Page 265 - Compression Machinery for Oil and Gas
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250 SECTION    II Types of Equipment


            well above potential excitations. In summary, lateral natural frequencies (or
            critical speeds) of a crankshaft that involve mode shapes with amplitudes within
            a reciprocating compressor are not a typical concern.
               Lateral natural frequencies for reciprocating compressor crankshafts that
            involve an overhung mass, such a coupling hub or flywheel, can become impor-
            tant. Specifically, this is referring to a lateral natural frequency that involves a
            mode shape with large amplitude at the overhung mass. These particular modes
            are controlled by the shaft stiffness of the overhung portion, and the mass of
            the overhung component. These modes are potentially excited by imbalance
            at 1 , misalignment at 1  and 2 , and also by the rod loads acting from
            the connecting rod at the two throws adjacent to the drive end, primarily at
            1  and 2 . With relatively high amplification and little damping (mostly from
            the crankshaft-bearing oil films), operating on or very near an overhung lateral
            natural frequency (primarily at 1  and 2 ) can cause significant lateral vibra-
            tion and potentially failed parts. In most cases, a simple hand calculation con-
            sidering the crankshaft held at the two drive-end bearings, shaft, and overhung
            mass may be adequate to determine that the lateral natural frequency is separate
            from 1  and 2  running speed. Such a check (or a complete lateral analysis)
            should be performed for these types of designs during the design phase to deter-
            mine the potential for any overhung modes to be excited in the running
            speed range.
               The lateral rotordynamics of a reciprocating compressor also become
            important when the crankshaft is rigidly connected to the driving equipment.
            When a rigid coupling is used, the lateral rotordynamic response of the crank-
            shaft is coupled to the driver shaft. Therefore, the lateral rotordynamic model
            and analysis should (at a minimum) include both the driver and reciprocating
            compressor crankshaft through the first two throws and crank bearings at the
            drive end. Traditional calculation of natural frequencies, mode shapes, and
            imbalance response should be considered for the coupled driver and compressor
            crankshaft model. It is noted that most oil and gas reciprocating compressors
            today are driven through flexible couplings, where the lateral response of the
            driver and compressor is de-coupled, or independent of one another.
               Lateral and torsional coupling, from a vibration standpoint, only occurs
            when a kinematic constraint relates lateral motion to torsional motion. This
            can be seen in a geared system or gearbox where lateral motion of the bull
            or pinion can influence or become affected by the torsional motion through
            the connection at the gear mesh. Typically, lateral-torsional coupling is seen
            when a torsional mode of a machinery train is excited, resulting in measureable
            lateral vibration of the pinion. There is the possibility, although considered very
            rare, of a coupled lateral-torsional mode in a geared system. Further information
            on lateral-torsional coupling in rotordynamics is discussed in Childs [18].
               In addition, lateral and torsional vibration coupling has been noted in recip-
            rocating compressors. The literature shows that lateral and torsional vibration
            coupling can be problematic in reciprocating compressors. Stephens et al.
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