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Beginning Vibration 
Analysis 
with 
Basic Fundamentals 
By: Jack Peters
Beginning Vibration 
Jack D. Peters 
2 
Introduction 
Understanding the basics and fundamentals of vibration analysis are 
very important in forming a solid background to analyze problems on 
rotating machinery. 
Switching between time and frequency is a common tool used for 
analysis. Because the frequency spectrum is derived from the data in 
the time domain, the relationship between time and frequency is very 
important. Units of acceleration, velocity, and displacement are 
typical. Additional terms such as peak-peak, peak, and rms. are often 
used. Switching units correctly, and keeping terms straight is a must. 
As much as possible, this training will follow the criteria as established 
by the Vibration Institute.
Mass & Stiffness 
Jack D. Peters 
3 
Mass & Stiffness 
All machines can be broken down 
into two specific categories. 
Mass & Stiffness 
Mass is represented by an object 
that wants to move or rotate. 
Stiffness is represented by springs 
or constraints of that movement.
Mass & Stiffness 
Jack D. Peters 
4 
Mass & Stiffness 
fn = 1/2П k/m 
Where: 
fn = natural frequency (Hz) 
k = stiffness (lb/in) 
m = mass 
mass = weight/gravity 
weight (lb) 
gravity (386.1 in/sec2)
Mass & Stiffness 
Jack D. Peters 
5 
Concept ! 
fn = 1/2П k/m 
If k increases 
Then f increases 
If k decreases 
Then f decreases
Mass & Stiffness 
Jack D. Peters 
6 
Concept ! 
fn = 1/2П k/m 
If m increases 
Then f decreases 
If m decreases 
Then f increases
Spectrum 
Magnitude 
1 
Jack D. Peters 
7 
What’s This ? 
0.0002 
inch 
Peak 
0 
0 Hz 100 Hz
Spectrum 
FFT, Frequency Spectrum, Power Spectrum 
Magnitude 
1 
Jack D. Peters 
8 
0.0002 
inch 
Peak 
0 
0 Hz 100 Hz
Spectrum 
Magnitude 
Jack D. Peters 
9 
Scaling X & Y 
0.0002 
inch 
Peak 
0 
1 
0 Hz 100 Hz 
X 
Y
Spectrum 
Magnitude 
Jack D. Peters 
10 
Scaling X & Y 
0.0002 
inch 
Peak 
0 
1 
0 Hz 100 Hz 
FREQUENCY 
A 
M 
P 
L 
I 
T 
U 
D 
E
Spectrum 
Magnitude 
Jack D. Peters 
11 
Scaling X & Y 
0.0002 
inch 
Peak 
0 
1 
0 Hz 100 Hz 
What is it 
Ho 
w 
Ba 
d 
I 
s 
I 
t
Time Waveform 
Real 
1 
Jack D. Peters 
12 
What’s That ? 
0.0004 
inch 
-0.0004 
0 s 7.996094 s
Time Waveform 
Real 
1 
Jack D. Peters 
13 
Time Waveform 
0.0004 
inch 
-0.0004 
0 s 7.996094 s
Time Waveform 
Real 
Jack D. Peters 
14 
Scaling X & Y 
X 
Y 
0.0004 
inch 
-0.0004 
1 
0 s 7.996094 s
Time Waveform 
Real 
Jack D. Peters 
15 
Scaling X & Y 
TIME 
A 
M 
P 
L 
I 
T 
U 
D 
E 
0.0004 
inch 
-0.0004 
1 
0 s 7.996094 s
Time Waveform 
Real 
Jack D. Peters 
16 
Scaling X & Y 
What is it 
Ho 
w 
Ba 
d 
I 
s 
I 
t 
0.0004 
inch 
-0.0004 
1 
0 s 7.996094 s
Time Waveform 
Real 
Jack D. Peters 
17 
Scaling X & Y 
What is it 
Ho 
w 
Ba 
d 
I 
s 
I 
t 
0.0004 
inch 
-0.0004 
1 
0 s 1 s
Time & Frequency 
Magnitude 
Real 
1 
1 
Jack D. Peters 
18 
Double Trouble 
0.0004 
inch 
-0.0004 
0 s 7.996094 s 
0.0002 
inch 
Peak 
0 
0 Hz 100 Hz
The X Scale 
Jack D. Peters 
19 
The X Scale
The X Scale 
Jack D. Peters 
20 
Hertz (Hz) 
One Hertz (Hz) is equal to 1 cycle / second 
It is the most common term used in vibration 
analysis to describe the frequency of a disturbance. 
Never forget the 1 cycle / second relationship ! 
Traditional vibration analysis quite often expresses 
frequency in terms of cycle / minute (cpm). This is 
because many pieces of process equipment have 
running speeds related to revolutions / minute (rpm). 
60 cpm = 1 cps = 1 Hz
The X Scale 
Relationship with Time 
The frequency domain is an expression of amplitude 
and individual frequencies. 
A single frequency can be related to time. 
Jack D. Peters 
21 
F(Hz) = 1 / T(s) 
The inverse of this is also true for a single frequency. 
T(s) = 1 / F(Hz) 
Keep in mind that the time domain is an expression 
of amplitude and multiple frequencies.
The X Scale 
Jack D. Peters 
22 
Concept ! 
If: F = 1/T and T = 1/F 
Then: FT = 1
The X Scale 
Jack D. Peters 
23 
Concept ! 
FT = 1 
If: F increases 
Then: T decreases 
If: T increases 
Then: F decreases
The X Scale 
Single Frequency 
Magnitude 
X:55 Hz Y:706.8129 mV 
Pwr Spec 1 
Real 
X:27.00806 ms Y:3.579427 mV 
dX:18.18848 ms dY:2.449082 mV 
Time 1 
Jack D. Peters 
24 
1V 
rms 
0 
0 Hz 100 Hz 
1V 
-1 
0 s 62.46948 ms
The X Scale 
Multiple Frequencies 
X:55 Hz Y:706.8129 mV 
1 
0 Hz 100 Hz 
X:78 Hz Y:706.9236 mV 
Pwr Spec 1 
X:21 Hz Y:706.7825 mV 
Pwr Spec 1 
X:42 Hz Y:706.9266 mV 
Pwr Spec 1 
Jack D. Peters 
25 
Pwr Spec 1 
1 
0 Hz 100 Hz 
1 
0 Hz 100 Hz 
1 
0 Hz 100 Hz
The X Scale 
Time 55 1 
Time 78 1 
Time 21 1 
Time 42 1 
Jack D. Peters 
26 
Multiple Time 
1V 
0 s 62.46948 ms 
1V 
0 s 62.46948 ms 
1V 
0 s 62.46948 ms 
1V 
0 s 62.46948 ms
The X Scale 
Real 
55 + 78 + 21 + 42 = Trouble ! 
