This section is intended to introduce the reader to various aspects of art that may be related to various aspects of the present invention, which are described and/or claimed below. This discussion is believed to be helpful in providing the reader with background information to facilitate a better understanding of the various aspects of the present invention. Accordingly, it should be understood that these statements are to be read in this light, and not as admissions of prior art.
Rotating equipment often utilizes the energy of fluids directed toward the rotating equipment to drive rotation. However, severe inlet configurations may lead to impingement, mixing of liquids, choked flow, cavitation, and/or reduced efficiencies and output of the rotating equipment.
Various features, aspects, and advantages of the present invention will become better understood when the following detailed description is read with reference to the accompanying figures in which like characters represent like parts throughout the figures, wherein:
One or more specific embodiments of the present invention will be described below. These described embodiments are only exemplary of the present invention. Additionally, in an effort to provide a concise description of these exemplary embodiments, all features of an actual implementation may not be described in the specification. It should be appreciated that in the development of any such actual implementation, as in any engineering or design project, numerous implementation-specific decisions must be made to achieve the developers' specific goals, such as compliance with system-related and business-related constraints, which may vary from one implementation to another. Moreover, it should be appreciated that such a development effort might be complex and time consuming, but would nevertheless be a routine undertaking of design, fabrication, and manufacture for those of ordinary skill having the benefit of this disclosure.
When introducing elements of various embodiments of the present invention, the articles “a,” “an,” “the,” and “said” are intended to mean that there are one or more of the elements. The terms “comprising,” “including,” and “having” are intended to be inclusive and mean that there may be additional elements other than the listed elements.
As discussed in detail below, a hydraulic energy transfer system transfers work and/or pressure between a first fluid (e.g., a pressure exchange fluid) and a second fluid (e.g., frac fluid or a salinated fluid). In certain embodiments, the first fluid may be substantially “cleaner” than the second fluid. In other words, the second fluid may contain dissolved or suspended particles. Moreover, in certain embodiments, the second fluid may be more viscous than the first fluid. Additionally, the first fluid may be at a first pressure between approximately 5,000 kPa to 25,000 kPa, 20,000 kPa to 50,000 kPa, 40,000 kPa to 75,000 kPa, 75,000 kPa to 100,000 kPa or greater than a second pressure of the second fluid. In operation, the hydraulic energy transfer system may or may not completely equalize pressures between the first and second fluids. Accordingly, the hydraulic energy transfer system may operate isobarically, or substantially isobarically (e.g., wherein the pressures of the first and second fluids equalize within approximately +/−1, 2, 3, 4, 5, 6, 7, 8, 9, or 10 percent of each other).
The hydraulic energy transfer system may also be described as a hydraulic protection system, hydraulic buffer system, or a hydraulic isolation system, because it blocks or limits contact between the second fluid and various pieces of hydraulic equipment (e.g., high-pressure pumps, heat exchangers), while still exchanging work and/or pressure between the first and second fluids. By blocking or limiting contact between various pieces of hydraulic equipment and the second fluid (e.g., more viscous fluid, fluid with suspended solids), the hydraulic energy transfer system reduces abrasion/wear, thus increasing the life/performance of this equipment (e.g., high-pressure pumps). Moreover, it may enable the hydraulic system to use less expensive equipment, for example high-pressure pumps that are not designed for abrasive fluids (e.g., fluids with suspended particles). In some embodiments, the hydraulic energy transfer system may be a hydraulic turbocharger, a rotating isobaric pressure exchanger (e.g., rotary IPX), or a non-rotating isobaric pressure exchanger (e.g., bladder, reciprocating isobaric pressure exchanger). Rotating and non-rotating isobaric pressure exchangers may be generally defined as devices that transfer fluid pressure between a high-pressure inlet stream and a low-pressure inlet stream at efficiencies in excess of approximately 50%, 60%, 70%, 80%, or 90% without utilizing centrifugal technology.
As explained above, the hydraulic energy transfer system transfers work and/or pressure between first and second fluids. These fluids may be multi-phase fluids such as gas/liquid flows, gas/solid particulate flows, liquid/solid particulate flows, gas/liquid/solid particulate flows, or any other multi-phase flow. Moreover, these fluids may be non-Newtonian fluids (e.g., shear thinning fluid), highly viscous fluids, non-Newtonian fluids containing proppant, or highly viscous fluids containing proppant. The proppant may include sand, solid particles, powders, debris, ceramics, or any combination therefore. For example, the disclosed embodiments may be used with oil and gas equipment, such as hydraulic fracturing equipment using a proppant (e.g., particle laden fluid) to frac rock formations in a well.
