WORLD RADIO DAY 2021

COS'È IL WORLD RADIO DAY?

Il World Radio Day è la Giornata Mondiale della Radio proclamata dall'UNESCO per il 13 Febbraio di ogni anno.

Anche l'Italia celebra la Giornata Mondiale della Radio con i più grandi protagonisti delle Radio Nazionali, Locali, Web e Universitarie.

https://www.worldradioday.it/

via Bruno Pecolatto-AIR 130

WORLD RADIO DAY - X° Giornata Mondiale della Radio - MUMEC

 

A tutti gli amici del MUMEC Museo dei Mezzi di Comunicazione di Arezzo

Inviamo con la presente, l’invito per la partecipazione al convegno di celebrazione del

WORLD RADIO DAY - X° Giornata Mondiale della Radio
Venerdì 12 febbraio 2021 alle ore 16:00 

 

L'evento, indetto da UNESCO, sarà celebrato dal Museo con convegno online assieme ai partner principali: Centri per l’UNESCO di Arezzo e Firenze, RAI TOSCANA ed AIRE Associazione Italiana per la Radio d’Epoca. Maggiori info in locandina allegata alla presente

 

 

Per partecipare collegarsi al link zoom alle venerdì 12 febbraio alle 15:45:

 

 

Entra nella riunione in Zoom
https://zoom.us/j/97305237877

ID riunione: 973 0523 7877
Passcode: 072093

via Bruno Pecolatto-AIR130

How to easily improve by a factor of 100 the measurement of the frequency difference between two reference oscillators

Recently I had the idea to improve the possibility to quick measure the frequency difference of two reference oscillators , in this case two Rubidium Oscillators : a Rhode Schwarz and an M100 that I put into a yellow rack with a power supply , as in the pictures .

The method is based on :

A) Multiplying by 100 the frequency of both oscillators ( with the use of  simple home made Comb Generators )

B) Comparing the  frequency of the two oscillators with the method of the " beats " at 1 GHz , using a selective receiver . In the test I have used a Spectrum Analyzer , but every simple receiver , even an RTL Dongle can be used with the same results .

The two Comb Generator needed was made with two EX-OR fast ports ( ACT86) , with one of the two inputs connected directly and the second through  a variable resistor that , with the input capacitor of the port ,add a small delay .

The drawings can be found here : http://air-radiorama.blogspot.com/2021/02/double-symmetrically-comb-generators.html

The input is so a very sharp pulse depending on the rise and fall time of the EX-OR and of the delay of the RC constant ( in the range of ns ) .

Trimming the resistor the component at 1 GHz was at a comfortably level of -50 dBm .

The output of the two Comb generator was summed simply with two capacitor and two resistors .

You can find here the images of the output of a single Comb Generator , wide band and relatively narrow band .

What can we espect from this setup while summing the signal of the two Comb Generator at 1 GHz coming from the two Rubidium ? 

The composition of the two signals will change from a maximum of +3 dB when the phase of the two oscillator is the same and to a minimum ( if the signals are exactly equal of ) zero .

In this case the spread is around 20 dB , but doesn't matter because we have only to count the cycles .

The maximums will be always very wide , while the nulls will be always very sharp .

To check this I have tuned the Rubidium M100 as far as was possible , and you can see in the first part of the following screen with zero span ( this means that the Spectrum Analyzer acts as a receiver tuned at 1 GHz with vertical logaritmic scale ) .

Please note that the horizontal time sweep is 1000 s ( 100 second/div) .

At the beginning you can count around 10 oscillations in 100s , that means one cicle each 10 seconsd = 0,1 Hz of difference at 1 GHz .

Being 1 GHz = 10E9 Hz , this means a frequency maximun difference of 10E-10 .

While time was running , I have changed the frequency of the Rubidium M100 to approach that one of the RS Rubidium .

At the end of the screen the difference is around one cycle each ten second at 1 GHz , that means 10E-11.

Continuing the approach of the frequencies , I have increased the timebase till 6000 s because the phase change was very slow .

At the end , using sequential methof of approximation , in the last picture ,it is not easy if impossible to see a real periodicity in the phase rotation and so in the frequency difference .

We are in the range of 10E-12 . I am pretty sure that this limit doesn't depend from the method of measurement ( being a "physical method ") , but from the limit of stability ( jitter ) of one ( if not both ) Rubidium Oscillator , and this was the scope of the experiment .

If I am right , this simple setup , that everyone can easily reproduce at low cost , can measure stability higher than that of Rubidium Oscillators .

To check this with no dubts , I need two oscillator with performance 10 times better than the rubidium oscilllator I have used .

Hope one day I can check this , if I am so crazy to invest in two Masers  , because actually I am only playing to infringe my limits .....

But I have another couple of Rubidium Oscillators from  Stanford that I can try to check in the same way ....

 

Seminar with small video from Minicircuits

https://www.minicircuits.com/applications/webinars.html

Discovery Science on Judica Cordiglia Brothers

Recorded some time ago with my cellular phone from the TV set . The audio is low , but understandable .