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2. Machine vibration measurements
The laboratory stand consists of: a set of accelerometers, preamplifiers and measuring
amplifiers with instrumentation (personal computers equipped with measurement cards), two
standard vibration sources and four fans of the same type in different technical condition.
The exercise consists of three parts (all parts are performed individually by each student).
The first part consists in completing the equipment, compiling the complete track for measuring
the effective value of the amplitude of vibration acceleration and calibrating the measuring track.
Complete measurement paths can be calibrated using a reference vibration signal with a known
amplitude. The discrepancy between the amplitude of the reference signal and the value indicated
by the meter can be treated as the result of calibration, each time improving the obtained
measurement results. If we do not have a reference source of vibrations, and the voltage
sensitivity of the measuring transducer with the matching circuit is known, the calibration element
is to synchronize the meter indications with the value of the reference voltage signal. During the
measurements, the voltage amplitude will be read, which gives the acceleration divided by the
sensitivity
First, attach the accelerometer to a selected point on the body of the tested
machine (the mounting method should be justified). Then, in the measurement protocol,
we note the results of ten readings of the amplitude of vibration acceleration with the
averaging time constant "fast”; and ten with the constant "slow".
The last and third step is to develop and interpret the results. You should:
• Calculate the average measured value of the vibration acceleration amplitude
separately for each time averaging method;
• Interpret discrepancies between results;
• Report the amplitude range for the 95% confidence level of the results;
• Estimate the maximum measurement error and justify the estimation made;
• Calculate the effective and peak values of vibration velocity and displacement for the
measured amplitude of the harmonic vibration acceleration with the given frequencies.
The report documents the performance of the exercise and is prepared in full
during the classes. The completion of the measurement track and the method of
conducting are assessed measurements, formulating conclusions and understanding
the issues related to the conducted research. The degree of mastering the material is
reflected in the proficiency in performing tasks.
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The exercise requires a good knowledge of the issues presented in the first part of the
manual (without chapter 4) and in the further part of the exercise description.
Background information
According to the standard definition (PN-82/N-01350), vibration is a process in which
certain characteristic quantities are functions of time, usually alternately increasing and
decreasing in successive time intervals.
Mechanical vibrations - these are vibrations in which the change of any kinematic or
dynamic quantity characterizing the state of the system is a function of time. The studied
motion parameters are usually: displacement, velocity, acceleration. As you know, integrating
acceleration over time gives velocity; displacement is obtained by reintegration. The mutual
relations of these three parameters are shown in Figure II.2.1, where both axes (frequency and
amplitude) are presented on a logarithmic scale.
Fig. II.2.1 Dependence between acceleration and speed and vibration displacement
as a function of frequency.
The choice of the measured parameter depends primarily on the frequency of the
significant vibrations from the point of view of the conducted research. For low-frequency
vibrations, the amplitude of displacements gives the most information. The vibration speed is
a good parameter in a fairly wide range because it is proportional to the energy of the
vibrating motion dissipated as a side effect of the machine operation.
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Vibration acceleration allows you to extend the analysis range also to higher
frequencies. It is often used in vibroacoustic diagnostics, for example in detecting short-term
damage to rolling bearings.
The set of apparatus for measuring vibrations follows the general scheme of the
measuring path. Various types of measuring transducers are used, including:
- electrodynamic,
- piezo-electric
- piezoresistive,
- Induction
- Capacitive
- using Foucault currents,
- optical (including laser),
- using an electromagnetic field.
Piezoelectric accelerometers are used in the exercise. Their main strengths below:
- Resistance to environmental factors
- wide frequency response,
- good linearity,
- low dependence of sensitivity on temperature,
- low interference impact,
- Size and weight
The drawback is relatively low sensitivity and high impedance, which makes it
necessary to use charge amplifiers or matching preamplifiers.
Charge preamplifiers practically make the sensitivity of the measurement path
independent of the length of the test lead. In voltage preamplifiers, on the other hand, the electric
capacity of the cable significantly changes the voltage sensitivity of the accelerometer. If we
consider a substitute diagram of such a converter (generating charge q) with a wire as shown in
the figure, then voltage will be applied to the input of the preamplifier V e according to the
relationship:
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where:
Ve - preamplifier input voltage,
Ce - capacity of electric cable,
Ca - internal capacity of accelerometer.
Fig. II.2.2 Equivalent diagram of an accelerometer with a wire.
Currently, quite common use is made of converters equipped with a miniature,
integrally placed preamplifier. Sometimes, when using piezoelectric accelerometers, it is
necessary to consider the influence of transverse vibrations on the measurement result. In
modern accelerometers, transverse vibrations have a small share (usually it does not exceed
3%). In higher-class accelerometers, the direction of the highest sensitivity axis deviation
from the vertical is often indicated by a red dot on the transducer body (Figure II.2.3
When selecting a transducer, consider its dynamic range (the size of the processed
amplitudes) and the frequency response. The usual rule of thumb is that measurements are
made in a linear region. The useful measuring bandwidth of piezoelectric transducers is well
below the accelerometer resonance (after considering the mounting effect).
The influence of different mounting methods on the frequency response is illustrated
in the following figures. It can be seen that the best properties have rigid connections, and at
higher temperatures, almost exclusively threaded connections are used. The results of
measurements with a hand-held probe are not very repeatable, and such a set is only suitable
for low-frequency vibration measurements.
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Fig. II.2.3 Illustration of the position of the axis of highest sensitivity of the accelerometer.
Fig. II.2.4 Resonance curve for mounting the accelerometer with a centrally located screw .
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Fig. II.2.5 Resonance curve for fixing an accelerometer with beeswax.
Fig. II.2.6 Resonance curve for accelerometer mount screw through the washer ceramic.
Fig. II.2.7 Resonance curve for mounting an accelerometer using a sticky threaded washer.
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Fig. II.2.8 Resonance curve for attaching the accelerometer with adhesive discs.
Fig. II.2.9 Resonance curve for mounting an accelerometer with a magnet.
Fig. II.2.10 Resonance curve illustrating the range of applications hand probe.