SYSTEMS AND METHODS FOR COMPRESSION AND EXPANSION OF GAS
20230151802 · 2023-05-18
Assignee
Inventors
Cpc classification
F04B35/045
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F04B39/102
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F04B53/1022
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F04B39/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F04B7/0076
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
Abstract
Valves used for reciprocating gas compression and expansion and methods for operating them are provided. In some embodiments, these systems and methods can be used to recover energy in heat pumps, compressed gas systems, and pumped heat energy storage systems. In other embodiments, they may be used for gas compression or both gas compression and expansion.
Claims
1. A valve system operable for use with a reciprocating machine, the valve system comprising: a first valve provided in a first valve housing and a second valve provided in a second valve housing; the first valve housing comprising a first conduit, and the second valve housing comprises a second conduit; the first valve comprising a valve plunger comprising a valve head and a stem and a ferromagnetic member provided on the stem; the second valve comprising a valve plunger comprising a valve head and a stem and a ferromagnetic member provided on the stem; wherein each of the valves comprise a first magnetic pole and a second magnetic pole and wherein the ferromagnetic member is moveable relative to the magnetic poles; wherein the first valve housing and the second valve housing comprise separate housings that are in fluid communication via at least one of the first conduit, the second conduit, and a piston cylinder.
2. The system of claim 1, wherein the first magnetic pole is provided a vertical position that is greater than a vertical position of the second magnetic pole.
3. The system of claim 1, wherein the first valve housing and the second valve housing each comprise a portion of a fluid flow path and wherein first valve and the second valve are in the fluid flow path.
4. The system of claim 1, wherein at least one of the first valve and the second valve comprise a solenoid and wherein the solenoid is provided with forced convective cooling in the fluid flow path.
5. The system of claim 1, wherein at least one of the first magnetic pole and the second magnetic pole are secured by a frame.
6. The system of claim 1, wherein the first and second conduits comprise portions of a bifurcated conduit in communication with a piston cylinder.
7. The system of claim 1, wherein a piston provided in the piston cylinder is operable to perform work on a working fluid, and wherein the system is reversible such that work can be performed on the piston.
8. A valve system operable for use with a reciprocating machine, the valve system comprising: a valve housing comprising a pressure vessel housing a valve; the valve comprising a valve plunger with a valve head and a stem and a ferromagnetic member provided on the stem; a first solenoid operable to receive an electric current and provide a magnetic force to the ferromagnetic member; a second solenoid operable to receive an electric current and provide a magnetic force to the ferromagnetic member; a first magnetic pole and a second magnetic pole and wherein the ferromagnetic member is moveable relative to the magnetic poles and the magnetic poles are operable to selectively control a vertical position of the valve head; a first conduit and a second conduit in communication with the valve housing, wherein the valve is in selective communication with a seat provided between the valve housing and the second conduit; and wherein a fluid flow path is provided that extends from the first conduit to the pressure vessel and to the second conduit, and wherein the first and second solenoids are provided in the fluid flow path.
9. The valve system of claim 8, wherein the first magnetic pole is provided a vertical position that is greater than a vertical position of the second magnetic pole.
10. The valve system of claim 8, wherein the fluid flow path is reversible.
11. The valve system of claim 8, wherein at least one of the first magnetic pole and the second magnetic pole are secured by a frame.
12. The valve system of claim 8, wherein the second conduit is provided in fluid communication with a piston cylinder at least when the valve is provided in an open position.
13. The valve system of claim 8, further comprising a second valve housing comprising a second valve.
14. The valve system of claim 13, further comprising a piston cylinder and wherein the piston cylinder is in fluid communication with the first valve housing and the second valve housing.
15. A method of gas compression and expansion, the method comprising: providing a first chamber and a second chamber, the first chamber comprising a first valve operable to control fluid flow to and from the first chamber and the second chamber comprising a second valve operable to control fluid flow to and from the second chamber; each of the first valve and the second valve being in communication with a solenoid and a magnetic pole; providing a controller in communication with at least one of the first valve and the second valve; determining, based on a measured reluctance of a magnetic circuit of at least one of the first valve and the second valve, a valve plunger position; and adjusting with the controller at least one of timing and position of at least one of the first valve and the second valve.
16. The method of claim 15 wherein the valve plunger position between open and closed states is measured and controlled in sequential time intervals of an operating cycle.
17. The method of claim 15, wherein an effective voltage across the solenoid is controlled by applying pulses having an intended duty cycle.
