The subject matter disclosed herein relates to gas compressors. More particularly, the subject matter disclosed herein relates to reciprocating gas compressors having an inertia conservation feature.
Gas compressors may be broadly grouped as either dynamic or positive displacement gas compressors. Positive displacement type compressors increase gas pressure by reducing volume occupied by the gas. Positive displacement gas compressors operate by confining a fixed amount of gas in a compression chamber, mechanically reducing the volume occupied by the gas thereby compressing the gas, and passing the compressed the gas into a distribution network. The gas pressure increase corresponds to the volume reduction of the space occupied by the amount of gas. As used herein, the term gas includes substances in a gaseous state, substances in a liquid state, and mixtures comprised of substances having both a liquid and a gaseous state.
Positive displacement compressors mechanically reduce the volume occupied gas using either a reciprocating piston or rotating component. Reciprocating compressors successively compress volumes of gas by repetitively driving a compression piston into a compression chamber in a first direction, withdrawing the piston from the compression chamber in a second direction, and allowing a volume of gas to be compressed to occupy the chamber. Each time the piston moves into the compression chamber it sweeps a portion of the chamber, thereby reducing the volume of chamber occupied by the gas, and raising the pressure therein. The compressed gas then exits the chamber, the piston withdraws from the chamber, and a second charge of gas enters the chamber for a subsequent reciprocation of the piston.
Reciprocating compressors may be either single-acting or double-acting. Single-acting compressors, as described above, effect compression only when driving the piston in the first direction. Double-acting compressors include a compression chambers associated with both the front face and rear face of the compression piston, thereby effecting compression with piston movement in both the first and second direction.
Reciprocating compressors may also be either single-stage or multi-stage. In single stage compressors, the compressor compresses the volume of gas in a single mechanical operation—such as in the first piston movement described above. In multi-stage compressors, the compressor compresses the volume of gas in more than one mechanical operation—such as by compressing gas with the front face of the piston in the first movement described above, moving the compressed gas to the chamber associated with the rear face of the piston, and further compressing the gas with the rear face of the piston in the second movement described above. Still other multi-stage compressors include a plurality of compression pistons arranged to compress gas with a plurality of compression operations.
Reciprocating compressors that use pistons for compressing have several disadvantages. For example, the inertial forces associated with the reciprocating components are high in piston-equipped compressors. During successive reciprocations, the compressor drive accelerates the piston in one direction, stops it, and then accelerates it in the opposite direction. The more massive the piston assembly, the greater the force the drive need supply to accelerate and decelerate the assembly. And since the kinetic energy of the assembly is typically dissipated (and not conserved) at the end of the stroke, the compressor is inherently less efficient. Such energy loss can be particularly severe in compressors having comparatively short strokes, where the inertial loads associated with accelerating the piston assembly is the peak load imposed upon the drive assembly. As a result, the majority of the force produced by the compressor drive goes not into compressing gas, but rather into successively accelerating the piston assembly.
In high-pressure natural gas applications, compressors are typically rotary driven. Rotary drives, in turn, have a mechanical connection between the rotating drive and the piston that converts drive shaft rotation into piston linear translation—typically through use of a connecting rod. Connecting rods constrain compression operation such that the portion of the compression chamber swept by the piston is constant. Hence, for purposes of varying the volume of gas compressed without altering drive shaft speed, piston-equipped compressors include a turndown. The turndown alters compression chamber volume by the volume of the chamber within which the piston reciprocates—thereby altering the compression the gas within the chamber undergoes during each stroke. Turndowns present their own disadvantages, such as being time consuming to adjust and even requiring that the compressor be taken off line so that an operator may physically operate a crank to alter the compression chamber volume.
One alternative that provides an adjustable capacity compressor is a linear motor driven compressor. Such a compressor was proposed in the Advanced Reciprocating Compression Technology Final Report, SwRI Project No. 18.11052 prepared under DOE Award No. DE-FC26-04NT42269, Deffenbaugh et al. (the “ARCT Report”), dated December 2005. However, as concluded in the ARCT Report, while a linear motor could be used to drive a reciprocating compressor, current linear motor technology limits such compressors to smaller diameter cylinders, operating at slower speeds and with relatively long stroke lengths—therefore having lower capacity and being unsuitable for conventional natural gas distribution systems. These limitations are due in part to the limited amount of force achievable through existing linear motor technology and in part due to the above-described rod load inertial load requirements.