In an embodiment using a hydraulic turbocharger, the first fluid (e.g., high-pressure proppant free fluid) enters a first side of the hydraulic turbocharger and the second fluid (e.g., low-pressure frac fluid) may enter the hydraulic turbocharger on a second side. In operation, the flow of the first fluid drives a first turbine coupled to a shaft. As the first turbine rotates, the shaft transfers power to a second turbine that increases the pressure of the second fluid, which drives the second fluid out of the hydraulic turbocharger and down a well during fracturing operations. In an embodiment using an isobaric pressure exchanger (IPX), the first fluid (e.g., high-pressure proppant free fluid) enters a first side of the hydraulic energy transfer system where the first fluid contacts the second fluid (e.g., low-pressure frac fluid) entering the IPX on a second side. The contact between the fluids enables the first fluid to increase the pressure of the second fluid, which drives the second fluid out of the IPX and down a well for fracturing operations. The first fluid similarly exits the IPX, but at a low-pressure after exchanging pressure with the second fluid.
As used herein, the isobaric pressure exchanger (IPX) may be generally defined as a device that transfers fluid pressure between a high-pressure inlet stream and a low-pressure inlet stream at efficiencies in excess of approximately 50%, 60%, 70%, or 80% without utilizing centrifugal technology. In this context, high pressure refers to pressures greater than the low pressure. The low-pressure inlet stream of the IPX may be pressurized and exit the IPX at high pressure (e.g., at a pressure greater than that of the low-pressure inlet stream), and the high-pressure inlet stream may be depressurized and exit the IPX at low pressure (e.g., at a pressure less than that of the high-pressure inlet stream). Additionally, the IPX may operate with the high-pressure fluid directly applying a force to pressurize the low-pressure fluid, with or without a fluid separator between the fluids. Examples of fluid separators that may be used with the IPX include, but are not limited to, pistons, bladders, diaphragms and the like. In certain embodiments, isobaric pressure exchangers may be rotary devices. Rotary isobaric pressure exchangers (IPXs) 20, such as those manufactured by Energy Recovery, Inc. of San Leandro, Calif., may include ramped inlets configured to induce rotation of a rotor of the IPX, as described in detail below with respect to
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In some embodiments, a controller using sensor feedback may control the extent of mixing between the first and second fluids in the rotary IPX 160, which may be used to improve the operability of the fluid handling system. For example, varying the proportions of the first and second fluids entering the rotary IPX 160 allows the plant operator to control the amount of fluid mixing within the hydraulic energy transfer system. Three characteristics of the rotary IPX 160 that affect mixing are: (1) the aspect ratio of the rotor channels 190, (2) the short duration of exposure between the first and second fluids, and (3) the creation of a fluid barrier (e.g., an interface) between the first and second fluids within the rotor channels 190. First, the rotor channels 190 are generally long and narrow, which stabilizes the flow within the rotary IPX 160. In addition, the first and second fluids may move through the channels 190 in a plug flow regime with very little axial mixing. Second, in certain embodiments, the speed of the rotor 166 reduces contact between the first and second fluids. For example, the speed of the rotor 166 may reduce contact times between the first and second fluids to less than approximately 0.15 seconds, 0.10 seconds, or 0.05 seconds. Third, a small portion of the rotor channel 190 is used for the exchange of pressure between the first and second fluids. Therefore, a volume of fluid remains in the channel 190 as a barrier between the first and second fluids. All these mechanisms may limit mixing within the rotary IPX 160. Moreover, in some embodiments, the rotary IPX 160 may be designed to operate with internal pistons that isolate the first and second fluids while enabling pressure transfer.
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As described above, the first fluid 208 enters the inlet 176 and is directed toward the rotor 166 via the aperture 196. In certain embodiments, the aperture 196 includes a sloped face configured to direct the first fluid 208 into the channel 90 at an angle (e.g., the aperture 196 directs the first fluid 208 against a wall of the channel 90). Accordingly, energy from the first fluid 208 may be transferred to the rotor 166, thereby facilitating rotation of the rotor 166 about the axis 188.
