EP0719945A1 - Enhanced mixing corrugated jet pump - Google Patents
Enhanced mixing corrugated jet pump Download PDFInfo
- Publication number
- EP0719945A1 EP0719945A1 EP95120233A EP95120233A EP0719945A1 EP 0719945 A1 EP0719945 A1 EP 0719945A1 EP 95120233 A EP95120233 A EP 95120233A EP 95120233 A EP95120233 A EP 95120233A EP 0719945 A1 EP0719945 A1 EP 0719945A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- jet pump
- corrugated
- mixing
- low
- ogive
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 239000012530 fluid Substances 0.000 claims abstract description 38
- 239000002131 composite material Substances 0.000 claims abstract description 7
- 230000001419 dependent effect Effects 0.000 claims description 5
- 230000002708 enhancing effect Effects 0.000 claims description 2
- 239000002648 laminated material Substances 0.000 claims 1
- 238000004519 manufacturing process Methods 0.000 abstract description 9
- 230000008901 benefit Effects 0.000 abstract description 6
- 230000001965 increasing effect Effects 0.000 abstract description 3
- 238000005086 pumping Methods 0.000 abstract description 2
- 239000000463 material Substances 0.000 description 4
- 239000000203 mixture Substances 0.000 description 3
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 125000004435 hydrogen atom Chemical class [H]* 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000005381 potential energy Methods 0.000 description 1
Images
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04F—PUMPING OF FLUID BY DIRECT CONTACT OF ANOTHER FLUID OR BY USING INERTIA OF FLUID TO BE PUMPED; SIPHONS
- F04F5/00—Jet pumps, i.e. devices in which flow is induced by pressure drop caused by velocity of another fluid flow
- F04F5/14—Jet pumps, i.e. devices in which flow is induced by pressure drop caused by velocity of another fluid flow the inducing fluid being elastic fluid
- F04F5/24—Jet pumps, i.e. devices in which flow is induced by pressure drop caused by velocity of another fluid flow the inducing fluid being elastic fluid displacing liquids, e.g. containing solids, or liquids and elastic fluids
Definitions
- the invention relates in general to the field of jet pump design. Specifically, the invention describes a jet pump design that utilizes a variable corrugated ogive to enhance fluid mixing and, therefore, the operational efficiency of the pump.
- jet pump technology is in combination (series) with a standard rotary pump where the available net positive suction head is low.
- a jet pump can be used to increase the pressure of a low pressure fluid to provide the necessary head for a standard (e.g., rotary) pump.
- a standard e.g., rotary
- jet pumps are used as "booster" pumps; they 'boost' the pressure of a low pressure fluid so that it may be pumped by a standard pump.
- a well known function of traditional jet pump technology is to transfer kinetic energy from a high-energy (high velocity, high pressure) fluid (HEF) to a low-energy (low velocity, low pressure) fluid (LEF).
- HEF high-energy
- LEF low-energy
- Energy transferred into the LEF is stored in the form of potential energy and results in an increase in the fluid's pressure.
- Energy transfer, and therefore jet pump efficiency, is enhanced by a thorough mixing of the low- and high-energy fluids.
- a jet pump utilizing said enhanced mixing apparatus is referred to as a corrugated jet pump.
- a corrugated jet pump incorporates a corrugated annular nozzle ogive that, during pumping operations, creates alternating low and high velocity zones in the ogive of the nozzle. These different velocity zones propagate shear planes that enhance the jet pumps downstream mixing. At the same time the core, or central portion, of the corrugated annular nozzle ring creates alternating vortices in the low- and high-energy fluids which also enhances mixing.
- the corrugated annular nozzle incorporates composite laminates for its fabrication. Advantages of the corrugated jet pump design include: (1) an overall reduction in boost pump length of as much as 75%, (2) a tremendous weight savings, and (3) significantly reduced production manufacturing costs.
- Figure 1 is a cross-sectional view of one embodiment of the invention.
- Figure 2 is an end-view of one embodiment of the invention.
- Figure 3 is a cut-away view of fluid mixing within one embodiment of a corrugated jet pump.
- Figure 4 is another cross-sectional view of an annular two-corrugation embodiment of the invention.
- cryogenic fluids e.g., liquid oxygen (LOX) or liquid hydrogen (H 2 ).
- LOX liquid oxygen
- H 2 liquid hydrogen
- high-energy fluid 90 is injected into a corrugated jet pump via a volute, or constant velocity manifold 100.
