Page 233 - Compression Machinery for Oil and Gas
P. 233

222 SECTION    II Types of Equipment


            user is cautioned about the use of excessively large bottles. These have two
            technical problems, potentially high shaking forces due to the gas pulsation act-
            ing on the baffles and because they are large and heavy the difficulty in support-
            ing safely above the compressor cylinders. Piping and bottles are usually
            designed to have a mechanically resonant frequency above 2.4  the running
            speed. Especially on high-speed machines the 2.4  limit can be difficult to
            achieve and it is often necessary to consider secondary bottles as a part of
            the pulsation control such as the separator or a secondary pulsation bottle.


            Cylinder Orifice Plates
            Gas enters (and leaves) a cylinder in two discrete slugs per revolution for a
            double-acting cylinder. Depending on the velocity of the gas flowing through
            passageway the velocity head results in a pressure pulsation. Applying an FFT
            analysis to this gas flow gives the harmonic content of the flow. Considering the
            gas passageway from the compressor valve to the pulsation bottle volume this
            acts as a closed-open pipe and the column of gas has a natural frequency of a
            quarter wave. So for 1200rpm natural gas compressor with a sonic velocity of
            519M/s and a distance from the valve to the bottle volume of 1.2m, the quarter-
            wave resonant frequency would be 519/(1.2 4)¼108Hz. The operating speed
            of 1200rpm is 20Hz so the quarter-wave resonant frequency is 108/20¼5.4
            running speed. Looking at Fig. 5.40 a double-acting cylinder will have signif-
            icant pulsation energy at 4  and 6  running speed. Considering that the sonic
            velocity for a given gas composition will vary primarily with gas temperature
            (higher temperatures have higher sonic velocity), then the pulsation analyst will
            often consider that an orifice plate in the cylinder nozzle is necessary to dampen
            the quarter-wave pulsation resonance. The orifice plate creates a pressure drop
            that is quite effective at damping the quarter-wave resonance (usually at 4  or
            6  machine speed), but this does nothing to reduce the 2  pulsation, in fact it is
            made worse. In addition, the pressure drop will cause an increase in overtone
            and undertone losses in the PV card causing an increase in compression HP
            and rod load. API-618 gives an allowable pulsation bottle pressure drop of
            ΔP ¼1.67((R  1)/R)%. This gives a value of 1% when the pressure ratio is
            2.5. Many packagers use a value of 1% pressure drop for all applications even
            though this is higher than the allowance for compression ratios below 2.5. In
            addition, the limit is calculated on the basis of Steady flow. As can be implied
            from Fig. 5.40 the steady flow is only a small fraction of the peak flow rate for
            the nozzle orifice plate, usually around 2  on the inlet and 3  on the discharge
            is typical. As pressure drop through an orifice is a function of flow velocity
            squared the effective instantaneous pressure drop through the orifice plate is
            typically 4–10  the value calculated based on steady flow through the orifice
            plate. This can have a significant effect on compression horsepower and rod
            load possibly causing overloading. As previously noted resonant pulsations
            do need to be controlled and API-618 gives allowable pulsation values at the
   228   229   230   231   232   233   234   235   236   237   238