TIME 1 
Jack D. Peters 
27 
Real Life Time 
4V 
-4 
0 s 62.46948 ms
The X Scale 
Frequency Spectrum 
Real 
TIME 1 
X:21 Hz Y:706.7825 mV 
X:42 Hz Y:706.9266 mV 
X:55 Hz Y:706.8129 mV 
X:78 Hz Y:706.9236 mV 
FREQUENCY 1 
Jack D. Peters 
28 
4V 
-4 
0 s 62.46948 ms 
1V 
rms 
0 Hz 100 Hz
The X Scale 
The Most Copied Slide in the History of Vibration Analysis ! 
Jack D. Peters 
29 
Amplitude 
Input Time 
Frequency 
Time Waveform 
Spectrum
The X Scale 
Lines of Resolution 
Jack D. Peters 
30 
0.0002 
inch 
Peak 
Magnitude 
0 
1 
0 Hz 100 Hz 
The FFT always 
has a defined 
number of lines 
of resolution. 
100, 200, 400, 
800, 1600, and 
3200 lines are 
common 
choices. 
This spectrum 
has 800 lines, or 
the X scale is 
broken down into 
800 points.
The X Scale 
Jack D. Peters 
31 
Filter Windows 
• Window filters are applied to the time 
waveform data to simulate data that 
starts and stops at zero. 
• They will cause errors in the time 
waveform and frequency spectrum. 
• We still like window filters !
The X Scale 
Window Comparisons 
Jack D. Peters 
32
The X Scale 
(Frequency Response) 
Jack D. Peters 
33 
Filter Windows 
• Hanning (Frequency) 
• Flat Top (Amplitude) 
• Uniform (No Window) 
• Force Exponential 
• Force/Expo Set-up 
Hanning 16% Amplitude Error 
Flat Top 1% Amplitude Error 
Window functions courtesy of Agilent 
“The Fundamentals of Signal Analysis” 
Application Note #AN 243
The X Scale 
Jack D. Peters 
34 
Filter Windows 
• Use the Hanning Window for normal 
vibration monitoring (Frequency) 
• Use the Flat Top Window for calibration 
and accuracy (Amplitude) 
• Use the Uniform Window for bump 
testing and resonance checks (No 
Window)
The X Scale 
Minimum Derived Hz 
The minimum derived frequency is determined by: 
Frequency Span / Number of Analyzer Lines (data points) 
The frequency span is calculated as the ending 
frequency minus the starting frequency. 
The number of analyzer lines depends on the analyzer 
and how the operator has set it up. 
Example: 0 - 400 Hz using 800 lines 
Answer = (400 - 0) / 800 = 0.5 Hz / Line 
Jack D. Peters 
35
The X Scale 
Jack D. Peters 
Note: More discussion 
later on window functions 
for the analyzer ! 
36 
Bandwidth 
The Bandwidth can be defined by: 
(Frequency Span / Analyzer Lines) Window Function 
Uniform Window Function = 1.0 
Hanning Window Function = 1.5 
Flat Top Window Function = 3.5 
Example: 0 - 400 Hz using 800 Lines & Hanning Window 
Answer = (400 / 800) 1.5 = 0.75 Hz / Line
The X Scale 
Jack D. Peters 
37 
Resolution 
The frequency resolution is defined in the following 
manner: 
2 (Frequency Span / Analyzer Lines) Window Function 
or 
Resolution = 2 (Bandwidth) 
Example: 0 - 400 Hz using 800 Lines & Hanning Window 
Answer = 2 (400 / 800) 1.5 = 1.5 Hz / Line
The X Scale 
Using Resolution 
The student wishes to measure two frequency 
disturbances that are very close together. 
Frequency #1 = 29.5 Hz. 
Frequency #2 = 30 Hz. 
The instructor suggests a hanning window and 800 lines. 
What frequency span is required to accurately measure 
these two frequency disturbances ? 
Jack D. Peters 
38
The X Scale 
Using Resolution 
Resolution = 30 - 29.5 = 0.5 Hz / Line 
Resolution = 2 (Bandwidth) 
BW = (Frequency Span / Analyzer Lines) Window Function 
Resolution = 2 (Frequency Span / 800) 1.5 
0.5 = 2 (Frequency Span / 800) 1.5 
0.5 = 3 (Frequency Span) / 800 
400 = 3 (Frequency Span) 
133 Hz = Frequency Span 
Jack D. Peters 
39
The X Scale 
Data Sampling Time 
Data sampling time is the amount of time required to take 
one record or sample of data. It is dependent on the 
frequency span and the number of analyzer lines being used. 
Jack D. Peters 
40 
TSample = Nlines / Fspan 
Using 400 lines with a 800 Hz frequency span will require: 
400 / 800 = 0.5 seconds
The X Scale 
Average & Overlap 
Jack D. Peters 
41 
• Average - On 
• Overlap Percent - 50% 
TR#1 TR#2 TR#3 
FFT#1 FFT#2 FFT#3 
TR#1 
TR#2 
TR#3 
FFT#1 
0% Overlap 
50% Overlap 
FFT#2 
FFT#3 
How long will it take for 10 
averages at 75% overlap 
using a 800 line analyzer and 
a 200 Hz frequency span?
The X Scale 
Jack D. Peters 
42 
75% Overlap ? 
• 10 Averages 
• 75% Overlap 
• 800 Lines 
• 200 Hz 
Average #1 = 800 / 200 
Average #1 = 4 seconds 
Average #2 - #10 = (4 x 0.25) 
Average #2 - #10 = 1 second 
each 
Total time = 4 + (1 x 9) 
Total time = 13 seconds
The Y Scale 
Jack D. Peters 
43 
The Y Scale
The Y Scale 
Jack D. Peters 
44 
Amplitude 
The “Y” scale provides the amplitude value for each 
signal or frequency. 
Default units for the “Y” scale are volts RMS. 
Volts is an Engineering Unit (EU). 
RMS is one of three suffixes meant to confuse you ! 
The other two are: 
(Peak) and (Peak - Peak)
The Y Scale 
Pk-Pk (Peak - Peak) 
Jack D. Peters 
X:55 Hz Y:1.999169 V 
X:22.43042 ms Y:-993.8563 mV 
45 
Magnitude 
1V 
Real 
-1 
Pwr Spec 1 
Time 1 
0 s 62.46948 ms 
2V 
Pk-Pk 
0 
0 Hz 100 Hz 
dX:9.094238 ms dY:1.994871 V 
The Peak - Peak value 
is expressed from the 
peak to peak amplitude. 
The spectrum value 
uses the suffix “Pk-Pk” 
to denote this.
The Y Scale 
The time wave has not X:55 Hz Y:999.5843 mV 
changed. The Peak 
value is expressed 
from zero to the peak 
amplitude. 
The spectrum value 
uses the suffix “Peak” 
to denote this. 
Jack D. Peters 
X:27.00806 ms Y:3.579427 mV 
46 
Pk (Peak) 
Magnitude 
1V 
Real 
-1 
Pwr Spec 1 
Time 1 
0 s 62.46948 ms 
1V 
Peak 
0 
0 Hz 100 Hz 
dX:4.516602 ms dY:997.4356 mV
The Y Scale 
RMS (Root Mean Square) 
Jack D. Peters 
X:55 Hz Y:706.8129 mV 
X:27.00806 ms Y:3.579427 mV 
dX:2.288818 ms dY:709.1976 mV 
47 
1V 
rms 
Magnitude 
0 
Pwr Spec 1 
0 Hz 100 Hz 
1V 
Real 
-1 
Time 1 
0 s 62.46948 ms 
The time wave has 
not changed. The 
RMS value is 
expressed from zero 
to 70.7% of the peak 
amplitude. 