- Low-energy fluid 80 can be provided from a storage tank (not shown) and enters the corrugated jet pump at the main inlet 105. After the HEF is injected into the LEF's path, via an injection nozzle 110, the two fluids begin to mix after leaving the corrugated annular nozzle ogive 115.
- the velocity of the fluid in the corrugate's valley regions 120 is less than the velocity of the fluid in the corrugate's crown regions 125.
- These regions of differing velocity set up shear planes within the fluid (comprised of low- and high-energy fluids), thereby enhancing the jet pump's mixing action.
- the shear planes also generate vortices; two vortices per crown region. These vortices, or swirling actions, further enhance the jet pump's mixing action, as indicated by arrows 150.
- the nozzle ogive has a constant cross-sectional area. This is analogous to a piece of cardboard, no matter where you cut a flat piece of cardboard the inner structure is constant. That is, no matter where along a conventional ogive you look, its cross-sectional area is constant.
- the corrugated annular nozzle ogive of the invention exhibits a position dependent cross-sectional area. For instance, the magnitude of the valley-to-crown distance at cut 130 is less than the magnitude of the valley-to-crown distance at cut 135. Thus, the area of the nozzle's throat 140 is less than the area of the nozzle's exit 145.
- the invention's fluctuating geometry imparts differing velocities into the low and high energy fluids which creates shear planes and, thereby, improves the ability of a jet pump to mix the two fluids.
- Figure 3 is a straight embodiment for which numeric designators retain previous definitions. This embodiment uses two sets of corrugations 115. Efficient mixing is indicated by arrows 150.
- a jet pump in accordance with the invention may have two concentric rings of corrugated nozzles 115 that efficiently mix high 90 and low 80 energy fluids. As previously mentioned, this two-ring configuration can decrease the required length for efficient mixing, indicated by arrows 150 (Fig. 3), thus minimizing the size (length) and weight of the jet pump system.
- An exemplary jet pump in accordance with the invention has a discrete mass flow rate, ⁇ , ratio between the HEF ( ⁇ HEF ) and LEF ( ⁇ LEF ) which is dependent on the pressure differential between the two fluids and the required net positive suction head of the rotary pump for which the jet pump is a booster.
- the mass flow rates of the two fluids typically depend upon the required head of the rotary pump and the location where the HEF source is tapped off, i.e., where the HEF source is tapped off relative to the jet pump's injection nozzle 110.
- the mass flow rate and the pressure difference between the HEF and LEF define the fluid velocities of the two streams and dictate the cross-sectional areas of the nozzle jets 140 and the LEF suction (inlet) port 105.
- the aforementioned areas can utilize any variation of geometry's, e.g., circular or rectangular.
- the operational velocities of the HEF and LEF are, in part, determined by the pressure difference between the two fluids and can be determined by means of a hydrodynamic analysis which takes into account head and line loss and acceleration within the nozzle.
- the location and configuration of the corrugated nozzle jets is a variable and depends upon the allowable mixing length (usually between 0.5 and 1.5 inlet flow diameters) and the required pump performance.
- the circumferential spacing 200 (Fig. 2), the amplitude of the corrugates 205 and the throat to exit area ratio of the nozzle ( ⁇ ) is set to maximize mixing effectiveness.
- the relative spacing of the two nozzle rings is set to eliminate reverse flow in the center of the mixing region.
- the thickness of the corrugations is dependent on the pressure difference between the HEF and LEF, the throat to exit area ratio of the nozzle ( ⁇ ), the nozzle's attachment scheme and the material used to form the corrugated nozzle. Material selection depends on the type of fluids being pumped.
- a jet pump in accordance with the invention can be positioned as close as one-half of the flow diameter to the inlet of the rotary pump. As one of ordinary skill in the field would understand, the actual position is dependent upon the specific system requirements.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Jet Pumps And Other Pumps (AREA)
Abstract
An apparatus for increasing the mixing efficiency of low- and high-energy fluids within a jet pump is described. A jet pump utilizing said enhanced mixing apparatus is referred to as a corrugated jet pump. A corrugated jet pump incorporates a straight or an annular nozzle ring with a variable corrugated ogive that, during pumping operations, creates alternating low and high velocity zones in the ogive of the nozzle. These different velocity zones propagate shear planes that enhance the jet pump's downstream mixing. At the same time the core, or central portion, of the corrugated annular nozzle ring creates alternating vortices in the low- and high-energy fluids which also enhances mixing. The corrugated annular nozzle incorporates composite laminates for its fabrication. Advantages of the (composite laminate) corrugated jet pump design include: an reduction in boost pump length of as much as 75%, a weight savings, and significantly reduced production manufacturing costs.
