Sensing Instrument
Dynamic vibration sensors generate an electrical charge proportional to the applied mechanical acceleration. This principle enables the piezoelectric accelerometer to measure rapid changes in motion and shock across a wide range of industrial and scientific testing environments. The instrument operates without moving parts, which gives it high durability and a long operating life.
Mechanical Assembly
The internal structure consists of a seismic mass resting on a piezoelectric crystal held under a pre-loaded force. When acceleration is applied to the sensor, the seismic mass exerts a dynamic force on the crystal, which displaces charge on the crystal faces. This charge is either measured directly by an external charge amplifier or converted to a voltage by built-in electronics.
Shear designs are widely used because they isolate the sensing element from thermal transients and base strain, which would otherwise introduce measurement errors.
Frequency Response
Sensor performance remains flat across a wide frequency band but rises sharply as it approaches the natural resonance of the mechanical structure. The usable frequency range is usually limited to one third of this resonant frequency to avoid excessive gain errors. Factors such as cable motion and strain on the mounting surface can introduce low-frequency noise that must be filtered out.
Mounting Configuration
Secure attachment to the test structure ensures that the high-frequency vibrations are transmitted without attenuation to the sensor. Stud mounting provides the widest frequency range, whereas magnetic bases or adhesive mountings reduce the usable upper limit. Calibration of the sensor should always occur using the same mounting method as the actual test to avoid measurement discrepancies.