The spectrum value 
uses the suffix 
“RMS” to denote this.
The Y Scale 
Suffix Comparison 
Jack D. Peters 
Pwr Spec 1 
Pwr Spec 1 
Pwr Spec 1 
48 
2 
V 
rms 
Magnitude 
0 
0 Hz 100 Hz 
2 
V 
Peak 
Magnitude 
0 
0 Hz 100 Hz 
2 
V 
Pk-Pk 
Magnitude 
0 
0 Hz 100 Hz 
1 
V 
Real 
-1 
X:27.00806 ms Y:3.579427 mV 
Time 1 
0 s 62.46948 ms 
1 
V 
Real 
-1 
X:27.00806 ms Y:3.579427 mV 
Time 1 
0 s 62.46948 ms 
1 
V 
Real 
-1 
X:22.43042 ms Y:-993.8563 mV 
Time 1 
0 s 62.46948 ms 
X:55 Hz Y:706.8129 mV 
X:55 Hz Y:999.5843 mV 
X:55 Hz Y:1.999169 V 
dX:2.288818 ms dY:709.1976 m 
dX:4.516602 ms dY:997.4356 m 
dX:9.094238 ms dY:1.994871 V 
RMS 
Peak 
Peak - Peak
The Y Scale 
Changing Suffixes 
Many times it is necessary to change between suffixes. 
Jack D. Peters 
49 
Pk-Pk / 2 = Peak 
Peak x 0.707 = RMS 
RMS x 1.414 = Peak 
Peak x 2 = Pk-Pk
The Y Scale 
Standard Suffixes 
Now that we have learned all about the three 
standard suffixes that might possibly confuse the 
“Y” scale values, what is the standard ? 
Vibration Institute: 
Displacement = mils Peak - Peak 
Velocity = in/s Peak or rms.. 
Acceleration = g’s Peak or rms.. 
Note: 1 mil = 0.001 inches 
Jack D. Peters 
50
The Y Scale 
Engineering Units (EU) 
Engineering units are used to give meaning to the 
amplitude of the measurement. 
Instead of the default “volts”, it is possible to incorporate 
a unit proportional to volts that will have greater 
meaning to the user. 
Examples: 100 mV / g 20 mV / Pa 
Jack D. Peters 
1 V / in/s 200 mV / mil 
50 mV / psi 10 mV / fpm 
33 mV / % 10 mV / V 
51
The Y Scale 
EU’s the Hard Way 
Sometimes we forget to use EU’s, or just don’t understand how 
to set up the analyzer. 
There is no immediate need to panic if ???? 
You know what the EU is for the sensor you are using. 
Example: An accelerometer outputs 100 mV / g and there is a 
10 mV peak in the frequency spectrum. 
What is the amplitude in g’s ? 
Answer = 10 mV / 100 mV = 0.1 g 
Jack D. Peters 
52
The Y Scale 
The Big Three EU’s 
Acceleration 
Velocity 
Displacement 
Jack D. Peters 
53
The Y Scale 
Converting the Big 3 
In many cases we are confronted with Acceleration, 
Velocity, or Displacement, but are not happy with it. 
Maybe we have taken the measurement in 
acceleration, but the model calls for displacement. 
Maybe we have taken the data in displacement, but 
the manufacturer quoted the equipment 
specifications in velocity. 
How do we change between these EU’s ? 
Jack D. Peters 
54
The Y Scale 
Jack D. Peters 
55 
386.1 What ? 
1g = 32.2 feet/second2 
32.2 feet 12 inches 
second2 X foot 
386.1 inches/second2 
g
The Y Scale 
Go With The Flow I 
÷ 386.1 
x 2(Pi)f 
Jack D. Peters 
56 
Acceleration (g’s) 
Velocity (inch/s) 
Displacement (inch) 
x 386.1 
÷ 2(Pi)f 
x 2(Pi)f ÷ 2(Pi)f
The Y Scale 
Metric Go With The Flow I 
÷ 9807 
x 2(Pi)f 
Jack D. Peters 
57 
Acceleration (g’s) 
Velocity (mm/s) 
Displacement (mm) 
x 9807 
÷ 2(Pi)f 
x 2(Pi)f ÷ 2(Pi)f
The Y Scale 
Go With The Flow II 
x 2 
Jack D. Peters 
58 
Peak - Peak 
Peak 
RMS 
÷ 2 
x 1.414 x .707
The Y Scale 
Doing the Math Units 
Jack D. Peters 
0.5g x 386.1 inches 
second2 
g 
2π x 25 cycles 
59 
second 
0.5g x 386.1 inches x 1 second 
g second2 2π x 25 cycles 
0.5 x 386.1 inches 
2π x 25 cycles second 
cycle 
1.23 inches/second 
There is a 0.5 g 
vibration at 25 Hz. 
What is the velocity ?
The Y Scale 
Acceleration - Velocity 
Example: Find the equivalent peak velocity for a 25 Hz 
Jack D. Peters 
60 
vibration at 7 mg RMS ? 
= (g x 386.1) / (2 Pi x F) 
= (0.007 x 386.1) / (6.28 x 25) 
= 0.017 inches / second RMS 
Answer = 0.017 x 1.414 = 0.024 inches / second Pk
The Y Scale 
Velocity - Displacement 
Example: Find the equivalent pk-pk displacement for a 
Jack D. Peters 
61 
25 Hz vibration at 0.024 in/s Pk ? 
= Velocity / (2 Pi x F) 
= 0.024 / (6.28 x 25) 
= 0.000153 inches Pk 
Answer = 0.000153 x 2 = 0.000306 inches Pk-Pk
The Y Scale 
Acceleration - Displacement 
Example: Find the equivalent Pk-Pk displacement for a 
Jack D. Peters 
62 
52 Hz vibration at 15 mg RMS ? 
= (g x 386.1) / (2 Pi x F)2 
= (0.015 x 386.1) / (6.28 x 52)2 
= 0.000054 inches RMS 
Answer = (0.000054 x 1.414) 2 = 0.000154 inches Pk-Pk
Sensors 
Jack D. Peters 
63 
Sensors
Sensors 
Jack D. Peters 
64 
Accelerometers 
• Integrated Circuit 
¾Electronics inside 
¾Industrial 
• Charge Mode 
¾ Charge Amplifier 
¾ Test & Measurement
Sensors 
Accelerometer Advantages 
• Measures casing vibration 
• Measures absolute motion 
• Can integrate to Velocity output 
• Easy to mount 
• Large range of frequency response 
• Available in many configurations 
Jack D. Peters 
65
Sensors 
Accelerometer Disadvantages 
• Does not measure shaft vibration 
• Sensitive to mounting techniques and 
surface conditions 
• Difficult to perform calibration check 
• Double integration to displacement often 
causes low frequency noise 
• One accelerometer does not fit all 
applications 
Jack D. Peters 
66
Sensors 
Jack D. Peters 
Relative movement 
between post & 
mass creates shear 
in ceramic 
producing charge. 