Description
- The invention relates in general to the field of jet pump design. Specifically, the invention describes a jet pump design that utilizes a variable corrugated ogive to enhance fluid mixing and, therefore, the operational efficiency of the pump.
- A conventional use of jet pump technology is in combination (series) with a standard rotary pump where the available net positive suction head is low. In these situations a jet pump can be used to increase the pressure of a low pressure fluid to provide the necessary head for a standard (e.g., rotary) pump. Hence, often times jet pumps are used as "booster" pumps; they 'boost' the pressure of a low pressure fluid so that it may be pumped by a standard pump.
- In this role a well known function of traditional jet pump technology is to transfer kinetic energy from a high-energy (high velocity, high pressure) fluid (HEF) to a low-energy (low velocity, low pressure) fluid (LEF). Energy transferred into the LEF is stored in the form of potential energy and results in an increase in the fluid's pressure. Energy transfer, and therefore jet pump efficiency, is enhanced by a thorough mixing of the low- and high-energy fluids.
- One key operational problem with conventional jet pumps, which utilize standard de Laval nozzle jets, is their low efficiency due to poor mixing of the low- and high-energy fluids.
- An apparatus for increasing the mixing efficiency of low- and high-energy fluids within a jet pump is described. A jet pump utilizing said enhanced mixing apparatus is referred to as a corrugated jet pump.
- A corrugated jet pump incorporates a corrugated annular nozzle ogive that, during pumping operations, creates alternating low and high velocity zones in the ogive of the nozzle. These different velocity zones propagate shear planes that enhance the jet pumps downstream mixing. At the same time the core, or central portion, of the corrugated annular nozzle ring creates alternating vortices in the low- and high-energy fluids which also enhances mixing. The corrugated annular nozzle incorporates composite laminates for its fabrication. Advantages of the corrugated jet pump design include: (1) an overall reduction in boost pump length of as much as 75%, (2) a tremendous weight savings, and (3) significantly reduced production manufacturing costs.
- Figure 1 is a cross-sectional view of one embodiment of the invention.
- Figure 2 is an end-view of one embodiment of the invention.
- Figure 3 is a cut-away view of fluid mixing within one embodiment of a corrugated jet pump.
- Figure 4 is another cross-sectional view of an annular two-corrugation embodiment of the invention.
- One illustrative embodiment of the invention is described below as it might be implemented for a jet pump designed to pump cryogenic fluids, e.g., liquid oxygen (LOX) or liquid hydrogen (H2). In the interest of clarity, not all features of an actual implementation are described in this specification. It will of course be appreciated that in the development of any such actual implementation (as in any mechanical design) numerous implementation-specific decisions must be made to achieve the developers' specific goals and subgoals, such as compliance with system- and business-related constraints, which will vary from one implementation to another. Moreover, it will be appreciated that such a development effort might be complex and time-consuming, but would nevertheless be a routine undertaking of mechanical design engineering for those of ordinary skill having the benefit of this disclosure.
- In reference to Figures 1 and 2, high-
energy fluid 90 is injected into a corrugated jet pump via a volute, orconstant velocity manifold 100. Low-energy fluid 80 can be provided from a storage tank (not shown) and enters the corrugated jet pump at themain inlet 105. After the HEF is injected into the LEF's path, via an injection nozzle 110, the two fluids begin to mix after leaving the corrugatedannular nozzle ogive 115. - As the low- and high-energy fluids mix within the corrugated
annular nozzle ogive 115, the velocity of the fluid in the corrugate'svalley regions 120 is less than the velocity of the fluid in the corrugate'scrown regions 125. These regions of differing velocity set up shear planes within the fluid (comprised of low- and high-energy fluids), thereby enhancing the jet pump's mixing action. The shear planes also generate vortices; two vortices per crown region. These vortices, or swirling actions, further enhance the jet pump's mixing action, as indicated byarrows 150. - In a conventional jet pump the nozzle ogive has a constant cross-sectional area. This is analogous to a piece of cardboard, no matter where you cut a flat piece of cardboard the inner structure is constant. That is, no matter where along a conventional ogive you look, its cross-sectional area is constant. The corrugated annular nozzle ogive of the invention, however, exhibits a position dependent cross-sectional area. For instance, the magnitude of the valley-to-crown distance at
cut 130 is less than the magnitude of the valley-to-crown distance atcut 135. Thus, the area of the nozzle'sthroat 140 is less than the area of the nozzle'sexit 145. The invention's fluctuating geometry imparts differing velocities into the low and high energy fluids which creates shear planes and, thereby, improves the ability of a jet pump to mix the two fluids. - Many conventional jet pump designs have length-to-diameter ratios of approximately 7:1. These large values (implying long jets, relative to their diameter) are necessary to ensure that the low- and high-energy fluids have sufficient time to thoroughly mix. Thus, length-to-diameter ratios are one indication of a jet pump's mixing efficiency. Using a corrugated annular nozzle ogive, as shown in Figures 1, 2 and 4, a jet pump's length-to-diameter ratio can be brought down to between 1:1 or 1.5:1 - indicating a significant improvement in the jet pump's mixing efficiency. A shorter pump also consumes less material in its manufacture, making a corrugated jet pump less costly and lighter than a conventional jet pump.
