Using OLED and TFT displays with Narrow boards
One of the very exciting possibilities when using an MCU is driving an LCD, OLED or TFT display module. In the recent years, the industry has produced a growing...
In this post we are going, just for once, to focus mainly on theoretical concepts, to explain the microcontroller performance when using direct and reciprocal frequency measurement.
This paper is objective is to expose the limitations of resolution and accuracy, and the techniques used to count frequencies over a very large bandwidth. Possibly you might want to skip the pure theory section and get to the theoretical experiment.
Basic theory of frequency vs period
Microcontroller computation techniques
Direct frequency measurement with a microcontroller
Reciprocal frequency measurement with a microcontroller
Limitations
1) Upper frequency limit
2) Accuracy
3) Resolution
Theoretical experiment
Operational hypothesis
1) Reciprocal counting resolution and domain of operation
2) Direct counting resolution and domain of operation
3) Reciprocal + direct counting resolution and domain of operation
4) Introducing the maximum frequency and clock accuracy limitations
5) Extending the domain of operation
6) Proposed display resolution
Real world application
In theory we can compute the frequency from the period (duration of a cycle) or the period from the frequency with this function
f = 1 / p that is equivalent to p = 1 / f
For example a 10 Hz signal has a period p = 1/10 = 0.1 second.
Our first problem is that when using a microcontroller we don’t have access to a precise time reference. What we have available is the number of microcontroller clock counts that executed while measuring the signal.
Since we know our microcontroller is clocked at 10 MHz (as an example), after we count 10 000 000 clock counts we know that a time duration of approximately one second has passed. So we just have to
The number in the counter 2 equals the frequency of the signal. For example counter 2 = 1000 means the signal has a frequency of 1 KHz and a period of 1/ 1000 = 0.001 seconds.
We can approximate the period of the signal in seconds with the function
p = clock counts (during one period of the signal) / mcu clock frequency
To achieve this we have to
For example if we count 1000 clock counts between two fronts of the waves, that is during a whole period, we compute the period as p = 1000 / 10 000 000 = 0.0001 second
And we deduct the frequency as explained above f = 1/0.0001 = 10 KHz
The main point of this paper will be to expose the limitations of this technology:
When direct counting it is not possible to count frequencies higher than half the microcontroller is clock frequency. This is explained by the Nyquist theorem. (Wikipedia full and complex explanation).
So, in our example, the maximum frequency that can be counted is 10/2 = 5 MHz.
But, we might cheat a little by using a prescaler. This is an external device that will pre-count the signal. It will output one clock signal every time it has seen a certain binary number of fronts on its input. In this example we will consider a 16:1 prescaler. That is we will be able to count up to 16 x 5 = 80 MHz
Common prescalers are 74HC93, 74VHC4040 and many others.
We just explained that our knowledge of time duration depends on to the microcontroller is clock frequency. Unfortunately this clock is not perfect. It vibrates at approximately its defined frequency (10 MHz here). But its accuracy error does create as much error in our computation. We will express this error in ppm. If the error of the clock is 1 part per million, that is our measuring of one second can be wrong at most by 1/1000000 of a second. Our computation will also have an error of 1 ppm. This creates an uncertainty on the 7th digit of our computation.
TCXO in 3225 package
This error in accuracy of around 1 ppm (on the frequency value + as much of drift due to temperature + aging) is the best we can get from nowadays small and affordable TCXO clock chips. It was more in the 50 ppm range only a few years ago. Looking for an even better accuracy would need more advanced, much more costly and space consuming devices.
Then we also have to consider the inner working of the MCU (internal signal propagation and management) and the fact that this computation is based on a code that executes on the MCU (with delays of code execution and possible queuing when using interrupts). In consequence a 1 ppm device is a good choice and we might not get much more accuracy when using a more accurate clock with these relatively simple techniques. And because of the different sources of errors the total accuracy will probably be above 1 ppm and not constant over the all bandwidth. But we will not consider these too complicated and ill-defined aspects of the problem.
