What is Vibration? (part 3)
DLI Engineering
Posted 11-17-03
Logarithmic Frequency Scaling
So far, the only type of frequency
analysis discussed has been on a linear frequency scale, i.e.,
the frequency axis
is set out in a linear fashion. This is suitable for frequency
analysis with a frequency resolution that is constant throughout
the frequency range, commonly called "narrow band" analysis.
The FFT analyzer performs this type of analysis.
There are several situations where frequency analysis is desired,
but narrow band analysis does not present the data in its most
useful form. An example of this is acoustic noise analysis
where the annoyance value of the noise to a human observer
is being studied. The human hearing mechanism is responsive
to frequency ratios rather than actual frequencies. The frequency
of a sound determines its pitch as perceived by a listener,
and a frequency ratio of two is a perceived pitch change of
one octave, no matter what the actual frequencies are. For
instance if a sound of 100 Hz frequency is raised to 200 Hz,
its pitch will rise one octave, and a sound of 1000 Hz, when
raised to 2000 Hz, will also rise one octave in pitch. This
fact is so precisely true over a wide frequency range that
it is convenient to define the octave as a frequency ratio
of two, even though the octave itself is really a subjective
measure of a sound pitch change.
This phenomenon can be summarized by saying that the pitch
perception of the ear is proportional to the logarithm of frequency
rather than to frequency itself. Therefore, it makes sense
to express the frequency axis of acoustic spectra on a log
frequency axis, and this is almost universally done. For instance,
the frequency response curves that sound equipment manufacturers
publish are always plotted in log frequency. Likewise, when
frequency analysis of sound is performed, it is very common
to use log frequency plots.
The vertical axis of an octave band spectrum is usually scaled
in dB.
The octave is such an important frequency interval to the
ear that so-called octave band analysis has been defined as
a standard for acoustic analysis.
The figure below shows a typical octave band spectrum where the ISO standard
center frequencies of the octave bands are used. Each octave band has a
bandwidth equal to about 70% of it center frequency. This type
of spectrum is called
constant percentage band because each frequency band has a width that is
a constant percentage of its center frequency. In other words, the analysis
bands become wider in proportion to their center frequencies.
It
can be argued that the frequency resolution in octave band
analysis is too poor to be of much use, especially in analyzing
machine vibration signatures, but it is possible to define
constant percentage band analysis with frequency bands of narrower
width. A common example of this is the one-third-octave spectrum,
whose filter bandwidths are about 27 % of their center frequencies.
Three one-third octave bands span one octave, so the resolution
of such a spectrum is three times better than the octave band
spectrum. One-third octave spectra are frequently used in acoustical
measurements.
A major advantage of constant percentage band analysis is
that a very wide frequency range can be displayed on a single
graph and the frequency resolution at the lower frequencies
can still be fairly narrow. Of course, the frequency resolution
at the highest frequencies suffers, but this is not a problem
for some applications such as fault detection in machines.
In the chapter on machine fault diagnosis, it will be seen
the narrow band spectra are very useful in resolving higher-frequency
harmonics and sidebands, but for the detection of a machine
fault, no such high resolution is required. The vibration velocity
spectra of most machines will be found to slope downwards at
the highest frequencies, and a constant percentage band (CPB)
spectrum of the same data will usually be more uniform in level
over a broad frequency range. This means that a CPB spectrum
takes better advantage of the dynamic range of the instrumentation.
One-third octave spectra are sufficiently narrow at low frequencies
to show the first few harmonics of run speed, and can be used
effectively for the detection of faults if trended over time.
The use of constant CPB spectra for machine monitoring is
not very well recognized in industry with a few notable exceptions
such as the US Navy submarine fleet.
Logarithmic Amplitude Scaling
The spectrum above plots the logarithm of the vibration level
rather than the level itself.
Since this spectrum is on a log amplitude scale, multiplication
by any constant value simply translates the spectrum up on
the screen without changing its shape or the relationship between
the components.
Multiplication of the signal level translates into addition
on a log scale. This means that if the amount of amplification
of a vibration signal is changed, the shape of the spectrum
is not affected. This fact greatly simplifies visual interpretation
of log spectra taken at different amplification factors --
the curves are simply translated up or down on the graph. With
a linear scaling, the shape of the spectrum changes drastically
with different degrees of amplification.
The next spectrum is presented in decibels, a special type
of log scaling that is very important in vibration analysis
Linear and Logarithmic Amplitude Scales
It may seem to be best
to look at vibration spectra with a linear amplitude scale
because that is a true representation
of the actual measured vibration amplitude. Linear amplitude
scaling makes the largest components in a spectrum very easy
to see and to evaluate, but very small components may be
overlooked completely, or are at best difficult to assign a
magnitude
to. The eye is able to see small components about 1/50th
as large as the largest ones in the same spectrum, but anything
smaller than this is essentially lost. In other words, the
dynamic range of the eye is about 50 to 1
Linear scaling may be adequate in cases where the components
are all about the same size, but in the case of machine vibration,
beginning faults in such parts as bearings produce very small
signal amplitudes. If we are to do a good job of trending the
levels of these spectral components, it is best to plot the
logarithm of the amplitude rather than the amplitude itself.
In this way, we can easily display and visually interpret a
dynamic range of at least 5000 to 1, or more than 100 times
better than the linear scaling allows.
To illustrate different types of amplitude presentations,
the same vibration signature will be shown in linear and two
different types of logarithmic amplitude scales.
It might be said that the dynamic range of the eye, when looking
at linear spectra, is about 34 dB.
Linear Amplitude Scaling
Note that this linear spectrum shows the larger peaks very
well, but lower level information is missing. In the case of
machine vibration analysis, we are often interested in the
smaller components of the spectrum, i.e., in the case of rolling
element bearing diagnosis. This subject will be covered in
detail in the chapter on Machine Vibration Monitoring.
The Decibel
The decibel (dB) is defined by the following expression:

where: LdB = The signal level in dB
L1 = Vibration level in Acceleration, Velocity, or Displacement
Lref = Reference level, equivalent to 0 dB
The Bell Telephone Labs introduced the concept of the decibel
before 1930. It was first used to measure relative power
loss and signal to noise ratio in telephone lines. It
was soon pressed into service as a measure of acoustic sound
pressure level.
The vibration velocity level in dB is abbreviated VdB, and
is defined as:
or
The Systeme Internationale, or SI, is the modern replacement for the metric
system.
The reference, or "0 dB" level of 10-9 meter per sec is sufficiently
small that all our measurements on machines will result in positive dB numbers.
this standardized reference level uses the SI, or "metric," system
units, but it is not recognized as a standard in the US and other English-speaking
countries. (The US. Navy and many American industries use a zero dB reference
of 10-8 m/sec, making their readings higher than SI readings by 20 dB.)
The VdB is a logarithmic scaling of vibration magnitude, and
it allows relative measurements to be easily made. Any increase
in level of 6 dB represents a doubling of amplitude, regardless
of the initial level. In like manner, any change of 20 dB represents
a change in level by a factor of ten. Thus any constant ratio
of levels is seen as a certain distance on the scale, regardless
of the absolute levels of the measurements. This makes it very
easy to evaluate trended vibration spectral data; 6 dB increases
always indicate doubling of the magnitudes.
dB Values vs. Amplitude Level Ratios
The following table relates dB values to amplitude ratios:
| dB Change |
Linear Level Ratio |
dB Change |
Linear Level Ratio |
| 0 |
1 |
30 |
31 |
| 3 |
1.4 |
36 |
60 |
| 6 |
2 |
40 |
100 |
| 10 |
3.1 |
50 |
310 |
| 12 |
4 |
60 |
1000 |
| 18 |
8 |
70 |
3100 |
| 20 |
10 |
80 |
10,000 |
| 24 |
16 |
100 |
100,000 |
It is strongly recommended that VdB be used as the vibration
amplitude scaling because so much more information is available
to the viewer compared to linear amplitude units. Also, compared
to a conventional log scale, the dB scale is much easier to
read.
Unit Conversions
Acceleration and Displacement can also be expressed on dB
scales. The AdB scale is the most used one, and its zero reference
is set 1 micro G, commonly abbreviated G.
It turns out that AdB = VdB at 159.2 Hz. VdB levels, AdB levels,
and DdB levels are related by the following formulas:
Any vibration parameter -- displacement, velocity, or acceleration
can be displayed on a dB scale. The reference quantities
for 0 dB on these scales were chosen such that the dB levels
of all three quantities are the same at a frequency of 159.2
Hz, which is equal to 1000 radians per second.

Acceleration and Velocity in linear units are calculated from
dB levels as follows:

It is convenient to remember the following rule of thumb:
At 100 Hz, 1G = 120 AdB = 124 VdB = 2.8 mils p-p.
Note that the time domain wave form is always represented
in linear amplitude units - it is not possible to use a log
scale in the wave form plot because some of the values are
negative, and the logarithm of a negative number is not defined.
VdB Levels vs. Vibration Levels in ips
Peak level is the de facto standard unit for vibration velocity
measurements, even though RMS level would make more sense in
most cases.
Following is a convenient conversion table for relating VdB
levels to inches per second peak:
| VdB |
ips peak |
VdB |
ips peak |
VdB |
ips peak |
| 60
|
.0006 |
90 |
.018 |
120 |
.56 |
| 62 |
.0007 |
92 |
.022 |
122 |
.70 |
| 64 |
.0009 |
94 |
.028 |
124 |
.88 |
| 66 |
.0011 |
96 |
.035 |
126 |
1.1 |
| 68 |
.0014 |
98 |
.044 |
128 |
1.4 |
| 70 |
.0018 |
100 |
.056 |
130 |
1.8 |
| 72 |
.0022 |
102 |
.070 |
132 |
2.2 |
| 74 |
.0028 |
104 |
.088 |
134 |
2.8 |
| 76 |
.0035 |
106 |
.11 |
136 |
3.5 |
| 78 |
.0044 |
108 |
.14 |
138 |
4.4 |
| 80 |
.0056 |
110 |
.18 |
140 |
5.6 |
| 82 |
.0070 |
112 |
.22 |
142 |
7.0 |
| 84 |
.0088 |
114 |
.28 |
144 |
8.8 |
| 86 |
.011 |
116 |
.35 |
146 |
11.1 |
| 88 |
.014 |
118 |
.44 |
148 |
14.0 |
|