- Figure 3 is a straight embodiment for which numeric designators retain previous definitions. This embodiment uses two sets of
corrugations 115. Efficient mixing is indicated byarrows 150. - As shown in cross-section in Figure 4, a jet pump in accordance with the invention may have two concentric rings of
corrugated nozzles 115 that efficiently mix high 90 and low 80 energy fluids. As previously mentioned, this two-ring configuration can decrease the required length for efficient mixing, indicated by arrows 150 (Fig. 3), thus minimizing the size (length) and weight of the jet pump system. - An exemplary jet pump in accordance with the invention has a discrete mass flow rate, ẇ, ratio between the HEF (ẇ HEF ) and LEF (ẇ LEF ) which is dependent on the pressure differential between the two fluids and the required net positive suction head of the rotary pump for which the jet pump is a booster. The mass flow rates of the two fluids typically depend upon the required head of the rotary pump and the location where the HEF source is tapped off, i.e., where the HEF source is tapped off relative to the jet pump's injection nozzle 110.
- The mass flow rate and the pressure difference between the HEF and LEF define the fluid velocities of the two streams and dictate the cross-sectional areas of the
nozzle jets 140 and the LEF suction (inlet)port 105. The aforementioned areas can utilize any variation of geometry's, e.g., circular or rectangular. The area of the nozzle's throat 140 (A throat ) is equal to the mass flow rate of the HEF divided by the product of the HEF's velocity (v HEF ) and its density (ρ HEF ): - The operational velocities of the HEF and LEF are, in part, determined by the pressure difference between the two fluids and can be determined by means of a hydrodynamic analysis which takes into account head and line loss and acceleration within the nozzle. The location and configuration of the corrugated nozzle jets is a variable and depends upon the allowable mixing length (usually between 0.5 and 1.5 inlet flow diameters) and the required pump performance.
- The circumferential spacing 200 (Fig. 2), the amplitude of the
corrugates 205 and the throat to exit area ratio of the nozzle (ε) is set to maximize mixing effectiveness. The relative spacing of the two nozzle rings is set to eliminate reverse flow in the center of the mixing region. - The thickness of the corrugations is dependent on the pressure difference between the HEF and LEF, the throat to exit area ratio of the nozzle (ε), the nozzle's attachment scheme and the material used to form the corrugated nozzle. Material selection depends on the type of fluids being pumped.
- It has been found that a jet pump in accordance with the invention can be positioned as close as one-half of the flow diameter to the inlet of the rotary pump. As one of ordinary skill in the field would understand, the actual position is dependent upon the specific system requirements.
- In summary, some of the design parameters that affect the construction of the invention's corrugate apparatus include:
- 1. Pressure differential between low- and high-energy fluids.
- 2. Pressure of incoming high-energy fluid.
- 3. Discharge pressure of mixed fluid.
- 4. Mass flow rate of the low-and high-energy fluids (the larger the jet pump's total mass flow rate, the larger the jet pump and, therefore, the larger the corrugated annular nozzle).
- 5. Type/temperature of the fluid being pumped (the temperature of the fluids being pumped determine the materials of choice for the composite laminates of the corrugated annular nozzle).
- Some advantages of the composite laminate corrugated jet pump design include:
- 1. An overall reduction in boost pump length of as much as 75%.
- 2. The low density of the composite laminate corrugated surface, and the reduction in length made possible by the increased mixing efficiency of a corrugated jet pump design, reduce weight.
- 3. Significantly reduced production manufacturing costs.
- It will be appreciated by those of ordinary skill having the benefit of this disclosure that numerous variations from the foregoing illustration will be possible without departing from the inventive concept described herein. Accordingly, it is the claims set forth below, and not merely the foregoing illustration, which are intended to define the exclusive rights claimed in this application program.
Claims (3)
- An apparatus for enhancing fluid mixing in a jet pump comprising a corrugated annular nozzle ogive, said corrugated nozzle ogive having a position dependent cross-sectional area.