Accordingly, there is a need for a reciprocating compressor where drive force requirement is driven by the force required to compress the gas in the compression chamber rather than the inertial force required to accelerate the compression piston. There is also a need a reciprocating compressor having a large bore diameter with an associated drive force requirement within the capabilities of existing linear motor technology. Finally, there is a need for a reciprocating compressor having a short stroke length with an associated drive force requirement within the capabilities of existing linear motor technology.
Various other features, objects, and advantages of the invention will be made apparent to those skilled in the art from the accompanying drawings and detailed description thereof.
According to an embodiment of the present invention, a reciprocating compressor is provided. The reciprocating compressor comprises a piston reciprocatably disposed in compression cylinder; a translatable assembly connected to the piston; an electromagnetic drive having a fixed stator and a core coupled to the translatable assembly, wherein the drive is configured to reciprocatably drive the translatable assembly within the compression chamber; and an accumulator coupled to the translatable assembly, wherein the accumulator is configured to store kinetic energy resident in the motion of a movement of the translatable assembly in a first direction, and wherein the accumulator is configured to impart kinetic energy resident in the motion of a movement of the translatable assembly in a second direction.
According to an embodiment of the present invention, a method of use for reciprocating comprising a translatable assembly, an accumulator coupled to the translatable assembly, and an electromagnetic drive coupled to the translatable assembly, is provided. The method comprises accelerating the translatable assembly in a first movement direction by applying a force to the translatable assembly with the electromagnetic drive; decelerating the translatable assembly in the first movement direction by storing kinetic energy resident in the translatable assembly in the accumulator; and accelerating the translatable assembly in a second movement direction by generating force from the accumulator stored energy.
These and other features, aspects, and advantages of the present invention will become better understood when the following detailed description is read with reference to the accompanying drawings in which like characters represent like parts throughout the drawings, wherein:
The following detailed description makes reference to the accompanying drawings that form a part the application and which illustrate certain embodiments of the invention. These embodiments are described in sufficient detail to enable those skilled in the art to practice the embodiments, and it is to be understood that other embodiments may be utilized and that logical, mechanical, electrical and other changes may be made without departing from the scope of the invention. The following detailed description is, therefore, not to be taken as limiting the scope of the invention.
As will be the convention throughout the drawings herein, elements/assemblies having 45 degree hash marks are fixed with respect to elements/assemblies not having such identification. Accordingly, as shown in
As used herein, the term “bottom dead center” refers to a positional arrangement wherein the piston is positioned within the compression assembly on an end adjacent the drive assembly. As used herein, the term “top dead center” refers to a positional arrangement wherein the piston is positioned within the compression assembly on an end opposite the drive assembly. As used herein, the term “reciprocation” refers to successive, alternating movements of the translatable assembly that drive a piston towards the head-end and then toward the crank-end along a translation axis.
During translation of piston 12 from bottom dead center to top dead center, first piston face 16 applies force to a gas occupying chamber 20, thereby pressurizing the gas. At the same time, the translation of piston 12 also increases the volume of chamber 22. As shown in
FDrive=(MTranslatable Assembly)*α+FPiston Face (Equation 1)
where α is an acceleration of the translatable assembly 40. The term “(MTranslatable Assembly)*α” represents the inertial force that must be overcome to accelerate the reciprocating mass of the translatable assembly 40 when undergoing acceleration.
As is clear from
Each time the compressor changes translation direction, the drive must (a) decelerate the moving translatable assembly to a stop, thereby overcoming the inertial force resident in the moving translatable assembly, and (b) accelerate the stopped translatable assembly in the opposite direction, thereby imparting an inertial force into the translatable assembly. As such, it would be advantageous to incorporate a mechanism into the compressor 10 that conserves the inertial force resident in a first movement for use in a second movement.
