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Page 1sensors.ppt
VibrationMeasurement
Sensors
VibrationMeasurement
Sensors
Page 2sensors.ppt
Who is Wilcoxon Research?
➤ Started in 1960 by engineers from UnitedStates Navy Research Laboratory
➤ Developed Accelerometers, ImpedanceHeads, and Reaction Shakers
Primary sales are to industrial customers➤ Pulp & Paper
➤ Machine Tool
➤ Power Generation
➤ Petrochemical
➤ Food Processing
➤ Steel & Aluminum
Page 3sensors.ppt
Who is Wilcoxon Research
➤ Early Markets were Naval Engineering andTest for US, French, and British Navies
➤ Entered Condition Monitoring in the early1980’s with Palomar, Scientific Atlanta,and CSI
Page 4sensors.ppt
Wilcoxon Research Today
➤ Worlds largest manufacturer of industrialaccelerometers
➤ Located in Metropolitan Washington DCalong the I 270 Technology Corridor
➤ Approximately 120 employees
Page 5sensors.ppt
Basic Vibration Sensors
ANoncontactingDisplacementTransducer
cce lerometer
Elec trodynamicVelocity Trans ducer
Page 6sensors.ppt
Eddy Current Probe Fabrication
Page 7sensors.ppt
Eddy Current Probe - How It Works
➤ Three matched components - Driver, probe and extension cable
➤ Voltage applied to the Driver causes an RF signal to be generated
➤ Signal is transmitted to the probe by the extension cable
➤ Coil inside probe tip serves as an antenna and radiates high frequencyenergy into free space
➤ Any conductive material within the field absorbs energy and causesoutput of probe to decrease proportional to gap distance
Page 8sensors.ppt
Eddy Current Probe
Page 9sensors.ppt
Page 10sensors.ppt
Eddy Current Specifications
80 mils beginning at approx. 10 mils
200mV/mil over a 80 mil range
200 mV/mil straight line +/- 0.8 mils
0 to 600,000 CPM (Theoretical)
Driver-60 F to +212 F
Probe and Cable-30 F to +350 F
to 95% noncondensing
Calibrated Range
Scale Factor
Linearity
Frequency Response
Temperature Range
Relative Humidity
Page 11sensors.ppt
➤ Housing vibrates while the spring-suspended coil remains stationary
➤ Amplitude of the output voltage is proportional to the velocity of thevibration
Fabrication of Electrodynamic Velocity Sensor
Page 12sensors.ppt
Types of Accelerometers
➤ Piezoelectric– Charge mode
– Internally amplified
➤ Strain Gauge
➤ Piezoresistive
➤ Variable Capacitance
➤ Others
Page 13sensors.ppt
Piezoelectric Accelerometers
➤ Measures Acceleration
➤ Velocity or DisplacementOutput Available
➤ Very Sensitive
➤ Contacting
➤ Measures Absolute CasingMotion
➤ Measures Very LowFrequency
➤ Measures Very HighFrequency
Pie zo c e ramic s
S e is m ic Mas s
Co nne c to r
2208a - R1
Am plifie r
Mo untingBas e
P ie zo c e ramic s
2339a
S e is m ic Mas s
Co nne c to r
Am plifie r
Mo untingB as e
2339b
Am plifie r
Co nne c to r
Mo unting Bas e
S e is micMas s
Pie zo c e ramic
Mo untingS c re w
Page 14sensors.ppt
Piezoelectric Accelerometer - How It Works
➤ Piezoelectric material (sensing element) isplaced under load using a mass
➤ As ‘stack’ vibrates, crystal is squeezed orreleased
➤ Charge output is proportional to the force(and acceleration)
➤ Electronics convert charge output intovoltage output
Pie zo c e ramic s
2339a
S e is mic Mas s
Co nne c to r
Am plifie r
Mo untingBas e
Page 15sensors.ppt
Operational Range
Page 16sensors.ppt
