US20100139292A1 - Temperature adjustable airflow device - Google Patents
Temperature adjustable airflow device Download PDFInfo
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- US20100139292A1 US20100139292A1 US12/345,110 US34511008A US2010139292A1 US 20100139292 A1 US20100139292 A1 US 20100139292A1 US 34511008 A US34511008 A US 34511008A US 2010139292 A1 US2010139292 A1 US 2010139292A1
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- gas
- high pressure
- vortex tube
- mixing chamber
- cooled
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B9/00—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point
- F25B9/02—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point using Joule-Thompson effect; using vortex effect
- F25B9/04—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point using Joule-Thompson effect; using vortex effect using vortex effect
Definitions
- This invention generally relates to vortex tubes and, more specifically, to a modified temperature adjustable airflow device.
- Vortex tubes known since the 1930s, are mechanical devices that convert gas tinder pressure into hot and cold gas streams. It has no moving parts.
- a typical vortex tube has two openings, one at each end and an intermediate inlet tube for introducing gas under a high pressure into a spiral flow path. While there are different explanations for the way in which vortex tubes work, it is known that when a gas is introduced under high pressure, it is separated into two different streams, a first gas stream exiting one end of the tube being heated air while the gas stream exiting the other end is cooled air. The gases that exit at two opposing ends of the tube being heated and cooled gas streams, are at lower pressures that the pressure of the inlet gas. While vortex tubes are not an efficient as traditional air-conditioning equipment, they are commonly used for inexpensive sport cooling, when compressed air is available. Commercial models, for example, are designed for industrial applications to produce temperature drops of approximately 45° C. (80° F.) from the temperature of the high pressure gas.
- U.S. Pat. No. 3,208,229 discloses a vortex tube, wherein it is proposed that the inner surface of the tube be roughened to produce turbulence and mixing of the gases that reduce the efficiency of the tube. Furthermore, a control ring is used in conjunction with the blades at the far end of the heated tube to enable the tube to be shortened without loss of efficiency.
- a ventilated suit refrigeration unit in which the heated and cooled streams of gas emanating from the vortex tube are mixed by two air flow regulated valves 44 , 45 interconnected through a rod 51 that may be regulated by a thermostat 58 .
- a non-freeze enhancement for a vortex tube in which the hot air flow is permitted to heat the vortex tubes inlet at a cross-section and diaphragm and warm the vortex cold fraction in its discharge pass that result in increasing the unit's performance reliability.
- a line 34 connects the heated end 20 of the vortex tube to the heat exchanger at the cooled side.
- the inlet air flow on the pressure, at 40 is not diverted to either side of the vortex tube.
- the present invention utilizes a relative conventional vortex tube that has two opposing ends one of which releases cooled gas while the other produces heated gas relative to an ambient temperature of a high pressure gas that input into the vortex device.
- the one of the two vortex tubes that releases the cooled gas is tapped into a mixing chamber that has a gas mixing compartment.
- a bypass tube connects the high pressure tube that feeds the vortex tube to the mixing compartment of the mixing chamber, an adjustable valve being placed within the bypass tube to allow gas flowing within the bypass tube to be freely transmitted or partially blocked or fully blocked.
- the high pressure gas that is fed by the bypass tube and the cooled gas that is output of the vortex tube are mixed within the mixing chamber and fed to the outlet of the mixing chamber.
- the mixed gas will achieve a temperature that is between the ambient temperature of the high pressure gas and the temperature of the cooled gas exiting the vortex tube. This matter, the temperature at the outlet of the mixing chamber can be adjusted while maintaining a relatively high pressure or flow speed of the temperature modified gas.
- a temperature feedback loop is provided for pre-cooling the high pressure gas being fed into the vortex tube so that the temperature of the cooled air is lower than the temperature that would normally be obtainable by using a conventional vortex tube. This is achieved, for example, by means of a pre-cooling chamber that is cooled by the cold air exiting the vortex tube for cooling the high pressure input gas into a vortex tube.
- FIG. 1 is a schematic representation of a temperature adjustable airflow device in accordance with the present invention, shown partially exploded to indicate the manner in which the device is assembled;
- FIG. 2 is a schematic representation of a temperature adjustable airflow device that includes a pre-cooling chamber as part of a temperature feedback loop for using the cold air from the vortex tube to pre-cool the high pressure gas entering into the vortex tube.
- FIG. 3 is a heat flow diagram representing the heat transfers in the embodiment illustrated in FIG. 2 ;
- FIG. 4 is a time temperature chart illustrating the incremental drop in temperature outlet for the embodiment illustrated in FIG. 2 .
- a temperature adjustable airflow device in accordance with the invention is generally designated by the reference numeral 10 .
- the device 10 includes a vortex tube 12 having a cold end outlet 12 a, a hot end outlet 12 b, and a spiral chamber 12 c.
- the internal construction of the vortex tube is conventional and the details need not to be described. All of the patents that mentioned in the background of the invention are incorporated herein for the teachings of the details of the vortex tubes, and any such construction can be used. The specific construction or details of the vortex tube are not critical and the subject invention may be used with any conventional or modified vortex tube of the type well known to those skilled in the art.
- the vortex tube 12 has at each of the ends 12 a and 12 b internal threads 14 .
- a cold air pipe 16 is provided with an external tread 16 a at one end and an external tread 16 b at the other end, the external treads being dimensioned and configured to threadably mesh with the internal treads 14 of the vortex tube, effectively enlarging or extending the ends of the vortex tube. Whether the vortex tube has an adequate length along direction A V the extension tube 16 may not be required.
