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Vibration Monitoring and Analysis  155




                               4
                                                              SENSITIVE AXIS
                                                        3

                              2





                                                   1
                              Figure 7–23 Schematic diagram of
                              accelerometer. (1) Base, (2) Piezoelectric
                              crystals, (3) Mass, (4) Case.



            The effective range of general-purpose accelerometers is from about 1Hz to 10,000
            Hz. Ultrasonic accelerometers are available for frequencies up to 1MHz. In general,
            vibration data above 1,000Hz, or 60,000cpm, should be taken and analyzed in accel-
            eration or g’s.

            A benefit of the use of accelerometers is that they do not require a calibration program
            to ensure accuracy; however, they are susceptible to thermal damage. If sufficient heat
            radiates into the piezoelectric crystal, it can be damaged or destroyed, but thermal
            damage is rare because data acquisition time is relatively short (less than 30 seconds)
            using temporary mounting techniques.


            Cables
            Most portable vibration data collectors use a coiled cable to connect to the transducer
            (see Figure 7–24).  The cable, much like a telephone cord, provides a relatively
            compact length when relaxed but will extend to reach distant measurement points. For
            general use, this type of cable is acceptable, but it cannot be used for all applications.

            The coiled cable is not acceptable for low-speed (less than 300rpm) applications or
            when there is a strong electromagnetic field. Because of its natural tendency to return
            to its relaxed length, the coiled cable generates a low-level frequency that corresponds
            to the oscillation rate of the cable. In low-speed applications, this oscillation frequency
            can mask real vibration that is generated by the machine. A strong electromagnetic
            field, such as that generated by large mill motors, accelerates cable oscillation. In these
            instances, the vibration generated by the cable will mask real machine vibration.

            In these and other applications where the coiled cable distorts or interferes with the
            accuracy of acquired data, a shielded coaxial cable should be used. Although these
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