In like manner, resilient members are configured such that, when the translatable assembly 140 is decelerating, the resilient members (164,170) apply a force directed in substantially opposite same direction as that of the motion of translatable assembly 140, thereby decelerating the speed of assembly 140 and reducing the force the drive assembly 132 would otherwise need apply to the assembly 140 in order to decelerate the assembly 140. The resilient members apply such force by being deformed from their respective relaxed states (not shown). As such, the accumulator 174 has the technical effect of ‘banking’ the inertia resident in the moving translatable assembly 140 during a first assembly movement by decelerating the assembly, and returning that inertia to the assembly 140 by accelerating the assembly in a second assembly movement.
During an interval when the drive 132 accelerates the translatable assembly 140 along axis 142, the accumulator 174 more particularly applies force in concert with the drive 132, thereby assisting the drive 132 in both (a) overcoming the gas force applied on the piston first face 116, and (b) increasing the inertial force resident in the translatable assembly 140. During such an acceleration interval, the force produced by drive 132 must satisfies the equation:
FDrive=(MTranslatable Assembly)*α+FPiston Face−FAccumulator (Equation 2)
During an interval when the drive 132 decelerates the translatable assembly along axis 142, the accumulator 174 more particularly applies force in concert with the drive 132, thereby assisting the drive 132 in removing inertial force resident in the translatable assembly 140, thereby decelerating the assembly 140 in the head-end direction. During such a deceleration interval, the force produced by drive 132 satisfies the equation:
FDrive=(MTranslatable Assembly)*(−α)+FPiston Face+FAccumulator (Equation 3)
As shown in Equation 2 and Equation 3, the accumulator 174 has the technical effect of reducing the force that the drive 132 needs produce in order to accelerate the translatable assembly 140. Expanding the “FAccumulator” term of Equation 2 and Equation 3 for an accumulator comprising a single spring, the force produced by the drive satisfies the equation:
FDrive=(MTranslatable Assembly)*(−α)+FPiston Face+(k*X) (Equation 4)
Where k is a spring constant, and X is the displacement of the spring end connected to the translatable member from its equilibrium position. The springs (164,170) shown in
For example, in an embodiment a capacitor (not shown) having a first conductor (not shown) fixed and a second conductor (not shown) attached to the translatable assembly are separated by a dielectric (e.g. air); in this way, the capacitor has moving plates (to be precise one plate moves with respect to the other plate) and thus has a variable capacitance. According to a variant of this embodiment, the dielectric-occupied distance between the two conductive plates varies with translation of the translatable assembly. The first and second conductors may be charged once-for-all and left isolated during operation of the compressor, or may be charged differently and left isolated during distinct operating periods of the compressors, or may be permanently connected to a constant voltage generator during operation of the compressor, or may be permanently connected to a variable voltage generator during operation of the compressor (typically the voltage of the generator is varied slowly with respect to the oscillation period of the translatable assembly). Such an accumulator stores a changeable electric charge corresponding to movement of the translatable assembly, the capacitor thereby banking the inertial energy of assembly and being configured to supply the charge to power a subsequent translation of the translatable assembly. The use of one or more capacitor may be combined with the use of one or more springs that may have a constant or a variable spring constant.
More particularly, in embodiments having resilient members comprising a spring, the spring may be configured such that the drive actuates the translatable assembly so as to excite the translatable assembly at a resonance frequency of the spring. The spring, in turn, may be designed to make coincident the resonance period with a desired actuation time. Alternatively, the spring may be designed to make coincident a harmonic of the resonance period with the desired actuation time.
It is worth noting that the springs of the embodiments of the present invention may have a spring constant that is constant with respect to time and space which corresponds to the most common case for helical springs; alternatively, the spring constant may vary in time and/or in position, in particular along its length (i.e. it depends on the degree of compression of the spring).
More in general, it may be said that the accumulator of the embodiment of
A further advantageous effect of compressor 100 is that existing linear motor technology can be adapted to construct machinery having commercially useful capacity.
For example, in a first non-limiting embodiment, compressor 100 comprises an electromagnetic drive assembly 132 having a synchronous linear motor. In this embodiment, the stator 134 comprises a plurality of conductive coils and the core 136 comprises a permanent magnet. The plurality of conductive coils is arranged coaxially and parallel with respect to the axis 142. Operatively, a coil within the plurality of coils can be individually energized, thereby generating a magnetic motive force pushes against core 136, thereby reciprocatably driving translatable assembly 140 along the axis 142.