18. The method of claim 15, wherein valve plunger position is determined using electrical measurements on the valves and a valve plunger position is controlled in a proportional-integral-derivative control feedback loop.
19. The method of claim 17, wherein a preferred effective voltage is calculated based on a preferred target current and a length of the subsequent interval.
20. The method of claim 19, further comprising a step of detecting a pressure reversal across a valve, and wherein the system is devoid of pressure sensors.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0038] The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate embodiments of the invention and together with the Summary given above and the Detailed Description of the drawings given below, serve to explain the principles of these embodiments. In certain instances, details that are not necessary for an understanding of the invention or that render other details difficult to perceive may have been omitted. It should be understood, of course, that the invention is not necessarily limited to the particular embodiments illustrated herein. Additionally, it should be understood that the drawings are not necessarily to scale.
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DETAILED DESCRIPTION
[0055]
[0056] Covers 6, 7 are fastened around their periphery by bolts to cylinder head 5. Gaskets are contemplated as being provided in some embodiments between the covers 6, 7 and cylinder head 5 and between cylinder head 5 and piston-cylinder 2 to help prevent gas leakage. The valve set 1 includes electronic auxiliaries (not shown in
[0057]
[0058] The referenced Norris Application discloses a system of energy storage and management. Systems and methods of the present disclosure, including valve systems, are contemplated for use with (but are not limited to) the systems of the Norris Application. For example, various embodiments of the present disclosure contemplate cylinders that are provided to perform compression and/or expansion of a working fluid of the kind referred to in the Norris Application as “dual-purpose” cylinders.
[0059] One embodiment of a valve set intended for use with a dual purpose cylinder is shown in
[0060] A cylinder head 5 may be manufactured as a single cast metal part, such as cast iron, using sand casting methods or similar methods known in the art. The parting plane between cope and drag may be the vertical centerline of
[0061] The elements of
[0062] At a predetermined point, as the piston 20a continues its downward motion, the high side plunger 16 is lowered to a closed position against its seal, preventing further flow from high side pressure vessel or chamber 18 into high side conduit 14. Flow through the high side port 4 stops. The gas below the high side plunger 16 expands because the variable cylinder volume 20 increases. In this state, the system contains three separate pressure regions: the high side pressure, the low side pressure, and an intermediate pressure found in the volume made up of high side conduit 14, cylinder port 15, cylinder volume 20, low side conduit 13, and low side pressure vessel or chamber 19. The intermediate pressure is lower than the high side pressure, so a downward force develops on high side plunger 16, forcing its seal and preventing flow past the high side plunger 16.
[0063] The intermediate pressure drops until such time as it reaches equilibrium with the low side pressure, i.e., when the pressure in the low side pressure vessel 19 equals the low pressure in the low side external pipe 11. As there is no longer any pressure differential across the head of low side plunger 17, it can move freely. In this state low side plunger 17 is opened, and the system again contains only two pressure regions: a low-pressure region contained in all elements between low pressure port 3 and the high side plunger 16, and a high pressure region between high side plunger 16 and the high side port 4.
[0064] For a short period of time near the end of the piston's 20a downward motion, low pressure gas is drawn into the system through the low pressure port 3, into the low side external pipe 11, into low side pressure vessel 19, through low side conduit 13, through cylinder port 15, and into cylinder volume 20. However, once the piston is fully drawn or expanded, the piston reverses its course and starts moving in the upward (i.e., compression) direction. The flow reverses, and a large volume of low-pressure gas is expelled via low pressure port 3.
[0065] At a predetermined point, the low side plunger 17 closes while the piston 20a continues its upward motion. This action again separates the system into three separate pressure regions. The intermediate pressure rises, forcing low side plunger 17 against its seal. The intermediate pressure rises until the point when it is in equilibrium with the high-pressure source gas. At this point, high side plunger 16 is free to move. The high side plunger 16 is opened, and the system is again returned to two pressure regions. For a short period at the end of the piston's upward motion, high pressure gas is forced out of the high-pressure port 4, but then the piston then reaches a fully compressed position, begins its downward motion, gas is draw in through high pressure port 4, and the cycle repeats.
[0066] During the expansion cycle just described, the gas is drawn into the cylinder at high pressure and expanded in the cylinder at intermediate pressure. During these two processes, work is done by the gas on the piston 20a. Gas is then expelled at low pressure, requiring a small amount of work to overcome internal friction, and then the piston must compress a small amount of residual cylinder gas to reach high pressure, also requiring work. In all, net work is done on the piston, and this may be employed for useful purposes including, for example, energy recovery.
