May 1967 Electronics World[Table of Contents] People old and young enjoy waxing nostalgic about and learning some of the history of early electronics. Electronics World was published from May 1959 through December 1971. All copyrights are hereby acknowledged. See all Electronics World articles.
This article from the May 1967 edition of Electronics World shows you just how long the Frequency Electronics company has been around! In fact, here is an excerpt from their website: "Frequency Electronics, Inc. was founded in 1962 and is now a well-established public company in Long Island, New York, and trades on the NASDAQ Stock Exchange under the symbol FEIM." Mr. Irwin Math, who wrote the article, has surely retired by now. The discussion on short- and long-term stability is as relevant today as it was 45 years ago.
The general expression for frequency stability is S=ΔF/F where F is the nominal frequency and ΔF is the allowable variation. Therefore, the actual frequency variation of our frequency standard (considering its output is 1 MHz nominal) is ±0.0001 Hz or ±1 x 10-10 of the nominal frequency.
However, this information is not enough. While it does indicate stability, it does not specify over what period of time this stability must be measured, The complete stability of a frequency-standard oscillator must be given in two parts: the long term and the short term.
The long-term stability of an oscillator is basically the average change in frequency over a long fixed period of time as compared to some absolute reference. Usually, long-term stability is measured in one of two ways. The first of these, as indicated in Fig. 1, depends on readings of frequency taken continuously for several days. The maximum peak-to-peak deviation over any 24-hour period is measured and the stability is then defined as ± one-half this maximum. For example, since both oscillators in Fig. 1 have a peak-to-peak variation of 1 part in 108 per day, their long-term stability would be specified as ±5 parts per 109 per day. Notice, though, that oscillator #2 has a much longer average rate of frequency change than does oscillator # 1. Therefore, while they both are ±5 parts in 109 per day oscillators, oscillator #2 is obviously superior.
The second method, and by far the more accurate one, is based on the average change of frequency over a given time interval. As shown in Fig. 2, the stability of oscillators #1 and #2 is now determined by the slope of their average frequencies. Now it is easy to see that oscillator #2 is substantially better than oscillator #1.
To further clarify the measurement and eliminate any remaining doubt, a few oscillator manufacturers incorporate both the average long-term frequency change and the day-to-day change in their long-term stability specification. For example, a 1-MHz oscillator such as the one shown in Fig. 4 with a rated long-term stability of ±1 part in 1010 is one whose maximum daily and average frequency will change by no more than ±1 cycle per 10 billion cycles per day or 0.0001 cycle per day.
The short-term stability of an oscillator is its frequency stability over periods of time from a few seconds to fractions of a second. This type of specification is important when the oscillator is used as the source for a frequency multiplication system, especially into the thousands of MHz. If, for example, a 1-MHz oscillator with a second-to-second variation of ±1 part in 106 were multiplied to 1000 MHz, the variation would now be ±1000 Hz per second.
As in long-term measurements, there are two general methods. One is similar to long term in that readings of frequency are taken. The time interval, however, is much shorter. Fig. 3 is a recording of an oscillator with a short-term variation of ±5 parts in 109 per second. Notice that in any 1-second interval, the frequency never deviates by ±5 parts in 109 from the nominal. This type of recording is used for intervals as low as 0.1 second. Smaller intervals require too fast a recorder speed and are measured by the second method.
This method involves a statistical approach. The oscillator to be measured is fed to a low-noise mixer along with a very stable reference frequency.
The difference of the two signals is then fed to a counter which measures the period (or wavelength) of this signal. A typical setup is shown in Fig. 5. The difference frequency actually triggers a gate, allowing a very stable 10-MHz signal to drive the counter. Since the period of the difference signal determines how many cycles of 10 MHz will be fed into the counter, great accuracy can be achieved. Assuming that the difference signal is 1 Hz, this means that 10,000,000 cycles will pass into the counter through the gate for each cycle of input. Therefore, only 1/10,000,000 of a second change in the difference signal will cause the counter to indicate a change. Since such great resolution is possible by this technique, extremely short intervals of time can be measured and interpreted as short-term stabilities.
Usually an oscillator with good short-term stability will not exhibit a good long-term characteristic and vice versa. As a result, where both long- and short-term stability must be as good as possible, the technique shown in Fig. 6 is used. A very good long-term standard and a very good short-term standard are fed to a phase detector. The d.c. output of the phase detector is then fed back to a voltage-variable capacitor in the short-term standard which causes its frequency to "lock" to the frequency of the long-term unit. This "phase-locking" technique now produces an output with excellent long- and short-term stabilities.
Fig. 5. Test setup employed for short-term measurements.
The stability of an oscillator with changes in ambient operating temperature is another important factor to consider when specifying high-stability oscillators. Fig. 7 is a curve of the temperature versus frequency characteristics of a typical high-quality crystal. It can be seen that changes in crystal temperature result in significant changes in frequency.
It is therefore extremely important to isolate the crystal from the effects of varying temperatures. Vacuum bottles (dewars) are often employed in the highest stability units and, in most cases, the crystal itself is in a well-regulated, temperature-controlled oven.
Similarly, changes in operating voltage, line voltages, and load impedances are all important and should be considered when choosing oscillators. The effects of these parameters are stated in terms of the maximum frequency changes they produce in the oscillators' output.
3. Measurements should be the result of exhaustive tests on many units of the type to be used, where possible.
Finally, perhaps the most important "specification" to many technical personnel is cost. While mechanical construction and ambient temperature isolation will determine the cost of a unit to an extent, the primary cost factor is the ultimate stability of the unit. The greater the stability required (both long- and short-term) the more elaborate the circuitry required and better the crystal must be. For example, while a ±1 part in 108 oscillator is available for $200, a ±1 part in 1010 oscillator can easily cost $2000.