67 
Mass & Charge 
Mass 
Ceramic/Quartz 
Post
Sensors 
Accelerometer Parameters 
Performance Suited for Application 
Sensitivity (mV/g) 
Frequency Response of target (f span) 
Dynamic Range of target (g level) 
Jack D. Peters 
68
Sensors 
Mounting the Accelerometer 
500 2000 6,500 10,000 15,000 15,000 
Jack D. Peters 
69 
Hz.
Sensors 
Realistic Mounting 
Jack D. Peters 
70 
Stud 
Bees Wax 
Adhesive 
Magnet 
Hand Held 
100 1,000 10,000 
Frequency, Hz 
In the real world, 
mounting might 
not be as good as 
the manufacturer 
had in the lab ! 
What happened 
to the high 
frequency ?
Sensors 
Mounting Location 
Jack D. Peters 
Axial 
71 
Horizontal 
Vertical 
¾Load Zone 
¾Radial 
9Vertical 
9Horizontal 
¾Axial
Sensors 
Mounting Location 
Jack D. Peters 
72 
¾Load Zone 
¾Radial 
9Vertical 
9Horizontal 
¾Axial
Sensors 
Accelerometer Alarms 
Jack D. Peters 
Velocity Limit 
73 
Machine Condition 
rms peak 
Acceptance of new or repaired equipment < 0.08 < 0.16 
Unrestricted operation (normal) < 0.12 < 0.24 
Surveillance 0.12 - 0.28 0.24 - 0.7 
Unsuitable for Operation > 0.28 > 0.7 
Note #1: The rms velocity (in/sec) is the band power or 
band energy calculated in the frequency spectrum. 
Note #2: The peak velocity (in/sec) is the largest positive 
or negative peak measured in the time waveform.
Sensors 
Proximity Probes 
Jack D. Peters 
74
Sensors 
Proximity Probe Theory 
Cable 
Jack D. Peters 
75 
Driver 
Target 
Probe 
The tip of the probe broadcasts a radio frequency signal 
into the surrounding area as a magnetic field. 
If a conductive target intercepts the magnetic field, eddy 
currents are generated on the surface of the target, and 
power is drained from the radio frequency signal. 
As the power varies with target movement in the radio 
frequency field, the output voltage of the driver also 
varies. 
A small dc voltage indicates that the target is close to the 
probe tip. 
A large dc voltage indicates that the target is far away 
from the probe tip. 
The variation of dc voltage is the dynamic signal 
indicating the vibration or displacement.
Sensors 
Jack D. Peters 
76 
Output Values 
• Typical 
– 100 mv/mil 
– 200 mv/mil 
• Depends on 
probe, cable 
(length), and 
driver. 
• Target material 
varies output. 
Calibration Examples 
• Copper 380 mV/mil 
• Aluminum 370 mV/mil 
• Brass 330 mV/mil 
• Tungsten Carbide 290 mV/mil 
• Stainless Steel 250 mV/mil 
• Steel 4140, 4340 200 mV/mil 
Based on typical output sensitivity 
of 200 mV/mil.
Sensors 
Proximity Probes - Advantages 
• Non-contact 
• Measure shaft dynamic motion 
• Measure shaft static position (gap) 
• Flat frequency response dc – 1KHz 
• Simple calibration 
• Suitable for harsh environments 
Jack D. Peters 
77
Sensors 
Proximity Probes - Disadvantages 
• Probe can move (vibrate) 
• Doesn’t work on all metals 
• Plated shafts may give false measurement 
• Measures nicks & tool marks in shaft 
• Must be replaced as a unit (probe, cable & 
driver) 
• Must have relief at sensing tip from 
surrounding metal 
Jack D. Peters 
78
Sensors 
Typical Mounting 
Jack D. Peters 
79 
vertical probe horizontal probe 
H 
V 
time 
Facing Driver to Driven 
(independent of rotation)
Sensors 
Looking at Orbits 
Jack D. Peters 
80 
Vertical for 
Amplitude 
Horizontal for 
Time Base
Sensors 
The Orbit Display 
Jack D. Peters 
81 
ils 
Mils 
Mils
Sensors 
Jack D. Peters 
82 
Unbalance
Sensors 
Unbalance with Orbit 
Jack D. Peters 
83
Sensors 
Jack D. Peters 
84 
Misalignment
Sensors 
Misalignment with Orbit 
Jack D. Peters 
85
Sensors 
And the problem is ? 
Jack D. Peters 
86
Sensors 
Proximity Probe Alarms 
Jack D. Peters 
Allowable R/C 
87 
Machine Condition 
< 3,600 RPM < 10,000 RPM 
Normal 0.3 0.2 
Surveillance 0.3 - 0.5 0.2 - 0.4 
Planned Shutdown 0.5 0.4 
Unsuitable for Operation 0.7 0.6 
Note #1: R is the relative displacement of the shaft 
measured by either probe in mils peak-peak. 
Note #2: C is the diametrical clearance (difference 
between shaft OD and journal ID) measured in mils.
Sensors 
Analyzer Input - Front End 
AC coupling will block the DC voltage. 
It creates an amplitude error below 1 
Hz. DC coupling has no error below 1 
Hz, but the analyzer must range on the 
total signal amplitude. 
Jack D. Peters 
88 
• Coupling - AC, DC 
• Antialias Filter - On, Off 
Prevents frequencies that are greater 
than span from wrapping around in 
the spectrum. 
Analyzer Input Capacitor 
Blocks DC 
AC Coupling Capacitor in DSA 
If the antialias filter is turned off, at what 
frequency will 175 Hz. appear using a 0 - 
100 Hz span, and 800 lines ? 
1024/800 = 1.28 
100 x 1.28 = 128 Hz 
175 Hz - 128 Hz = 47 Hz. 
128 Hz - 47 Hz = 81 Hz
Sensors 
Low End Frequency Response 
Jack D. Peters 
X:500 mHz Y:720.0918 m 
X:2.8125 Hz Y:984.7542 m 
X:5.34375 Hz Y:1.000001 
89 
0.01 
V 
rms 
Magnitude 
0.002 
Input 1 
0 Hz 25 Hz 
0.01 
V 
rms 
Magnitude 
0 
Output 2 
0 Hz 25 Hz 
2 
Magnitude 
0 
Freq Resp 2:1 
0 Hz 25 Hz 
1.1 
Magnitude 
0.9 
Coherence 2:1 
0 Hz 25 Hz 
To the right is a typical 
problem with frequency 
response at the low end of 
the frequency spectrum. 
This low end roll off was a 
result of AC coupling on 
CH #2 of the analyzer. 
Values below 2.8 Hz are in 
error, and values less than 
0.5 Hz should not be used.
Data Collection 
Jack D. Peters 
90 
Data Collection
Data Collection 
Tape Recorders “Insurance Policy” 
Jack D. Peters 
Multi-channel 
digital audio tape 
recorders. 