[0067] The valve set may also be operated as a compressor. In this case, and again with reference to
[0068] Dimensions of high side flow channels, plungers, and ports may be smaller than their low side counterparts because they contain higher pressure gas with lower specific volume. In the figures and description of this disclosure, they are shown to have identical dimensions for simplicity.
[0069] Other geometries are contemplated including those having plungers that open in the downward direction, those with plungers moving in a direction other than vertical, those moving in a rotational motion, and those with plunger heads and mating valve seats having a geometry other than flat.
[0070]
[0071] In some embodiments, plungers are moved in one direction by an electromagnet and in the opposite direction by a spring. For example, the plunger(s) is/are contemplated as being raised by an electromagnetic force and biased closed by a spring. In a preferred embodiment, described in detail below, plungers are moved in both directions by electromagnets. Collectively, two fixed electromagnets and the moving plunger comprise a variation of the linear switched reluctance motor with only two stator poles, the poles being placed on opposite sides of the mover (or rotor), and with continuous or near-continuous overlap of the ring and all poles. The linear motor offers several advantages over the spring alternative: it avoids wear and failure of the spring and improves reliability. It avoids the materials uncertainty of fatigue strength in high temperature environments. It avoids the need to overdesign the spring so that it provides sufficient force at partial compression, while providing excessive force at full compression, thereby requiring overdesign of the compressing electromagnet.
[0072] In some embodiments, the ring comprises a permanent magnet. In some embodiments the ring comprises a permanent magnet and the valve comprises a single electromagnet and a spring. In some embodiments, additional poles are added to the stator and/or mover.
[0073]
[0074] A lower electromagnet is provided that comprises lower magnetic poles 31, 32. As shown in
[0075] The magnetic core 35 and the magnetic poles 31, 32 are made from a ferromagnetic material. In some embodiments, the poles comprise pressed iron powder. The powder, used in the manufacture of some inductors, is made from discrete insulated high-permeability ferromagnetic particles, and is selected with a suitably high Curie temperature. The magnetic core 35 is mechanically clamped or similarly secured to poles 31 and 32, which are shaped and arranged geometrically to approach the plunger from either side and surround the plunger ring in a close, non-contact, proximal relationship at terminals 37a, 37b. Poles may be made of the same material and in the same manner as the core. The terminals 37a, 37b preferably comprise curvilinear or C-shaped terminals to increase surface area, but no limitation with respect to the shape of the terminals 37a, 37b are provided.
[0076] The electromagnet and plunger together form a magnetic circuit as follows. The solenoid 34 produces magnetomotive force (MMF). This produces magnetic flux which passes through the core 35, through the first pole 32, crosses a first gap between the pole and the plunger ring 24, continues around the ring, crosses a second gap, and returns via the second pole 31 to the core and solenoid. These components are designed such that the magnetic force will be sufficient to move the plunger along its intended path of motion. The poles are contemplated as comprising curved terminals 37a, 37b to follow the shape of the ring while maintaining a constant gap, as shown. The system comprises a solenoid that is operable to produce a magnetic flux and operate as a switched reluctance motor.
[0077] Current to and from solenoid 34 is provided by wires (not shown) from the high pressure conductor feedthrough 8 shown in
[0078] The reluctance of the magnetic circuit derives primarily from the two gaps of the magnetic circuit. Reluctance depends upon the size of the gap, i.e., the distance between the ring and terminals 37a, 37b, and the area of overlap between the ring and terminals. The gap size is fixed, but the area of overlap varies by plunger position. When the plunger is in a position having high overlap, the reluctance is small, and this corresponds to high magnetic flux. When the plunger is in a position with small overlap, the reluctance is high, and this corresponds to low magnetic flux. The relationship between plunger position and reluctance is central to the position detection method described later.
[0079] The height of the poles and the vertical spacing between upper magnet poles 29, 30 and lower magnet poles 31, 32 are sized based on considerations of the ring height and the maximum vertical distance of plunger travel. These dimensions may be such that there is always some minimum amount of overlap, regardless of plunger position.