In the illustrated embodiment, the torque generated by a supply of fluid entering the rotor 166 is represented by a first line 216. The torque is a function of RPM as well as several characteristics of the system. For example, the flow rate of the first fluid 208 directed toward the rotary IPX 160 may affect the supply, and therefore the position of the first line 216. Accordingly, the flow rate of the first fluid 208 entering the rotor 166 may change the slope of the first line 216. Additionally, the geometry of the apertures 196, 198, 200, 202 may also impact the position of the first line 216. In certain embodiments, the flow rate may be substantially constant (e.g., constrained by associated equipment). Accordingly, to adjust the position of the first line 216, modifications to the inlet geometry of components of the rotary IPX 160 may be utilized.
A second line 218 represents a torque demand or load of the rotor 166. For example, the second line 218 may represent the torque associated with a given rotational speed. Like the supply, the demand is a function of several characteristics of the system. For example, the viscosity of the fluid utilized in the system may increase the load on the rotor 166, thereby shifting the position of the second line 218. Moreover, the inlet geometries, clearances between the rotor 166 and sleeve 164, clearance between the rotor 166 and the end covers 184, 186, operating conditions, and other equipment associated with the system may also affect the torque demand on the rotor 166. In the illustrated embodiment, the first and second lines 216, 218 intersect at a first steady state point 220. The first steady state point 220 represents the desired RPM (e.g., steady state RPM) of the rotor given a particular torque supplied and torque demand. As will be described below, changes and/or shifts in the torque supply or torque demand applied to the system may change the position of the steady state point.
Under certain operating conditions, the demand on the rotor 166 may change. For example, the viscosity of the first and/or second fluids 208, 206 may increase, thereby generating a greater demand on the rotor 166. As a result, the second line 218 shifts in the direction 222 to form a third line 224. In the illustrated embodiment, third line 224 intersects the first line 216 at a second steady state point 226. The second steady state point 226 is at a point representing a lower RPM, while also utilizing a higher torque than the first steady state point 220. As a result, the larger demand placed on the rotor 166 slows the rotor 166 down while simultaneously using a larger torque to induce rotation of the rotor 166.
As mentioned above, the supply, represented by the first line 216, is a function of the flow rate, geometry of the rotary IPX, and the like. In certain embodiments, it may be difficult or undesirable to raise the flow rate of the supply. For instance, increasing the flow rate may damage associated piping coupling the rotary IPX 160 to the system. Therefore, in certain embodiments, modifications to the inlet geometry of the rotary IPX 160 may increase the torque applied to the rotor 166 without modifying the flow rate. For instance, the geometry of the aperture 196 may direct the supply toward an interior surface of the channel 190, thereby transferring a larger amount of force to the rotor 166 to facilitate rotation. As shown, the first line 216 is shifted in a direction 228 to form a fourth line 230. The fourth line 230 represents a supply configured to apply a larger torque to the rotor 166 than the first line 216. The third line 224 and the fourth line 230 intersect at a third steady state point 232 to establish a desired speed of operation of the rotor 166. It should be noted that the RPM of the third steady state point 232 is substantially equal to the RPM at the first steady state point 220. Accordingly, modifications to the inlet geometry of the rotary IPX 160 may enable the rotor 166 to maintain a desired speed (e.g., steady state RPM) while a larger load is acting to the rotor 166.
The angle 236 of the first flow path 234 is configured to generate sufficient force to maintain rotation of the rotor 166 about the axis 188, while also decreasing the likelihood of mixing within the channel 190. For example, the first fluid 208 contacts the second fluid 206 in the channel (e.g., at the dynamic fluid interface 210) to drive the second fluid 206 from the channel 190. As a result, the portion of the flow directed along the channel axis 238 is configured to be sufficient to drive the second fluid 206 from the channel 190 while minimizing the contact time between the first and second fluids 208, 206. Minimizing the contact time between the first and second fluids 208, 206 reduces the likelihood of mixing.
In the illustrated embodiment, the angle 236 is approximately 30 degrees relative to the channel axis 238. However, in other embodiments, the angle 236 may be greater than, less than, or equal to approximately 10 degrees, approximately 20 degrees, approximately 40 degrees, approximately 50 degrees, approximately 60 degrees, approximately 70 degrees, approximately 80 degrees, or any suitable angle to facilitate rotation of the rotor 166. Moreover, the angle 236 may be between approximately 10 degrees and approximately 20 degrees, approximately 20 degrees and approximately 30 degrees, approximately 30 degrees and approximately 40 degrees, approximately 40 degrees and approximately 50 degrees, approximately 50 degrees and approximately 60 degrees, approximately 60 degrees and approximately 70 degrees, approximately 70 degrees and approximately 80 degrees, or any other suitable range. Additionally, the angle 236 may be less than approximately 20 degrees, less than approximately 30 degrees, less than approximately 40 degrees, less than approximately 50 degrees, less than approximately 60 degrees less than approximately 70 degrees, less than approximately 80 degrees, less than approximately 90 degrees, or any other angle configured to generate rotation of the rotor 166. Accordingly, the angle 236 is configured to direct the fluid into the channels 190 to facilitate rotation of the rotor 166 while also driving fluid from the channels 190.
