Revista de Ciencias Tecnológicas (RECIT): Volumen 7 (3): e288.
3 ISSN: 2594-1925
possible [18]. The methods reported to solve this
task should have a minimum measurement time;
at the same time, if a more accurate
approximation to the measurand is required, a
longer time is needed to obtain a satisfactory
signal.
In case of optical sources, frequency
approximation systems based on Mach–Zehnder
interferometers are used [19]. In the work of Li
et al. [20], variations on relative phase shifts are
used through an optical delay line and spacing
between antennas. Then the phase comparison
based on a multi-base line eliminates the
ambiguity of the angle of arrival over a large
frequency range. Hence, the frequency and angle
of arrival are determined by analyzing the phase
shift of the intermediate frequency signal.
Considering the technological applications of
sensors these days, frequency measurement
systems are being integrated into embedded
systems. For example, an IoT based system has
been proposed for vibration analysis by Kneifel
et al. [21]. In such a system, frequency
measurement is done after realizing fast Fourier
Transform.
In case of methods based on pulse counting, the
principle of rational approximations has been
exhaustively studied in the last years, as a result,
plenty of mathematical formalisms has been
provided for explaining the functioning of such a
method, and experimental prototypes have been
built for experimental evaluation.
As has been reported [14], the principle of
rational approximations requires enough time to
yield a good approximation, which is based on
reaching numerator in the form of “one with r
zeros”. Later, theoretical advances included the
understanding of the pulse width effect in the
reduction of error [15], [16]. Then, the phase
effect and the relation with the shape of error
during measurement was discovered [17]. In
these reports, the authors present evaluation of
the measurement process of signals with an
unknown frequency, then another problem came
up; when the signal from sensors has a frequency
value that changes from one value to another,
there is a frequency shift, then, there are two
unknown frequency values. So, with the aim to
solve this problem, a formalism to solve the
problem of measuring the frequency shift was
proposed [22], [23], [24], [25].
It is based on measuring the desired or unknown
frequency before and after the stimulation of the
sensor, then the difference between both
measurements is computed. There are two
restrictions before this task can be performed, the
first is that the approximation to desired
frequency must be achieved in a time as short as
possible, this with the aim to quantize the
frequency variations caused by input stimulus.
The second restriction is related to the
uncertainty that is adequate for the sensor, this is
that if the frequency shifts generated by the
sensor are below of the uncertainty during the
measurement, then, there is no relevant
information during the measurement process.
This is an important aspect, in particular for
piezoelectric sensors with a variation of their
proper frequency of several parts per million
[26]. From the study of the principle of rational
approximations, experimental implementations
of this method have been proposed.
In particular, the application of this method for
the quantification of frequency shifts generated
by a quartz crystal has been explored [27], [28].
And also, different applications have been
proposed, i.e. the automotive [29] and aerospace
industries [30], [24]. A proper understanding of
this method would allow its application for
improving other instruments that are of current
use, for example, frequency response analyzers,
such as the used on materials science for studying
the nature of nanoparticles [31], [32], [33], [34].