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Measuring FM Deviation Via Bessel Nulls

 

What is a Bessel Null and how does it relate to a Z90?

One use of a Z90, in addition to its obvious use as a ham band monitor, is to calibrate FM modulation of a transmitter or a signal generator via the Bessel Null technique.

The principle behind Bessel Nulls is that in a phase or frequency modulation system, the relationship of the carrier level, the modulating frequency and the deviation is defined by a mathematical relationship known as a Bessel function, named after their discoverer, the German mathematician Friedrich Bessel. Bessel lived nearly 100 years before FM was invented but his mathematical techniques have proven useful in describing many physical phenomena.  For more details, see Agilent's Application Note 1390. At the moment, it may be found at http://cp.literature.agilent.com/litweb/pdf/5988-5677EN.pdf, but Agilent periodically rearranges its web site so this address may not last indefinitely.

For our purpose, it is sufficient to understand that for certain values of deviation and modulating frequencies, the carrier will reduce to zero. More practically, a deep null, on the order of 30 or 40 dB can be seen as these values are approached. Appropriately enough, these are called Bessel nulls, and the more useful values are:
 

Null Modulation Index β
1 2.40
2 5.52
3 8.66
4 11.79
5 14.93
6 18.07

Modulation index β is defined as:

In other words, if we modulate an FM transmitter with a 1 KHz audio tone, and slowly increase the deviation, we see the carrier drop in level, and disappear when the deviation is 2.40 KHz and then increase, to disappear again when the deviation is 5.52 KHz, etc.

If we instead modulate the transmitter with a 3 KHz tone, the first null is seen with 3.0 KHz * 2.4 = 7.2 KHz deviation, etc.

To clarify one point, the total power in an FM system remains constant, regardless of deviation and modulating frequency. However, the total power is spread out amongst the carrier and the modulating sidebands in a complex fashion, described by the Bessel functions. At a Bessel null, 100% of the power is in the sidebands, with the carrier reduced to zero.
 

Let's see how this works in practice. I connected a Boonton 102D signal generator to a Z90. The particular frequency I used is 4915 KHz, but this is not important to the concept. In order to resolve the carrier, I've set the Z90's span to 10 KHz.

 

Signal generator with modulation turned off. Carrier level is approximately 40 dB over the base line.


I  then selected FM modulation, 1 KHz internal source and set the deviation to be an indicated 3 KHz. The result shows the carrier and several modulating sidebands.
 
With 1 KHz modulating frequency and 3 KHz deviation, many sidebands are seen. The carrier is approximately 12 dB reduced from the no modulation stage.

I gradually reduced the deviation control, watching the carrier level on the Z90's screen.
First Bessel Null. 1 KHz modulation frequency.

At this deviation setting, the carrier is reduced by 30 dB from the unmodulated state. This is "close enough" to zero for our purpose.
 
The modulation setting on my 102D at the level corresponding to the null condition shown above. The meter multiplier is 0-3 KHz, so the displayed value is 2.50 KHz deviation.

The theoretical deviation at the first null is 2.40 KHz, and my 102D reads 2.50 KHz, so it's about 4% high. The 102D's specification is ±10%, so it's well within tolerance.

Let's try a different combination - 3 KHz modulating frequency. The 1st Bessel null is found at modulation index β= 2.40. Since β is defined as deviation/modulating frequency, then

deviation = β * modulating frequency

With 3 KHz modulation, we should see the carrier null at a deviation of 2.40 * 3.0 KHz  = 7.20 KHz.

 

First Bessel null, 3 KHz modulating frequency, 7.2 KHz deviation
 
At this carrier null, the 102D's meter reads 7.6 KHz (0-10 KHz scale)

The error between indicated deviation and actual deviation is 5.5%, again well within the 102D's ±10% FM modulation indication accuracy.