In certain embodiments, the aperture 200 (e.g., the outlet) may also include a sloped interface to facilitate rotation of the rotor 166. For example, the geometry of the aperture 200 may mirror the geometry of the aperture 196. However, in other embodiments, the sloped interfaces of the apertures 196, 200 may be different. For example, the sloped interface of the aperture 196 may be more severe (e.g., a larger angle 236) than the sloped interface of the aperture 200.
To generate rotation of the rotor 166, the rotary IPX 160 may also include guide vanes positioned on the sloped interfaces of the apertures 196, 198, 200, 202 to direct the fluid. For example, the guide vanes may include raised protrusions on the sloped interface configured to direct the fluid toward the channels at the angle 236. In certain embodiments, the guide vanes may be distributed along the face of the apertures 196, 198, 200, 202. However, in other embodiments, the guide vanes may be positioned within the channels 190 to facilitate additional rotational force upon the rotor 166.
Furthermore, in certain embodiments, fluid jets may be positioned proximate to the rotor 166. For example, the fluid jets may include outlet nozzles positioned at an angle (e.g., the angle 236) relative to the channels 190. To this end, the fluid jets may direct the fluid toward the channels 190 at an angle sufficient to induce rotation of the rotor 166 while maintaining minimal mixing between the first fluid 208 and the second fluid 206. As will be appreciated, the outlet nozzles of the fluid jets may have smaller cross-sectional areas than the conduits directing the fluid toward the fluid jets, thereby increasing the velocity of the fluid as it exits the outlet nozzles. As a result, the supply (e.g., line 216) may shift in the direction 228 because of the configuration of the outlet nozzles of the fluid jets. Additionally, in other embodiments, apertures 196, 198, 200, 202 converge toward the channel, thereby increasing the velocity of the fluid as it enters the channels 190. Furthermore, in certain embodiments, the inlet angle may vary across the apertures (e.g., the aperture 196). For example, the inlet angle may be smaller at a first end of the aperture in which the dynamic fluid interface 210 is closer to the edge of the channel 190 and larger at a second end of the aperture in which the dynamic fluid interface 210 is farther from the edge of the channel 190. That is, as the dynamic fluid interface 210 is moved toward the second end of the channel 190 (e.g., toward the aperture 200), the inlet angle may increase to generate more torque.
A fourth section 254 represents a dead head in the channel 190 as the fluid drives the dynamic fluid interface 210 through the channel 190. In the illustrated embodiment, the channel 190 is not in fluid contact with the aperture (e.g., the aperture 200 at the outlet of the channel 190) through the fourth section 254. As a result, the outlet of the channel 190 is blocked, thereby blocking the first fluid 208 from driving the second fluid 206 from the channel 190. Accordingly, the acceleration line 246 has a negative value because of the decreased acceleration caused by the blockage of the outlet of the channel 190. A fifth section 256 illustrates the acceleration line 246 with a substantially zero slope. Additionally the magnitude of the acceleration line 246 is substantially zero because the channel 190 is not fluidly coupled to the apertures (e.g., the aperture 200). In other words, the fluid may be stationary in the channel 190 in the fifth section 256. However, once the outlet of the channel 190 aligns with the aperture (e.g., the aperture 200), the first fluid 208 may drive the second fluid 206 from the channel 190. Finally, a sixth section 258 represents a mirrored image of the first, second, third, fourth, and fifth sections 248, 250, 252, 254, 256 as the first fluid 208 (now having a low pressure as opposed to a high pressure) is driven from the channel 190 by the second fluid 206 (now having a higher pressure than the low pressure first fluid 208).