Alternatively, in a second non-limiting embodiment, compressor 100 comprises an electromagnetic drive assembly 132 having an asynchronous linear induction motor. In this embodiment, the stator 134 comprises a plurality of conductive coils and the core 136 comprising a reaction plate constructed of a conductive material, such as copper or aluminum. The plurality of conductive coils is arranged substantially coaxially or parallel with respect to the axis 142. The plurality of coils connects to a three-phase AC power supply (not shown) and is configured such that, upon being energized, an electric current is induced in the reaction plate. The induced current produces a magnetic field that interacts with the coils, thereby producing a motive force that pushes the core 136, thereby reciprocatably driving translatable assembly 140 along the axis 142.
In the various magnetically-geared drive embodiments depicted above, the cores of the compressors are implemented with permanent magnet cores. However, it is also contemplated that the integrated magnetic gearing may also be accomplished through the use of cores having wound field, squirrel cage, or switched reluctance poles. In other words, the core's magnetic field may be implemented through DC powered electromagnets, in lieu of permanent magnets. Furthermore, with regard to the stationary pole-pieces that serve as flux modulation devices, the shape of such pieces may be embodied by other insert shapes in addition to square inserts, such as oval or trapezoidal shapes for example. The configurations illustrated in the above embodiments are shown as including three-phase windings for purposes of example. It should also be understood that a different number of phases might be used as well.
More particularly, the embodiments shown in
As discussed in the preceding sections, the shape of the core of the drive described herein may be, for example, an “E” shape or a “U” shape. To generate a high electromagnetic force in the core in a very short span of time, the core of the solenoid as well as the plate are typically manufactured out of metal sheets to avoid eddy current effects as eddy current growing in the core may reduce the magnetic flux produced by the electromagnetic force. In order to facilitate reasonable ease of fabrication of the core out of metal sheets, a suitable design configuration should be used. The exemplary “E” shaped or “U” shaped cores described herein can be easily fabricated from metal sheets such as an iron sheet. Furthermore the “E” shaped core also provides a large area for the poles developed in the core once the coils are energized. Since the plunger is aligned through the center of the “E” shaped core, the magnetic force generated is distributed uniformly on both sides of the plunger (due to the uniform location of the coils with respect to the center of the “E” core and the movement of the plunger due the electromagnetic force may be balanced adequately.
Operationally, piston 812 assumes the bottom dead center position (shown in
In a solenoid drive embodiment (not shown), one or both the cores may be independently translatable along the translation axis. Such adjustability more particularly allows for adjustment piston travel distance between bottom dead center position and top dead center position, thereby adjusting the capacity of the compressor. In another embodiment, frequency and translation speed may be adjusted by compensating for the accumulator configuration as described above.
While only certain features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. For example,
In an embodiment of the invention, a method of operating a reciprocating compressor comprises accelerating a translatable assembly in a first direction. Acceleration comprises, from a substantially motionless state, applying force to the translatable assembly such that it achieves some desired velocity. Once the target velocity is reached, force is applied to substantially overcome the force applied at the piston face of the translatable assembly by the gas occupying the compression chamber of the reciprocating compressor. Accelerating the translatable assembly imparts inertia to the translatable assembly, and increases the kinetic energy resident in the translatable assembly.
The method further comprises decelerating the translatable assembly while it travels in the first direction. Decelerating the translatable assembly is accomplished by shifting a portion of the inertia resident in the translatable assembly into the accumulator, such as by deforming the above-discussed resilient member. Decelerating the translatable assembly reduces the inertia resident in the translatable assembly, and reduces the kinetic energy associated with the assembly during its movement in the first direction.
The method additionally comprises accelerating the translatable assembly in a second direction using energy stored in the accumulator. In one embodiment, a resilient member, deformed during the first movement of the translatable assembly, relaxes and returns to its original state, thereby applying force to the translatable assembly and accelerating the assembly during its second movement.
It will be understood by those skilled in the art that various changes may be made and equivalents may be substituted without departing from the scope of the invention. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from its scope. Therefore, it is intended that the invention not be limited to the particular embodiment disclosed, but that the invention will include all embodiments falling within the scope of the appended claims.
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