[0080]
[0081] The low side linear motor 36 is shown in exploded view in
[0082] Additional features of the lower frame 25 are shown in
[0083]
[0084] The solenoid 34 of the lower electromagnet 33 is represented in
[0085] Current i.sub.1 is manipulated by valve controller 43 by switching transistors T.sub.1 and T.sub.2 ON and OFF in four possible configurations. In the first configuration, both T.sub.1 and T.sub.2 are ON, allowing current to flow from the positive rail at node b, through T.sub.1 to node f, through S.sub.1 to node g, and through T.sub.2 to the negative rail at node n. This configuration applies driving voltage v.sub.r across S.sub.1 such that the potential at node f relative to node g is v.sub.r. This will cause a change in current i.sub.1. If the plunger were immobile in its closed position, for example, this configuration would cause current i.sub.1 to increase at a rate inversely proportional to the inductance of S.sub.1. In the second configuration, both T.sub.1 and T.sub.2 are OFF, preventing current from flowing between b and f and between g and n. However, current is allowed to flow through S.sub.1 along the path m-f-g-c, in which case the negative driving voltage is applied, that is, the potential at node f relative to node g is −v.sub.r. This configuration would cause current i.sub.1 to decrease. In the third configuration, T.sub.1 is ON and T.sub.2 is OFF. This permits circulation of current along the path b-f-g-c-b, although no driving voltage is applied: the potential at f relative to g is zero. Finally, in the fourth configuration, T.sub.1 is OFF and T.sub.2 is ON. This permits circulation of current along the path m-f-g-n-m, with no voltage applied. Current i.sub.2 through solenoid S.sub.2 may be similarly manipulated using the same four transistor configurations applied to T.sub.3 and T.sub.4.
[0086] In some embodiments, pulse width modulation (PWM) is contemplated as being used to approximate a time-varying analog voltage profile applied across the terminals of each solenoid. This is illustrated in
[0087] Switching transistors as described above results indirectly in the control of electric currents through the solenoids, magnetic fluxes in the cores and poles, magnetic forces on the plungers, and plunger motion. These methods may be used to match a predefined kinematic behavior of the plungers, such as path s(t) shown in
[0088] To compare the actual plunger position against the idealized cycle path s(t) of
[0089] By Faraday's law, the voltage v across a solenoid is equal to the number of turns N around the core times the rate of change of magnetic flux ϕ through the core. The flux depends upon solenoid current i and position z of the plunger along its vertical axis. Faraday's law may therefore be expanded as Eqn. 1:
v=N∂ϕdi/∂i dt+N∂ϕdz/∂z dt
The first term of Eqn. 1 is in the form of voltage across a stationary inductor. The second term relates solenoid voltage to plunger speed. The above equation may be re-written as Eqn. 2:
v=LΔi/Δt+Ku
where the current-related differentials are replaced by finite intervals, the coefficient in the first term is replaced by a defined inductance L, the coefficient in the second term is replaced by K, and the plunger speed is denoted u. Inductance L is known to be a function of plunger position because the reluctances of the two pole-ring gaps depend on the areas of overlap, and these change with plunger position. K is known to be a function of current because flux ϕ is a function of current, and the definition of K−N times the partial derivative of ϕ with respect to z—holds current constant. Furthermore, we know based on physical laws that neither plunger speed u nor current i can change instantaneously (as in step functions), even when a voltage is applied or removed at the solenoid terminals. They may, however, change in a continuous fashion.
[0090] In reference to
[0091] In some embodiments, the conversion to position is based an empirical lookup table developed and added to the valve controller 43 prior to operation. The table may be created by independently measuring position and inductance at several points. Later, when operating the valve, the controller interpolates position based on data contained in the table. In some embodiments, the data may instead be converted into a model function, such as a polynomial, with coefficients selected to fit the function to the measured data. Model coefficients are added to the controller. The controller may then use the same model and coefficients during operation to calculate position as a function of inductance.
[0092] In some embodiments, the controller includes a self-calibration mode that is performed prior to operation. This mode may be automatically performed at any time. This mode assumes a model form, such as a linear relationship, between inductance and position. When operated in such a mode, the controller determines the inductance at each of the two extreme known positions as limited by physical stops. It can do this by measuring inductance over a range of conditions and determining the minimum and maximum inductance. In the upper electromagnet, inductance increases with z, and in the lower electromagnet, the inductance decreases with z, so it is possible to determine in both cases the inductance at the closed position and at the maximum open position. From these two points and the assumed model form, the controller can interpolate to create intermediate points of position z and inductance L. It can then create either a lookup table or model function as described above. The linear model is preferred for its simplicity. The actual relationship is of course not linear because of complicated flux fringing between the poles and ring. However, the intended purpose is not to accurately measure position, but rather to open and close a valve along a smooth, continuous pathway, even if this deviates from s(t).
