Time Signals

 

 

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When I started work at the NPL in 1929 the only way of measuring the frequency of an oscillator was to count the number of cycles between two of the 1-second ticks transmitted from an observatory. These were primarily intended to give the time to ships at sea and enable them to determine their longitude, and the measurement of frequency was a secondary application. The time signals were accurate to about 0.01s so that it was necessary to extend the measurement over a period of 24 hours to obtain a value accurate to 1 part in 107 and this was a great inconvenience. The frequencies of two oscillations can be compared with a far greater accuracy in a few minutes and experiments were initiated by the International Scientific Radio Union to find out how such comparisons were influenced by the propagation conditions, when made at a distance. In one experiment in 1934 the NPL standard tuning fork was used to modulate the powerful 193kHz transmitter at Droitwich. It was received and measured at a number of standards’ laboratories in Europe and the results agreed to 1 part in 107, representing the highest accuracy achieved in international comparisons at that time.

 

 

During this period I amused myself by trying to measure the weak transmission of 5MHz made from Washington USA for their own local standardisation purposes. It could be received for a few hours during the night and I compared its frequency with that of the 250th harmonic of our 20kHz quartz standard. Although the accuracy of measurement was good to 2 parts in 108 and the standards in the two countries were believed to be known and stable to the same degree of accuracy, erratic variations of several parts in 107 were observed. These were attributed to Doppler effect changes caused by variations in the height of the reflecting layer. On occasions a regular beat was obtained but still gave a frequency difference of as much as 1 part in 107 due to a seemingly steady change in the height of the layer. The results showed that on average the frequencies could be compared to 2 parts in 108an that a detail study of the results could give useful information concerning the height of the reflecting layers.

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MSF

 

All standard frequency transmissions from the UK were suspended during 1939-1945 but a new service with the call sign MSF was inaugurated in 1950. It was too expensive a service to be met from the NPL budget but Sir Edward Appleton, who was then secretary of the government’s Department of Scientific and Industrial Research (DSIR), realised their importance, having himself used the early NPL transmissions in his fundamental work on the study of reflections at the ionosphere, made the necessary financial arrangements. The transmissions were operated by the PO (Post Office) at Rugby on behalf of the NPL which supplied the frequency standard. The frequencies used were those agreed internationally at 2.5, 5 and 10MHz but we added a frequency of 60kHz to cover Europe without ionospheric reflections. On one of my visits to the USA I was introduced to Jack Pierce at Harvard. He was investigating the application of frequency transmissions to air and sea navigation and I suggested that he might like to try and receive our frequency-controlled transmission at 60kHz. He found that he could receive it for a few hours at night and he was so impressed by its stability that he put in a formal request that the powerful 16kHz transmitter, which was also sited at Rugby, should be controlled by the same standard. The PO agreed to do this and this station, having an almost world wide coverage without ionospheric reflections, was the first to be controlled by the national frequency standard. When it was later controlled by our atomic clock it made atomic time available throughout the world.

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World wide synchronised time

 

The close co-operation with the USA made it easy to establish a world wide synchronised time service. As atomic clocks became available in the USA, Wm. Markowitz used them to control the service from the US Naval Observatory. The value of the atomic unit had been agreed but atomic clocks do not, of course, give the time of day and, although this is not required with the same accuracy, it is useful to have agreement throughout the world. To establish the accuracy of achieving this, time signals were interchanged between Washington and the NPL and a small difference of 2 milliseconds was revealed and resolved by mutual agreement between us including the Royal Greenwich Observatory. As other services came into use with atomic standards they adopted the same time, and an international synchronised time service was established without any formal discussions. More precise time comparisons were made later by re-transmitting the signals from the satellite Telstar, and avoiding errors due to ionospheric reflection. In this way synchronisation to 1 microsecond was achieved.

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Uncertainty

 

It was assumed in all these comparisons that the transmit time was the same in both directions, which could be proved only within the limits of experimental accuracy. This residual uncertainty was a great worry to Einstein, and the basis of his theory. But it was only an example of the uncertainty present in all scientific results. It is usually assumed that in order to obtain a consistent structure of science the units of measurement must be independent, and every effort was made to secure this. As measurements became more precise it should have been realised but was overlooked that this independence cannot be fully achieved because the units are determined in the complex earth environment in which all units are involved. The distinguishing feature of science is that experiments are repeatable and that the limits of error can often be made very small, and are, themselves, determined by experiment. The limits in time and frequency measurement are by far the smallest of all.

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Basic units

 

I was fortunate to take part in a transformation of two of the basic measurements in physics; time from the solar system and astronomy to the atom and physics, and length from a metal bar to the velocity of light multiplied by time. In both cases there was an enormous increase in accuracy and in the case of time measurements an enormous simplification as a bonus.

 

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