- A jet pump comprising a corrugated nozzle ogive of claim 1, which nozzle is annular.
- The jet pump of claim 2 wherein the corrugated annular nozzle ogive comprises composite laminate materials.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US36538694A | 1994-12-28 | 1994-12-28 | |
US365386 | 1994-12-28 |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0719945A1 true EP0719945A1 (en) | 1996-07-03 |
Family
ID=23438689
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP95120233A Withdrawn EP0719945A1 (en) | 1994-12-28 | 1995-12-20 | Enhanced mixing corrugated jet pump |
Country Status (2)
Country | Link |
---|---|
EP (1) | EP0719945A1 (en) |
JP (1) | JPH08232899A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2161273C1 (en) * | 1999-05-12 | 2000-12-27 | Волгоградский государственный технический университет | Jet-type pump |
US20100316493A1 (en) * | 2007-03-23 | 2010-12-16 | Flodesign Wind Turbine Corporation | Turbine with mixers and ejectors |
US20110002781A1 (en) * | 2007-03-23 | 2011-01-06 | Flodesign Wind Turbine Corporation | Wind turbine with pressure profile and method of making same |
US20110058937A1 (en) * | 2007-03-23 | 2011-03-10 | Flodesign Wind Turbine Corporation | Nacelle configurations for a shrouded wind turbine |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
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JP4844236B2 (en) * | 2005-12-20 | 2011-12-28 | ソニー株式会社 | NOZZLE, JET GENERATOR, COOLING DEVICE, AND ELECTRONIC DEVICE |
JP2016200088A (en) * | 2015-04-13 | 2016-12-01 | 三菱重工メカトロシステムズ株式会社 | Ejector, and high-altitude combustion test exhaust equipment having the ejector |
JP6543809B2 (en) * | 2015-12-22 | 2019-07-17 | パナソニックIpマネジメント株式会社 | Air blower |
JP2023008630A (en) * | 2021-07-06 | 2023-01-19 | アルテミラ製缶株式会社 | Liquid amplification device |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
SU449177A1 (en) * | 1969-12-31 | 1974-11-05 | Одесский Ордена Трудового Красного Знамени Государственный Университет Им.И.И.Мечникова | Jet pump |
DE3239197A1 (en) * | 1981-11-03 | 1983-05-11 | Rolls-Royce Ltd., London | INFRARED RADIATION SUPPRESSION DEVICE FOR A GAS TURBINE ENGINE |
GB2260369A (en) * | 1991-08-30 | 1993-04-14 | United Technologies Corp | Jet propulsion system having ejector shroud |
-
1995
- 1995-12-20 EP EP95120233A patent/EP0719945A1/en not_active Withdrawn
- 1995-12-22 JP JP33521295A patent/JPH08232899A/en active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
SU449177A1 (en) * | 1969-12-31 | 1974-11-05 | Одесский Ордена Трудового Красного Знамени Государственный Университет Им.И.И.Мечникова | Jet pump |
DE3239197A1 (en) * | 1981-11-03 | 1983-05-11 | Rolls-Royce Ltd., London | INFRARED RADIATION SUPPRESSION DEVICE FOR A GAS TURBINE ENGINE |
GB2114229A (en) * | 1981-11-03 | 1983-08-17 | Rolls Royce | Gas turbine engine infra-red radiation suppressor |
GB2260369A (en) * | 1991-08-30 | 1993-04-14 | United Technologies Corp | Jet propulsion system having ejector shroud |
Non-Patent Citations (1)
Title |
---|
DATABASE WPI Section PQ Week 7634, Derwent World Patents Index; Class Q56, AN 76-h5247x, XP002001865 * |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2161273C1 (en) * | 1999-05-12 | 2000-12-27 | Волгоградский государственный технический университет | Jet-type pump |
US20100316493A1 (en) * | 2007-03-23 | 2010-12-16 | Flodesign Wind Turbine Corporation | Turbine with mixers and ejectors |
US20110002781A1 (en) * | 2007-03-23 | 2011-01-06 | Flodesign Wind Turbine Corporation | Wind turbine with pressure profile and method of making same |
US20110058937A1 (en) * | 2007-03-23 | 2011-03-10 | Flodesign Wind Turbine Corporation | Nacelle configurations for a shrouded wind turbine |
US8657572B2 (en) * | 2007-03-23 | 2014-02-25 | Flodesign Wind Turbine Corp. | Nacelle configurations for a shrouded wind turbine |
Also Published As
Publication number | Publication date |
---|---|
JPH08232899A (en) | 1996-09-10 |
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