We will consider that the total raw inaccuracy of our circuit (frequency + temperature drift + aging + computation errors) is less than 10 ppm (6 digits).
But, to compensate some of the inaccuracy, the program might include a calibration mechanism. This would allow to reduce the total inaccuracy when calibrated to possibly as low as 1 ppm (7 digits).
Now, we have another big problem. Since we measure the time in terms of clock counts, we are working with digital data. We can’t measure with more resolution than 1 clock count. This brings a terrible limitation to our approximation of the frequency.
From this we can see that direct frequency measurement has a reasonable resolution only for high frequency signals, while reciprocal frequency measurement has a reasonable resolution only for low frequency signals.
Thus if we want to create a frequency counter that covers very lows up to very high frequencies, we need to use both computation methods.
After reading the theory section we know that our measurement system is limited. We have to consider these parameters:
As seen above the resolution Res = log(f_mcu_clock/f) + 1 is plotted on this chart
Reciprocal frequency measurement domain of operation
The green area is the low frequencies domain of operation. It is the area between the minimum of 4 digits of resolution and the maximum theoretical resolution. When measuring frequencies from 1 Hz to 10 KHz we are certain to get the minimum resolution we would like.
As seen above the resolution Res = log(freq) +1 is plotted on this chart
Direct frequency measurement domain of operation
The green area is the high frequencies domain of operation. It is the area between the minimum of 4 or 5 digits of resolution that we chose and the maximum theoretical resolution. When measuring frequencies from 1 KHz to the upper limit we are certain to get the minimum resolution we would like.
Direct frequency measurement + reciprocal frequency measurement domain of operation
When using both computations we can extend the domain of operation from the very low frequencies to the ultra high frequencies. Here we have
Direct + reciprocal frequency measurement with accuracy and frequency limits domain of operation
Now if we add the limitations that we exposed before regarding the maximum frequency that can be measured and the accuracy of the microcontroller clock, the domain of operation gets limited.
We can see that the domain of operation has been much narrowed. But we still maintain the resolution we wanted. And we can build a frequency counter that will work as expected from 1 Hz to 8 MHz.
We have exposed that we might increase the upper frequency limit by using a prescaler. And we can also push the accuracy limit by calibrating the device. Here is what we should get
Direct + reciprocal frequency measuremen with accuracy and frequency limits, with prescaler and calibration, domain of operation
When using a 16:1 prescaler we can see that we can extend the domain of operations from over 1 Hz to 128 MHz.
We used the prescaling in two stages 4:1 at 5 MHz and 16:1 at 20 MHz. So, even though we reduced the theoretical resolution, the direct counting resolution line (in dark blue) it is still above the accuracy error and preserves the domain of operation.
After calibrating the device we expect to reduce the accuracy error from 10 ppm to 1 ppm at best, providing some overhead (light green area) in the domain of operation.
In this paper we have shown that the microcontroller performance when using direct and reciprocal frequency measurement depends a lot on the mcu clock speed and accuracy, but that we have techniques to increase the performance of the device.
Now that we know the resolution profile, we can choose how to display the results. Here, we have to define a profile of display resolution.
If we prefer to be conservative and the device is not calibrated we can use a display resolution profile like this one
Proposed display resolution, device not calibrated
This profile guaranties that we will never display any biased values over the all bandwidth even though the device is not calibrated. We did not exploit the possible high resolution in low frequencies because a regular user might find strange to have a drop of resolution in the mid band.
But if we are ready to take a risk to get a few biased values between 5 KHz and 10 KHz, if the device is calibrated and if we want to use the enhance resolution in the low frequencies band we could use this profile:
Proposed display resolution, device calibrated with enhanced resolution on LF
This profile will give us the maximum possible display resolution over the all bandwidth.
These 4 techniques (direct & reciprocal counting, prescaler and calibration) are used in the Arduino compatible frequency counter.