An accelerometer is a device that measures the vibration, or acceleration of motion of a structure.
The force caused by vibration or a change in motion (acceleration) causes the mass to "squeeze" the piezoelectric
material which produces an electrical charge that is proportional to the force exerted upon it. Since the charge is
proportional to the force, and the mass is a constant, then the charge is also proportional to the acceleration.
There are two types of
piezoelectric accelerometers (vibration sensors). The first type is a "high impedance" charge output accelerometer. In this type
of accelerometer the piezoelectric crystal produces an electrical charge which is connected directly to the measurement instruments.
The charge output requires special accommodations and instrumentation most commonly found in research facilities. This type of
accelerometer is also used in high temperature applications (>120C) where low impedance models can not be used.
The second type of accelerometer is a low impedance output accelerometer. A low impedance accelerometer has a charge accelerometer
as its front end but has a tiny built-in micro-circuit and FET transistor that converts that charge into a low impedance voltage
that can easily interface with standard instrumentation. This type of accelerometer is commonly used in industry. An accelerometer
power supply like the ACC-PS1, provides the proper power to the microcircuit 18 to 24 V @ 2 mA constant current and removes the DC
bias level, they typically produces a zero based output signal up to +/- 5V depending upon the mV/g rating of the accelerometer.
All OMEGA(R) accelerometers are this low impedance type.
Dynamic Range is the +/- maximum amplitude that the accelerometer can measure before distorting or clipping
the output signal. Typically specified in g's.
Frequency Response is determined by the mass, the piezoelectric properties of the crystal, and the resonance
frequency of the case. It is the frequency range where the output of the accelerometer is within a specified deviation,
typically +/- 5%.
g 1g is the acceleration due to the earth's gravity which is 32.2 ft/sec2, 386 in/sec2 or 9.8 m/sec2.
Grounding - There are two types of signal grounding in accelerometers. Case Grounded accelerometers have the
low side of the signal connected to their case. As the case is part of the signal path and may be attached to a conductive material,
care must be used when using this type of accelerometer to avoid noise from the ground plain. Ground Isolated accelerometers
have the electrical components isolated from the case and are much less susceptible to ground induced noise.
High Frequency Limit is the frequency where the output exceeds the stated output deviation. It is typically
governed by the mechanical resonance of the accelerometer.
Low Frequency Cut-off is the frequency where the output starts to fall off below the stated accuracy.
The output does not "cut-off " but the sensitivity decreases rapidly with lower frequencies.
Noise - Electronic noise is generated by the amplifying circuit. Noise can be specified either broad band
(specified over the a frequency spectrum) or spectral - designated at specific frequencies. Noise levels are specified
in g's, i.e. 0.0025 g 2-25,000 Hz. Noise typically decreases as frequency increases so noise at low frequencies is more
of a problem than at high frequencies.
Resonance Frequency is the frequency at which the sensor resonates or rings. Frequency measurements want
to be well below the resonance frequency of the accelerometer.
Sensitivity is the output voltage produced by a certain force measured in g's. Accelerometers typically
fall into two categories - producing either 10 mV/g or 100 mV/g. The frequency of the AC output voltage will match the
frequency of the vibrations. The output level will be proportional to the amplitude of the vibrations. Low output accelerometers
are used to measure high vibrational levels while high output accelerometers are used to measure low level vibrations.
Temperature Sensitivity is the voltage output per degree of measured temperature. The sensors are temperature
compensated to keep the change in output to within the specified limits for a change in temperature.
Temperature Range is limited by the electronic micro circuit that converts the charge to a low impedance output.
Typically the range is -50 to 120C.
When selecting an accelerometer for your application many parameters must be considered.
- What is the vibration amplitude to be monitored?
- What is the frequency range to be monitored?
- What is the temperature range of the installation?
- What is the size and shape of the sample to be monitored?
- Are there electromagnetic fields?
- Is there a high level of electrical noise in the area?
- Is the surface where the accelerometer is to be mounted grounded?
- Is the environment corrosive?
- Does the area require Intrinsically safe or explosion proof instruments?
- Is the area a wet or a wash down area?
The mass of the accelerometers should be significantly smaller than the mass of the system to be monitored.
The accelerometer dynamic range should be broader than the expected vibration amplitude range of the sample.
The frequency range of the accelerometer should fit the expected frequency range.
The Sensitivity of the accelerometer should produce an electrical output compatible with existing instrumentation.
Use a low sensitivity accelerometer to measure high amplitude vibrations and conversely use a high sensitivity accelerometer
to measure low amplitude vibrations.
The sensor must be mounted directly to the machine surface to correctly measure the vibrations. This can be accomplished by several types of mounts:
Magnet Mounts are generally temporary mountings.
- Flat Magnet Mount
- 2-pole Magnet Mount
- Adhesives (Epoxy/Cyanoacrylate)
- Mounting Stud
- Isolating Stud
Magnetic mounts are used to mount accelerometers to ferromagnetic materials commonly found in machine tools, structures and motors.
They allow the sensor to be easily relocated from site to site for multiple location readings. Two-pole magnetic mounts are used
to mount an accelerometer to a curved ferromagnetic surface.
Adhesives, and threaded studs are considered permanent mountings.
Adhesives such as epoxy or cyanoacrylate have proven to provide satisfactory bonding for most applications. Keep the film as thin
as possible to avoid any unwanted dampening of the vibrations due to the flexibility of the film. To remove an adhesive mounted
accelerometer, use a wrench on the case's wrench flats and twist to break the adhesive bond. DO NOT USE A HAMMER. Striking the
accelerometer will damage it.
Mounting studs are the preferred mounting technique.
They require the structure to be drilled and tapped but provide solid reliable mountings. Be sure to follow the specified torque
settings to avoid damaging the sensor or stripping the threads.