The velocity line 266 is obtained by integrating the angular acceleration (e.g., the acceleration line 246) of the fluid (e.g., the first fluid 208) as the fluid moves through the channel 190. Additionally, the position line 268 is obtained by integrating the velocity line 266. As the fluid enters the channel 190, the fluid facilitates rotation of the rotor 166. In a first section 270, the velocity line 266 has a positive slope due to the force exerted on the dynamic fluid interface 210 by the fluid. Additionally, the position line 268 also has a positive slope, representing a change in the position of the dynamic fluid interface 210 facilitated by the driving force of fluid (e.g., the first fluid 208) entering the channel 190. A second section 272 represents a dead head scenario in which the dynamic fluid interface 210 substantially stops before the dynamic fluid interface 210 is driven toward a far end of the channel 190. For example, as described above, the channel 190 may not be in fluid contact with the apertures while the flow dead heads. As shown, the position line 268 is substantially unchanged in the second section 272. However, the velocity line 266 has a downward slope, indicating a slowing and/or stoppage of the dynamic fluid interface 210 (e.g., at approximately a center position of the channel 190).
Additionally, a third section 274 represents a substantial stoppage of the dynamic fluid interface 210. As shown, both the velocity line 266 and the position line 268 have substantially zero slope. In the illustrated embodiment, the third section 274 represents the dynamic fluid interface 210 before the entering fluid drives the fluid in the channel 190 out of the channel 190. A fourth section 276 substantially mirrors the first, second, and third sections 270, 272, 274 as the first fluid 208 is driven from the channel 190 by the second fluid 206 in an opposite direction.
The acceleration profile may be integrated to determine a velocity profile, as represented by block 282. For example, the acceleration profile may be integrated with respect to time. Accordingly, a representation of the velocity may be generated. In certain embodiments, the velocity profile may be compared to the acceleration profile. As will be appreciated, the velocity profile may substantially correspond to the acceleration profile (e.g., velocity increases as acceleration increases). Then, the velocity profile may be integrated to determine a position profile, as represented by block 284. For example, the velocity profile may be integrated with respect to time to determine the position of the dynamic fluid interface 210 in the channel 190. Thereafter, the velocity profile may be compared to the position profile, as represented by block 284. For example, the shape of the velocity profile may substantially correspond to the shape of the position profile, as represented by line 286. As will be appreciated, because the velocity of the dynamic fluid interface 210 is directly related to the position of the dynamic fluid interface 210, the profiles may substantially correspond to represent the dynamic fluid interface 210 moving through the channel 190. If the profiles correspond, as represented by line 288, the fluid inlet angle (e.g., plug flow angle) may be calculated, as represented by block 290. Upon determining the fluid inlet angle, end covers having the ramps at the calculated fluid inlet angle may be manufactured.
In certain embodiments, the fluid inlet angle may be determined as a function of the rotor index angle. For example, the axial component may be determined utilizing the velocity profile. Additionally, the circumferential velocity may be a product of the radius of the rotor 166 and the angular velocity of the rotor 166. Accordingly, the fluid inlet angle may be calculated to reduce mixing of the first and second fluids 208, 206 at the dynamic fluid interface 210 while generating sufficient torque on the rotor 166. In embodiments where the fluid inlet angle is greater (e.g., more severe) than the calculated inlet angle, a larger torque is applied to the rotor 166. Additionally, in embodiments where the fluid inlet angle is smaller (e.g., less severe) than the calculated angle, the rotor 166 may slow down.
However, in other embodiments, the position profile may not correspond to the velocity profile, as represented by the line 292. For example, the position profile may illustrate movement of the dynamic fluid interface 210 while the velocity profile has a negative slope, indicative of a blocked outlet of the channel 190. Accordingly, the acceleration profile may be adjusted by returning to block 280.
While the embodiments described above included modifications to the end covers 184, 186, in certain embodiments the channels 190 may include geometric modifications to facilitate rotation of the rotor 166. For example, the channels 190 may include sloped and/or chamfered inlets to direct the fluid toward the interior surface 240 of the channels 190 to induce rotation of the rotor 166. Moreover, as described above, guide vanes may be distributed along the interior surface 240 of the channels 190 to facilitate rotation of the rotor 166. Accordingly, geometric modifications may be made to the rotor 166 to direct the fluid toward the interior surface 240 at an angle to apply a force to the interior surface 240 sufficient to facilitate rotation of the rotor 166 about the axis 188.
While the invention may be susceptible to various modifications and alternative forms, specific embodiments have been shown by way of example in the drawings and have been described in detail herein. However, it should be understood that the invention is not intended to be limited to the particular forms disclosed. Rather, the invention is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the invention as defined by the following appended claims.
This application is a non-provisional of U.S. Provisional Patent Application No. 62/088,413, entitled “INLET RAMPS FOR PRESSURE EXCHANGE DEVICES”, filed Dec. 5, 2014, which is herein incorporated by reference in its entirety.
Number | Date | Country | |
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62088413 | Dec 2014 | US |