are often not being measured and completely discounted/neglected.

Further analysis of the literature available on the web (go to Agilent's site and take the various application notes available and the uncertainty calculation tools) clearly highlights where the largest sources of possible measurement error/uncertainty occur.

It is not my intention here, nor is it necessary with all this excellent professionally prepared & written material available, to go into details of all the equipment contributions and DUT contributions to the overall uncertainty. Instead I will focus on one parameter only, the one that makes the largest contribution to amateur, noise figure optimised, measuring uncertainty.

Let us take two devices to be tested out of the collection box........

The top pre amp (DUT) uses a piece of LDF550 as a tuned input and I will call this DUT 1.

this is most often referred to as a cavity input design

The lower pre amp is a broad banded input design and I will call this DUT 2.

It is very clear which of these devices will offer the best bandwith response, the cavity input will. The broadband input design does have a high pass filter at ouput For the moment I am not examining these parameters as their influence, in this case, on the noise figure measurement/assesment is minimal..

Before I start to analyse & measure some parameters of these designs let me be clear. I am not going to be trying to prove or say that one is 'better' or 'worse' than the other overall. I am not going to be proving that the measurement of one is bad and the measurement of the other is good. My sole objective is to quantify the uncertainty contained in the two measurments, so that this can be taken into account in any judgemental decision taken.

I am going to put them both, in turn, on a Network Analyser and look at the match they provide to the test equipment (Even this will change when we move the DUT from the Network Analyser to the Noise Analyser, but we have to start somewhere), why we might wish to investigate this parameter will become clear later.

You can express such a match in several different ways, 'amateurs' tend to be more familiar with "SWR" expressed as a ratio like "1.5 to 1", and professionals tend to be more comfortable with "Return Loss" expressed in dB like " -10dB".

You can express the port (entry or exit) of the DUT in two ways also, either referenced as the familiar "Input" or "Output", or using the more flexible "S" terminology.

In this case Port 1 will be the input to the preamp and what we measure will be a reflection from that port, so this is know as S11 and will be expressed in dBs, generally negative, but not always in the case of noise optimised pre amplifiers. In the following displays the gain of the DUT is expressed as a measurement of S21 (port 1=input, port 2=ouput)

It is not my intention here to go deeply into S parameters or the measuring of them, but I do need to explain at least this particular parameter of S11, or "goodness of device under test input match", or, if you prefer, "the input SWR of the pre amp."

 

Here is the analyser screen for DUT number 1. (sorry for quality it had to be snapped off screen with my camera)

The lower plot is parameter S11(input match), the higher plot is parameter S21 (gain)

from the markers employed we can see that for DUT no.1. s11 is +2.7 dB and s21 is 23 dB

 

 

Here is the analyser screen for DUT number 2.

The lower plot is parameter S11(input match), the higher plot is parameter S21 (gain)

 

we can see that for DUT no.2. at 144 Mhz s11 is -4.8 dB and s21 is 24 dB

 

Now I turn to making the noise figure measurments

 

First DUT 1. (the cavity)

Here we have a Noise figure of 0.57 dB , as it turns out a surprising and poor result for this type of pre amplifier design, this is due to a) poor construction methods b) poor components employed. c) 'cold soldering' on the large copper line. For the purposes of this discussion the NF result as shown is not the point.

next DUT 2.

A result of 0.25 dB.

As traditionally published the results of these two DUT's would be displayed like this:

Pre Amp Gain Noise Figure
DUT1 23 dB 0.57 dB
DUT2 24 dB 0.25 dB

 

What this table does not show us is the input match of the pre amplifier, if it did it would look like this

Pre Amp Gain Noise Figure S11
DUT1 23 dB 0.57 dB +2.7 dB
DUT2 24 dB 0.25 dB -4.8 dB

Why would we want to see this additional column of S11 added ?

Firstly, it can tell us a little more about likely stability of the pre amp. Without getting 'hung up' on unconditional stability, which is NOT a requirement for amateur use pre amplifiers, in that conditional stability within the used parameters is sufficient. In general a poor s11 (low negative numbers or even positive numbers) can indicate likely stability issues.

Secondly, it can be used in conjunction with the following graph I have constructed to tell us something about the 'quality' of the measured result.

This plot is for a changing value of S11, Other contributing parameters are shown in the heading of this Plot. They are 'typical' values taken for the test equipment in use and 'general values' for the DUTs, we can surely discuss, or even argue the 'general values', however those parameters fixed in tbis plot have little change on the result of S11 changes.

Certainly case can be made for changing some of the equipment values, if you wish to change these recomendations given by the equipment manufacturer. (certainly improvement of noise head match will reduce the steepness of the slope of this s11 curve)

Now we have the possibility to add another column to our results table:

Pre Amp Gain Noise Figure S11 measurement uncertainty
DUT1 23 dB 0.57 dB +2.7 dB +/- > 0.7 dB
DUT2 24 dB 0.25 dB -4.8 dB +/- 0.4 dB

If we now change the table by adding another DUT

Pre Amp Gain Noise Figure S11 measurement uncertainty
DUT 23 dB 0.15 dB -0.5 dB +/- 0.6dB
DUT1 23 dB 0.57 dB +2.7 dB +/-> 0.7 dB
DUT2 24 dB 0.25 dB -4.8 dB +/- 0.4 dB

Can we now clearly identify the best Noise Figure here ?