91 
For the 
Measurement that 
can’t get away !
Data Collection 
Dynamic Signal Analyzers “Test & Measurement” 
Jack D. Peters 
Large PC driven solutions 
with multiple channels and 
windows based software. 
92 
Smaller portable units 
with 2 – 4 channel 
inputs and firmware 
operating systems.
Data Collection 
Data Collectors “Rotating Equipment” 
Jack D. Peters 
93
Data Collection 
Data Collectors “Rotating Equipment” 
Jack D. Peters 
94 
• Route Based 
• Frequency 
Spectrum 
• Time Waveform 
• Orbits 
• Balancing 
• Alignment 
• Data Analysis 
• History 
• Trending 
• Download to PC 
• Alarms 
• “Smart” algorithms
Beginning Vibration 
Jack D. Peters 
95 
Bibliography 
• Eisenmann, Robert Sr. & Eisenmann, Robert Jr., Machinery 
Malfunction Diagnosis and Correction, ISBN 0-13-240946-1 
• Eshleman, Ronald L., Basic Machinery Vibrations, ISBN 0- 
9669500-0-3 
• LaRocque, Thomas, Vibration Analysis Design, Selection, 
Mounting, and Installation, Application Note, Connection 
Technology Center 
• Agilent Technologies, The Fundamentals of Signal Analysis, 
Application note 243 
• Agilent Technologies, Effective Machinery Measurements using 
Dynamic Signal Analyzers, Application note 243-1
Beginning Vibration 
Jack D. Peters 
96 
Thank You ! 
You can find technical papers on 
this and other subjects at 
www.ctconline.com 
in the “Technical Resources” section

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01 beginning vibration analysis

  • 1. Beginning Vibration Analysis with Basic Fundamentals By: Jack Peters
  • 2. Beginning Vibration Jack D. Peters 2 Introduction Understanding the basics and fundamentals of vibration analysis are very important in forming a solid background to analyze problems on rotating machinery. Switching between time and frequency is a common tool used for analysis. Because the frequency spectrum is derived from the data in the time domain, the relationship between time and frequency is very important. Units of acceleration, velocity, and displacement are typical. Additional terms such as peak-peak, peak, and rms. are often used. Switching units correctly, and keeping terms straight is a must. As much as possible, this training will follow the criteria as established by the Vibration Institute.
  • 3. Mass & Stiffness Jack D. Peters 3 Mass & Stiffness All machines can be broken down into two specific categories. Mass & Stiffness Mass is represented by an object that wants to move or rotate. Stiffness is represented by springs or constraints of that movement.
  • 4. Mass & Stiffness Jack D. Peters 4 Mass & Stiffness fn = 1/2П k/m Where: fn = natural frequency (Hz) k = stiffness (lb/in) m = mass mass = weight/gravity weight (lb) gravity (386.1 in/sec2)
  • 5. Mass & Stiffness Jack D. Peters 5 Concept ! fn = 1/2П k/m If k increases Then f increases If k decreases Then f decreases
  • 6. Mass & Stiffness Jack D. Peters 6 Concept ! fn = 1/2П k/m If m increases Then f decreases If m decreases Then f increases
  • 7. Spectrum Magnitude 1 Jack D. Peters 7 What’s This ? 0.0002 inch Peak 0 0 Hz 100 Hz
  • 8. Spectrum FFT, Frequency Spectrum, Power Spectrum Magnitude 1 Jack D. Peters 8 0.0002 inch Peak 0 0 Hz 100 Hz
  • 9. Spectrum Magnitude Jack D. Peters 9 Scaling X & Y 0.0002 inch Peak 0 1 0 Hz 100 Hz X Y
  • 10. Spectrum Magnitude Jack D. Peters 10 Scaling X & Y 0.0002 inch Peak 0 1 0 Hz 100 Hz FREQUENCY A M P L I T U D E
  • 11. Spectrum Magnitude Jack D. Peters 11 Scaling X & Y 0.0002 inch Peak 0 1 0 Hz 100 Hz What is it Ho w Ba d I s I t
  • 12. Time Waveform Real 1 Jack D. Peters 12 What’s That ? 0.0004 inch -0.0004 0 s 7.996094 s
  • 13. Time Waveform Real 1 Jack D. Peters 13 Time Waveform 0.0004 inch -0.0004 0 s 7.996094 s
  • 14. Time Waveform Real Jack D. Peters 14 Scaling X & Y X Y 0.0004 inch -0.0004 1 0 s 7.996094 s
  • 15. Time Waveform Real Jack D. Peters 15 Scaling X & Y TIME A M P L I T U D E 0.0004 inch -0.0004 1 0 s 7.996094 s
  • 16. Time Waveform Real Jack D. Peters 16 Scaling X & Y What is it Ho w Ba d I s I t 0.0004 inch -0.0004 1 0 s 7.996094 s
  • 17. Time Waveform Real Jack D. Peters 17 Scaling X & Y What is it Ho w Ba d I s I t 0.0004 inch -0.0004 1 0 s 1 s
  • 18. Time & Frequency Magnitude Real 1 1 Jack D. Peters 18 Double Trouble 0.0004 inch -0.0004 0 s 7.996094 s 0.0002 inch Peak 0 0 Hz 100 Hz
  • 19. The X Scale Jack D. Peters 19 The X Scale
  • 20. The X Scale Jack D. Peters 20 Hertz (Hz) One Hertz (Hz) is equal to 1 cycle / second It is the most common term used in vibration analysis to describe the frequency of a disturbance. Never forget the 1 cycle / second relationship ! Traditional vibration analysis quite often expresses frequency in terms of cycle / minute (cpm). This is because many pieces of process equipment have running speeds related to revolutions / minute (rpm). 60 cpm = 1 cps = 1 Hz
  • 21. The X Scale Relationship with Time The frequency domain is an expression of amplitude and individual frequencies. A single frequency can be related to time. Jack D. Peters 21 F(Hz) = 1 / T(s) The inverse of this is also true for a single frequency. T(s) = 1 / F(Hz) Keep in mind that the time domain is an expression of amplitude and multiple frequencies.