[0093] Valves never open against a significant pressure gradient. For example, when the valve set is operated as a compressor, gas is drawn into the cylinder through the low-pressure valve, but the valve is only opened when the gas inside the cylinder is approximately equal to the low-pressure source. Also, the drawing of gas by the piston into the cylinder forces open the valve because the expanding cylinder volume results in an internal cylinder pressure lower than the low port pressure. The pressure difference produces a force in the upward direction needed to begin opening it passively, like a check valve. The movement of the plunger may then be detected, triggering the controller to actively open the valve.
[0094] Embodiments of the present disclosure provide for methods of detecting the time at which valves should open. The following cases are relevant: in compression when drawing gas through the low side valve; in compression when expelling gas through the high side valve; in expansion when expelling gas through the low side valve; and in expansion when drawing gas through the high side valve. In all these cases, the valves should open when the pressures on either side of the plunger heads are equal.
[0095] According to one embodiment, whenever either valve is closed, it is not necessary to actively control its position. Instead, the plunger is held closed by the pressure above the valve head. This is true for both valves and for both compression and expansion. Though the plunger when closed does not need active control, the method for detecting position is applied continuously. When the plunger position changes from closed to any detectable positive position above its seat, the time for opening the valve is discovered, and the active motion control is initiated.
[0096] Embodiments of the present disclosure provide for methods of computing sequential PWM duty cycles to reach target solenoid currents. The target solenoid current is the current calculated by the controller in one measurement interval to be carried in the solenoid by the end of the following interval. It may be obtained in any number of ways. In some embodiments a PID controller may be used to calculate a control variable as the sum of PID terms using established PID methods. The control variable may be positive or negative. Referring to
[0097] Regardless of the method for setting target solenoid currents, the following method may be used to set the effective voltage and duty cycles such that the target currents may be reached in the next interval. Inductance L and term Ku are calculated using the methods described previously for determining plunger position. Then, using Eqn. 2, the controller computes effective voltage v required in the next interval. In this calculation, Δi is the required increase in current, i.e., the target current minus the most recent measured current, and Δt is the duration of the interval, T.sub.S. Finally, the duty cycle is the resulting effective voltage v divided by the rail voltage v.sub.r. For example, if the required effective voltage is 75 V and the rail voltage is 100 V, then the duty cycle to be used in the next interval is 0.75. This means that the controller will impose v.sub.r on the solenoid for 75% of the interval, followed by zero volts for 25% of the interval using transistor switching. In some cases, the calculated duty cycle will exceed 1, in which case the duty cycle will be limited, and the target current will not be reachable in a single interval. The resulting error will be reflected in the next duty cycle calculation.
[0098] Embodiments of the present disclosure provide for methods of recovering energy used to open and close the valves during braking periods. In various embodiments, upon opening, electrical energy is converted to kinetic energy by putting the plunger into motion. As the plunger slows, whether slowing to the open position or the closed position, the kinetic energy is recovered and returned to the rail.
[0099] For example, a plunger may be provided in upward motion by activating the upper electromagnet (i.e., current was introduced into the upper electromagnet). To slow the plunger as it approaches an upper limit, the lower electromagnet is be activated, and the upper electromagnet is deactivated. Whether this is performed using PID control or other control method, the effect is the same. Referring to
[0100] Although the foregoing text sets forth a detailed description of numerous different embodiments, it should be understood that the detailed description is to be construed as exemplary only and does not describe every possible embodiment since describing every possible embodiment would be impractical, if not impossible. Numerous alternative embodiments could be implemented, using either current technology or technology developed after the filing date of this patent, which would still fall within the scope of the claims. To the extent that any term recited in the claims at the end of this patent is referred to in this patent in a manner consistent with a single meaning, that is done for sake of clarity so as to not confuse the reader, and it is not intended that such claim term by limited, by implication or otherwise, to that single meaning.
[0101] While various embodiments of the present invention have been described in detail, it is apparent that modifications and alterations of those embodiments will occur to those skilled in the art. Moreover, references made herein to “the present invention” or aspects thereof should be understood to mean certain embodiments of the present invention and should not necessarily be construed as limiting all embodiments to a particular description. It is to be expressly understood that such modifications and alterations are within the scope and spirit of the present invention.