Vibration vs. Frequency
➤ Very Little VibrationAmplitude in terms ofAcceleration is Producedat Low Frequencies
➤ Much Larger Amplitudesare produced in terms ofDisplacement
1,000
100
10
1.0
0.1
.01
.001
.0001.1.6
Hzcpm
160
10600
1006,000
1,00060,000
EU(mils pp)
(ips)(g)
FREQUENCY
Velocity (ips)
Acceleration (g)
Displacement (mils pp)
1607-R1
Page 17sensors.ppt
Eddy Probe
Advantages
➤ Low frequency response(to 0 Hz)
➤ Can measure relativedisplacement
➤ Useful as a key phasorfor dynamic balancing &analysis
➤ Reliable if propertyinstalled and maintained
Disadvantages
➤ Difficult to install
➤ Practical limits of highfrequency displacementmeasurement
➤ Calibration dependenton shaft material
➤ Shaft runout / glitchproduces false signals
Page 18sensors.ppt
Electrodynamic Velocity Transducer
Advantages
➤ No external powering
➤ Powerful signal Output
➤ Easy to use (not assensitive to mountingproblems as alternative)
➤ Ability to operate atelevated temperatures
Disadvantages
➤ Not useful for verylow frequency
➤ Not useful for veryhigh frequency
➤ Moving parts wear
➤ Mounting orientationmay be important
➤ Size
➤ Accuracy (resolution /noise as compared toalternatives)
Page 19sensors.ppt
Advantages
➤ Very wide frequency
➤ Wide amplitude range
➤ Broad temperaturerange
➤ Velocity ordisplacement outputavailable
➤ Rugged, industrialdesign
Disadvantages
➤ Not responsive to 0 Hz
➤ Internal Amplifierlimits temperature
Internally Amplified Accelerometer
Page 20sensors.ppt
Low FrequencyAccelerometer Considerations
➤ High Sensitivity
➤ Low Noise
➤ Low Pass Filter
➤ Environmental Protection➤ Overload Protected
➤ Resists Thermal transients
➤ Low Strain Sensitivity
➤ Limited Amplitude Range
Pie zo c e ramic s
S e is mic Mas s
Co nne c to r
2208a - R1
Amplifie r
Mo untingBas e
Page 21sensors.ppt
Sensitivity Selection
793, 786A797, 736
799M
732A, 732AT
Page 22sensors.ppt
Electronic Sensor Noise
➤ Sets the AbsoluteMeasurement Floor
➤ Increases asFrequency Decreases
➤ Dependent on ChargeSensitivity
PZT Piezoceramics are very sensitive and must beused for Low Frequency Accelerometers
Page 23sensors.ppt
500 mV/g
100 mV/g
Page 24sensors.ppt
Electronic Sensor Noise
➤ Electronic Sensor Noise can be Improved by usingmore Lines of Resolution
➤ The Cost is greater Measurement Time
➤ Data Acquisition Time = Lines/Fmax
2348a - R1
400 800 1600 3200 3200Lines of Res olution
Electronic Spectral Noise ofa Low Frequency Sensor(1 g/ Hz)
Measurement TimePer Data Set
Measurement Time forFour (4) Averages WithoutOverlapping
Measurement Time forEight (8) Averages WithoutOverlapping
µ ⌦0.16 g
40 sec
160 sec
320 sec
µ 0.11 g
80 sec
320 sec
640 sec
µ 0.79 g
160 sec
640 sec
1,280 sec
µ 0.056 g
320 sec
1,280 sec
2,560 sec
µ
(5.3 min)
(21.3 min)
(42.7 min)
Page 25sensors.ppt
Summary of Concepts
Reminder - very little motion in terms of acceleration isproduced at low frequencies
Page 26sensors.ppt
Strain Gage Accelerometers
➤ Metal (wire or foil) strain gages on a beam or diaphragmstructure
➤ Measure strain caused by inertial forces on mass
➤ Low sensitivity and/or low natural frequency
➤ Rarely used; being replaced by PR and VC
Page 27sensors.ppt
Piezoresistive Accelerometers
Page 28sensors.ppt
Variable Capacitance
Page 29sensors.ppt
Servo Force Balance