  • 22. The X Scale Jack D. Peters 22 Concept ! If: F = 1/T and T = 1/F Then: FT = 1
  • 23. The X Scale Jack D. Peters 23 Concept ! FT = 1 If: F increases Then: T decreases If: T increases Then: F decreases
  • 24. The X Scale Single Frequency Magnitude X:55 Hz Y:706.8129 mV Pwr Spec 1 Real X:27.00806 ms Y:3.579427 mV dX:18.18848 ms dY:2.449082 mV Time 1 Jack D. Peters 24 1V rms 0 0 Hz 100 Hz 1V -1 0 s 62.46948 ms
  • 25. The X Scale Multiple Frequencies X:55 Hz Y:706.8129 mV 1 0 Hz 100 Hz X:78 Hz Y:706.9236 mV Pwr Spec 1 X:21 Hz Y:706.7825 mV Pwr Spec 1 X:42 Hz Y:706.9266 mV Pwr Spec 1 Jack D. Peters 25 Pwr Spec 1 1 0 Hz 100 Hz 1 0 Hz 100 Hz 1 0 Hz 100 Hz
  • 26. The X Scale Time 55 1 Time 78 1 Time 21 1 Time 42 1 Jack D. Peters 26 Multiple Time 1V 0 s 62.46948 ms 1V 0 s 62.46948 ms 1V 0 s 62.46948 ms 1V 0 s 62.46948 ms
  • 27. The X Scale Real 55 + 78 + 21 + 42 = Trouble ! TIME 1 Jack D. Peters 27 Real Life Time 4V -4 0 s 62.46948 ms
  • 28. The X Scale Frequency Spectrum Real TIME 1 X:21 Hz Y:706.7825 mV X:42 Hz Y:706.9266 mV X:55 Hz Y:706.8129 mV X:78 Hz Y:706.9236 mV FREQUENCY 1 Jack D. Peters 28 4V -4 0 s 62.46948 ms 1V rms 0 Hz 100 Hz
  • 29. The X Scale The Most Copied Slide in the History of Vibration Analysis ! Jack D. Peters 29 Amplitude Input Time Frequency Time Waveform Spectrum
  • 30. The X Scale Lines of Resolution Jack D. Peters 30 0.0002 inch Peak Magnitude 0 1 0 Hz 100 Hz The FFT always has a defined number of lines of resolution. 100, 200, 400, 800, 1600, and 3200 lines are common choices. This spectrum has 800 lines, or the X scale is broken down into 800 points.
  • 31. The X Scale Jack D. Peters 31 Filter Windows • Window filters are applied to the time waveform data to simulate data that starts and stops at zero. • They will cause errors in the time waveform and frequency spectrum. • We still like window filters !
  • 32. The X Scale Window Comparisons Jack D. Peters 32
  • 33. The X Scale (Frequency Response) Jack D. Peters 33 Filter Windows • Hanning (Frequency) • Flat Top (Amplitude) • Uniform (No Window) • Force Exponential • Force/Expo Set-up Hanning 16% Amplitude Error Flat Top 1% Amplitude Error Window functions courtesy of Agilent “The Fundamentals of Signal Analysis” Application Note #AN 243
  • 34. The X Scale Jack D. Peters 34 Filter Windows • Use the Hanning Window for normal vibration monitoring (Frequency) • Use the Flat Top Window for calibration and accuracy (Amplitude) • Use the Uniform Window for bump testing and resonance checks (No Window)
  • 35. The X Scale Minimum Derived Hz The minimum derived frequency is determined by: Frequency Span / Number of Analyzer Lines (data points) The frequency span is calculated as the ending frequency minus the starting frequency. The number of analyzer lines depends on the analyzer and how the operator has set it up. Example: 0 - 400 Hz using 800 lines Answer = (400 - 0) / 800 = 0.5 Hz / Line Jack D. Peters 35
  • 36. The X Scale Jack D. Peters Note: More discussion later on window functions for the analyzer ! 36 Bandwidth The Bandwidth can be defined by: (Frequency Span / Analyzer Lines) Window Function Uniform Window Function = 1.0 Hanning Window Function = 1.5 Flat Top Window Function = 3.5 Example: 0 - 400 Hz using 800 Lines & Hanning Window Answer = (400 / 800) 1.5 = 0.75 Hz / Line
  • 37. The X Scale Jack D. Peters 37 Resolution The frequency resolution is defined in the following manner: 2 (Frequency Span / Analyzer Lines) Window Function or Resolution = 2 (Bandwidth) Example: 0 - 400 Hz using 800 Lines & Hanning Window Answer = 2 (400 / 800) 1.5 = 1.5 Hz / Line
  • 38. The X Scale Using Resolution The student wishes to measure two frequency disturbances that are very close together. Frequency #1 = 29.5 Hz. Frequency #2 = 30 Hz. The instructor suggests a hanning window and 800 lines. What frequency span is required to accurately measure these two frequency disturbances ? Jack D. Peters 38
  • 39. The X Scale Using Resolution Resolution = 30 - 29.5 = 0.5 Hz / Line Resolution = 2 (Bandwidth) BW = (Frequency Span / Analyzer Lines) Window Function Resolution = 2 (Frequency Span / 800) 1.5 0.5 = 2 (Frequency Span / 800) 1.5 0.5 = 3 (Frequency Span) / 800 400 = 3 (Frequency Span) 133 Hz = Frequency Span Jack D. Peters 39
  • 40. The X Scale Data Sampling Time Data sampling time is the amount of time required to take one record or sample of data. It is dependent on the frequency span and the number of analyzer lines being used. Jack D. Peters 40 TSample = Nlines / Fspan Using 400 lines with a 800 Hz frequency span will require: 400 / 800 = 0.5 seconds
  • 41. The X Scale Average & Overlap Jack D. Peters 41 • Average - On • Overlap Percent - 50% TR#1 TR#2 TR#3 FFT#1 FFT#2 FFT#3 TR#1 TR#2 TR#3 FFT#1 0% Overlap 50% Overlap FFT#2 FFT#3 How long will it take for 10 averages at 75% overlap using a 800 line analyzer and a 200 Hz frequency span?
  • 42. The X Scale Jack D. Peters 42 75% Overlap ? • 10 Averages • 75% Overlap • 800 Lines • 200 Hz Average #1 = 800 / 200 Average #1 = 4 seconds Average #2 - #10 = (4 x 0.25) Average #2 - #10 = 1 second each Total time = 4 + (1 x 9) Total time = 13 seconds
  • 43. The Y Scale Jack D. Peters 43 The Y Scale
  • 44. The Y Scale Jack D. Peters 44 Amplitude The “Y” scale provides the amplitude value for each signal or frequency. Default units for the “Y” scale are volts RMS. Volts is an Engineering Unit (EU). RMS is one of three suffixes meant to confuse you ! The other two are: (Peak) and (Peak - Peak)
  • 45. The Y Scale Pk-Pk (Peak - Peak) Jack D. Peters X:55 Hz Y:1.999169 V X:22.43042 ms Y:-993.8563 mV 45 Magnitude 1V Real -1 Pwr Spec 1 Time 1 0 s 62.46948 ms 2V Pk-Pk 0 0 Hz 100 Hz dX:9.094238 ms dY:1.994871 V The Peak - Peak value is expressed from the peak to peak amplitude. The spectrum value uses the suffix “Pk-Pk” to denote this.
  • 46. The Y Scale The time wave has not X:55 Hz Y:999.5843 mV changed. The Peak value is expressed from zero to the peak amplitude. The spectrum value uses the suffix “Peak” to denote this. Jack D. Peters X:27.00806 ms Y:3.579427 mV 46 Pk (Peak) Magnitude 1V Real -1 Pwr Spec 1 Time 1 0 s 62.46948 ms 1V Peak 0 0 Hz 100 Hz dX:4.516602 ms dY:997.4356 mV
  • 47. The Y Scale RMS (Root Mean Square) Jack D. Peters X:55 Hz Y:706.8129 mV X:27.00806 ms Y:3.579427 mV dX:2.288818 ms dY:709.1976 mV 47 1V rms Magnitude 0 Pwr Spec 1 0 Hz 100 Hz 1V Real -1 Time 1 0 s 62.46948 ms The time wave has not changed. The RMS value is expressed from zero to 70.7% of the peak amplitude. The spectrum value uses the suffix “RMS” to denote this.
  • 48. The Y Scale Suffix Comparison Jack D. Peters Pwr Spec 1 Pwr Spec 1 Pwr Spec 1 48 2 V rms Magnitude 0 0 Hz 100 Hz 2 V Peak Magnitude 0 0 Hz 100 Hz 2 V Pk-Pk Magnitude 0 0 Hz 100 Hz 1 V Real -1 X:27.00806 ms Y:3.579427 mV Time 1 0 s 62.46948 ms 1 V Real -1 X:27.00806 ms Y:3.579427 mV Time 1 0 s 62.46948 ms 1 V Real -1 X:22.43042 ms Y:-993.8563 mV Time 1 0 s 62.46948 ms X:55 Hz Y:706.8129 mV X:55 Hz Y:999.5843 mV X:55 Hz Y:1.999169 V dX:2.288818 ms dY:709.1976 m dX:4.516602 ms dY:997.4356 m dX:9.094238 ms dY:1.994871 V RMS Peak Peak - Peak
  • 49. The Y Scale Changing Suffixes Many times it is necessary to change between suffixes. Jack D. Peters 49 Pk-Pk / 2 = Peak Peak x 0.707 = RMS RMS x 1.414 = Peak Peak x 2 = Pk-Pk
  • 50. The Y Scale Standard Suffixes Now that we have learned all about the three standard suffixes that might possibly confuse the “Y” scale values, what is the standard ? Vibration Institute: Displacement = mils Peak - Peak Velocity = in/s Peak or rms.. Acceleration = g’s Peak or rms.. Note: 1 mil = 0.001 inches Jack D. Peters 50
  • 51. The Y Scale Engineering Units (EU) Engineering units are used to give meaning to the amplitude of the measurement. Instead of the default “volts”, it is possible to incorporate a unit proportional to volts that will have greater meaning to the user. Examples: 100 mV / g 20 mV / Pa Jack D. Peters 1 V / in/s 200 mV / mil 50 mV / psi 10 mV / fpm 33 mV / % 10 mV / V 51
  • 52. The Y Scale EU’s the Hard Way Sometimes we forget to use EU’s, or just don’t understand how to set up the analyzer. There is no immediate need to panic if ???? You know what the EU is for the sensor you are using. Example: An accelerometer outputs 100 mV / g and there is a 10 mV peak in the frequency spectrum. What is the amplitude in g’s ? Answer = 10 mV / 100 mV = 0.1 g Jack D. Peters 52
  • 53. The Y Scale The Big Three EU’s Acceleration Velocity Displacement Jack D. Peters 53
  • 54. The Y Scale Converting the Big 3 In many cases we are confronted with Acceleration, Velocity, or Displacement, but are not happy with it. Maybe we have taken the measurement in acceleration, but the model calls for displacement. Maybe we have taken the data in displacement, but the manufacturer quoted the equipment specifications in velocity. How do we change between these EU’s ? Jack D. Peters 54
  • 55. The Y Scale Jack D. Peters 55 386.1 What ? 1g = 32.2 feet/second2 32.2 feet 12 inches second2 X foot 386.1 inches/second2 g
  • 56. The Y Scale Go With The Flow I ÷ 386.1 x 2(Pi)f Jack D. Peters 56 Acceleration (g’s) Velocity (inch/s) Displacement (inch) x 386.1 ÷ 2(Pi)f x 2(Pi)f ÷ 2(Pi)f
  • 57. The Y Scale Metric Go With The Flow I ÷ 9807 x 2(Pi)f Jack D. Peters 57 Acceleration (g’s) Velocity (mm/s) Displacement (mm) x 9807 ÷ 2(Pi)f x 2(Pi)f ÷ 2(Pi)f
  • 58. The Y Scale Go With The Flow II x 2 Jack D. Peters 58 Peak - Peak Peak RMS ÷ 2 x 1.414 x .707
  • 59. The Y Scale Doing the Math Units Jack D. Peters 0.5g x 386.1 inches second2 g 2π x 25 cycles 59 second 0.5g x 386.1 inches x 1 second g second2 2π x 25 cycles 0.5 x 386.1 inches 2π x 25 cycles second cycle 1.23 inches/second There is a 0.5 g vibration at 25 Hz. What is the velocity ?
  • 60. The Y Scale Acceleration - Velocity Example: Find the equivalent peak velocity for a 25 Hz Jack D. Peters 60 vibration at 7 mg RMS ? = (g x 386.1) / (2 Pi x F) = (0.007 x 386.1) / (6.28 x 25) = 0.017 inches / second RMS Answer = 0.017 x 1.414 = 0.024 inches / second Pk
  • 61. The Y Scale Velocity - Displacement Example: Find the equivalent pk-pk displacement for a Jack D. Peters 61 25 Hz vibration at 0.024 in/s Pk ? = Velocity / (2 Pi x F) = 0.024 / (6.28 x 25) = 0.000153 inches Pk Answer = 0.000153 x 2 = 0.000306 inches Pk-Pk
  • 62. The Y Scale Acceleration - Displacement Example: Find the equivalent Pk-Pk displacement for a Jack D. Peters 62 52 Hz vibration at 15 mg RMS ? = (g x 386.1) / (2 Pi x F)2 = (0.015 x 386.1) / (6.28 x 52)2 = 0.000054 inches RMS Answer = (0.000054 x 1.414) 2 = 0.000154 inches Pk-Pk
  • 63. Sensors Jack D. Peters 63 Sensors
  • 64. Sensors Jack D. Peters 64 Accelerometers • Integrated Circuit ¾Electronics inside ¾Industrial • Charge Mode ¾ Charge Amplifier ¾ Test & Measurement
  • 65. Sensors Accelerometer Advantages • Measures casing vibration • Measures absolute motion • Can integrate to Velocity output • Easy to mount • Large range of frequency response • Available in many configurations Jack D. Peters 65
  • 66. Sensors Accelerometer Disadvantages • Does not measure shaft vibration • Sensitive to mounting techniques and surface conditions • Difficult to perform calibration check • Double integration to displacement often causes low frequency noise • One accelerometer does not fit all applications Jack D. Peters 66
  • 67. Sensors Jack D. Peters Relative movement between post & mass creates shear in ceramic producing charge. 67 Mass & Charge Mass Ceramic/Quartz Post
  • 68. Sensors Accelerometer Parameters Performance Suited for Application Sensitivity (mV/g) Frequency Response of target (f span) Dynamic Range of target (g level) Jack D. Peters 68
  • 69. Sensors Mounting the Accelerometer 500 2000 6,500 10,000 15,000 15,000 Jack D. Peters 69 Hz.
  • 70. Sensors Realistic Mounting Jack D. Peters 70 Stud Bees Wax Adhesive Magnet Hand Held 100 1,000 10,000 Frequency, Hz In the real world, mounting might not be as good as the manufacturer had in the lab ! What happened to the high frequency ?
  • 71. Sensors Mounting Location Jack D. Peters Axial 71 Horizontal Vertical ¾Load Zone ¾Radial 9Vertical 9Horizontal ¾Axial
  • 72. Sensors Mounting Location Jack D. Peters 72 ¾Load Zone ¾Radial 9Vertical 9Horizontal ¾Axial
  • 73. Sensors Accelerometer Alarms Jack D. Peters Velocity Limit 73 Machine Condition rms peak Acceptance of new or repaired equipment < 0.08 < 0.16 Unrestricted operation (normal) < 0.12 < 0.24 Surveillance 0.12 - 0.28 0.24 - 0.7 Unsuitable for Operation > 0.28 > 0.7 Note #1: The rms velocity (in/sec) is the band power or band energy calculated in the frequency spectrum. Note #2: The peak velocity (in/sec) is the largest positive or negative peak measured in the time waveform.
  • 74. Sensors Proximity Probes Jack D. Peters 74
  • 75. Sensors Proximity Probe Theory Cable Jack D. Peters 75 Driver Target Probe The tip of the probe broadcasts a radio frequency signal into the surrounding area as a magnetic field. If a conductive target intercepts the magnetic field, eddy currents are generated on the surface of the target, and power is drained from the radio frequency signal. As the power varies with target movement in the radio frequency field, the output voltage of the driver also varies. A small dc voltage indicates that the target is close to the probe tip. A large dc voltage indicates that the target is far away from the probe tip. The variation of dc voltage is the dynamic signal indicating the vibration or displacement.
  • 76. Sensors Jack D. Peters 76 Output Values • Typical – 100 mv/mil – 200 mv/mil • Depends on probe, cable (length), and driver. • Target material varies output. Calibration Examples • Copper 380 mV/mil • Aluminum 370 mV/mil • Brass 330 mV/mil • Tungsten Carbide 290 mV/mil • Stainless Steel 250 mV/mil • Steel 4140, 4340 200 mV/mil Based on typical output sensitivity of 200 mV/mil.
  • 77. Sensors Proximity Probes - Advantages • Non-contact • Measure shaft dynamic motion • Measure shaft static position (gap) • Flat frequency response dc – 1KHz • Simple calibration • Suitable for harsh environments Jack D. Peters 77
  • 78. Sensors Proximity Probes - Disadvantages • Probe can move (vibrate) • Doesn’t work on all metals • Plated shafts may give false measurement • Measures nicks & tool marks in shaft • Must be replaced as a unit (probe, cable & driver) • Must have relief at sensing tip from surrounding metal Jack D. Peters 78
  • 79. Sensors Typical Mounting Jack D. Peters 79 vertical probe horizontal probe H V time Facing Driver to Driven (independent of rotation)
  • 80. Sensors Looking at Orbits Jack D. Peters 80 Vertical for Amplitude Horizontal for Time Base
  • 81. Sensors The Orbit Display Jack D. Peters 81 ils Mils Mils
  • 82. Sensors Jack D. Peters 82 Unbalance
  • 83. Sensors Unbalance with Orbit Jack D. Peters 83
  • 84. Sensors Jack D. Peters 84 Misalignment
  • 85. Sensors Misalignment with Orbit Jack D. Peters 85
  • 86. Sensors And the problem is ? Jack D. Peters 86
  • 87. Sensors Proximity Probe Alarms Jack D. Peters Allowable R/C 87 Machine Condition < 3,600 RPM < 10,000 RPM Normal 0.3 0.2 Surveillance 0.3 - 0.5 0.2 - 0.4 Planned Shutdown 0.5 0.4 Unsuitable for Operation 0.7 0.6 Note #1: R is the relative displacement of the shaft measured by either probe in mils peak-peak. Note #2: C is the diametrical clearance (difference between shaft OD and journal ID) measured in mils.
  • 88. Sensors Analyzer Input - Front End AC coupling will block the DC voltage. It creates an amplitude error below 1 Hz. DC coupling has no error below 1 Hz, but the analyzer must range on the total signal amplitude. Jack D. Peters 88 • Coupling - AC, DC • Antialias Filter - On, Off Prevents frequencies that are greater than span from wrapping around in the spectrum. Analyzer Input Capacitor Blocks DC AC Coupling Capacitor in DSA If the antialias filter is turned off, at what frequency will 175 Hz. appear using a 0 - 100 Hz span, and 800 lines ? 1024/800 = 1.28 100 x 1.28 = 128 Hz 175 Hz - 128 Hz = 47 Hz. 128 Hz - 47 Hz = 81 Hz
  • 89. Sensors Low End Frequency Response Jack D. Peters X:500 mHz Y:720.0918 m X:2.8125 Hz Y:984.7542 m X:5.34375 Hz Y:1.000001 89 0.01 V rms Magnitude 0.002 Input 1 0 Hz 25 Hz 0.01 V rms Magnitude 0 Output 2 0 Hz 25 Hz 2 Magnitude 0 Freq Resp 2:1 0 Hz 25 Hz 1.1 Magnitude 0.9 Coherence 2:1 0 Hz 25 Hz To the right is a typical problem with frequency response at the low end of the frequency spectrum. This low end roll off was a result of AC coupling on CH #2 of the analyzer. Values below 2.8 Hz are in error, and values less than 0.5 Hz should not be used.
  • 90. Data Collection Jack D. Peters 90 Data Collection
  • 91. Data Collection Tape Recorders “Insurance Policy” Jack D. Peters Multi-channel digital audio tape recorders. 91 For the Measurement that can’t get away !
  • 92. Data Collection Dynamic Signal Analyzers “Test & Measurement” Jack D. Peters Large PC driven solutions with multiple channels and windows based software. 92 Smaller portable units with 2 – 4 channel inputs and firmware operating systems.
  • 93. Data Collection Data Collectors “Rotating Equipment” Jack D. Peters 93
  • 94. Data Collection Data Collectors “Rotating Equipment” Jack D. Peters 94 • Route Based • Frequency Spectrum • Time Waveform • Orbits • Balancing • Alignment • Data Analysis • History • Trending • Download to PC • Alarms • “Smart” algorithms
  • 95. Beginning Vibration Jack D. Peters 95 Bibliography • Eisenmann, Robert Sr. & Eisenmann, Robert Jr., Machinery Malfunction Diagnosis and Correction, ISBN 0-13-240946-1 • Eshleman, Ronald L., Basic Machinery Vibrations, ISBN 0- 9669500-0-3 • LaRocque, Thomas, Vibration Analysis Design, Selection, Mounting, and Installation, Application Note, Connection Technology Center • Agilent Technologies, The Fundamentals of Signal Analysis, Application note 243 • Agilent Technologies, Effective Machinery Measurements using Dynamic Signal Analyzers, Application note 243-1
  • 96. Beginning Vibration Jack D. Peters 96 Thank You ! You can find technical papers on this and other subjects at www.ctconline.com in the “Technical Resources” section