- the hot pipe 18 that likewise has external treads 18 a shown at the end that meshes with the vortex tube.
- a high pressure inlet pipe 20 is in fluid-flow communication with the interior of the vortex tube and the chamber 12 c.
- the details of the chamber 12 c are not shown as these are well known to those skilled in the art.
- the high pressure inlet pipe 20 has an outlet 20 a that is joined to the vortex tube 12 , or may be integrally formed therewith.
- the high pressure inlet pipe 20 also has an inlet 20 b that can be connected to a source of high pressure gas in any conventional manner.
- a bypass tube 24 has a first tube section 24 a in fluid flow communication with the high pressure inlet pipe 20 and a tube portion 24 b fluid flow communication with the mixing chamber 22 .
- An additional tube portion 24 c may be provided that aligns the outlet end of the bypass tube with an axis A C of the mixing chamber 22 although, clearly, the two portions 24 b and 24 c are shown as an integral bent tube portion.
- Another feature of the invention is the provision of a adjustable valve 26 between the two portions 24 a and 24 b that can be adjusted from the fully open position, in which case the gas in the tube portion 24 a may flow freely into the tube portion 24 b, or may be partially or fully closed to block, wholly or partially, the flow of gas between the portions 24 a and 24 b.
- a pressure gauge 28 is advantageously provided that is connected to the adjustable valve 26 or to one of the two portions 24 a, 24 b by means of a tube 30 to provide an indication of the level of pressure in the bypass tube 24 .
- tube 24 is shown as a bypass tube connected to the same supply of high pressure gas supplying the inlet pipe 20 , it is also possible, and contemplated by the invention, that two separate entries of high pressure are provided, each separately supplying high pressure to the inlet pipe 20 and to the tube 24 , which would no longer be a bypass tube as shown in FIGS. 1 and 2 .
- a mixing compartment shown as being generally elongated along the chamber axis A C .
- the cold pipe 16 and specifically its external tread and the remote end 16 b are dimensioned to mesh with internal threads at the cold gas inlet opening 22 b. All of the threaded connections are preferably sealed in any conventional manner to prevent the escape of gas through these joints. In this connection, it is also possible to attach the various tubes and pipes shown and discussed above by means other than treated connections. Thus, these tubes may be attached to each other by the conventional means such as welding, adhesive, etc.
- the gas that feeds the mixing chamber 22 by means of the bypass tube 24 is designated by the reference numeral 34 , this being high pressure gas that is at ambient temperature.
- the cold pipe 16 injects a cold stream of gas 36 into the mixing compartment 32 , at a point intermediate the outlet end of the tube portion 22 c and the outlet tube 38 of the mixing chamber 22 .
- the specific configuration of the mixing chamber 22 is not critical, although it is preferable that the end of the cold pipe 16 at 16 b be positioned or is located closer to the outlet opening 22 c than is the tube portion 24 c.
- the mixing chamber 22 is in the form of cylindrical hollow tubular member that is sealed or closed with the exceptions of openings described.
- the mixing chamber has an axial length “1” along the axis A C and has a diameter “d”.
- the cold and hot pipes 16 , 18 are shown aligned with the vortex tube 12 axis A V , and the axes A C and A V are preferably relative to each other inclined at an angle ⁇ as shown.
- the angle ⁇ is 45° in the present preferred embodiment, although this angle may be varied considerably, with different degrees of advantage. It is also preferred that the cold air stream 36 be injected at a distance approximately 1.5-2 inches from the outlet to 38 . This distance can, also, be modified slightly with different degrees of advantage. The angle of 45° is generally preferred and provides improved results.
- the high pressure air stream 34 generally enters along the axis A C shown
- the lower pressure cold air stream 36 as injected at angle of 45° relative to the high pressure stream 34 the gas is being mixed within the mixing chamber and exit as a stream 40 that may be at higher pressure than the pressure of the stream 36 but it has been elevated temperature somewhat depending on the adjustment of the valve 26 , between the temperatures of the ambient and cold streams 34 , 36 respectively.
- FIG. 3 another present preferred embodiment of the invention is illustrated that is generally is designated by the reference numeral 10 ′.
- the difference between the device illustrated in FIG. 2 and the one illustrated in FIG. 1 is that the device illustrated in FIG. 2 includes a temperature amplification device, utilizing a feedback loop, that is used for a lower temperature of the usable out-stream of gas.
- a pre-cooler housing 42 is provided that may be made of plastic or other temperature insulating or heat-flow resistant material.
- the pre-cooler housing 42 has an inlet opening 42 a and an outlet opening 42 b, shown at opposing or opposite sides of the housing.
- a pair of opposing openings 42 c and 42 d are provided that are arranged along a direction generally transverse to the direction of the openings 42 a, 42 b shown.
- the pre-cooling housing 42 has an internal chamber, cavity or compartment 42 e that serves as a heat exchange chamber, as it will become more evident from the discussion that follows.
- the mixer 22 is connected, at its inlet end with a bypass tube 24 b, 24 c that is coupled to the valve 26 .
- the valve 26 can be used to adjust the pressure and, therefore, the gas flow velocity from the inlet to the mixer chamber 22 .
- the cold air inlet tube 16 transfers the cooled air 36 from the cooled air end 12 a of the vortex tube 12 as previously described.
- the high pressure gas 34 is mixed with the cooled air 36 and the mixed gas is channeled by means of pipe portions 38 a - 38 e to the inlet opening 42 c of the cooling chamber.
- the high pressure inlet tube 20 is now formed of spaced sections 20 x and 20 y that are aligned but spaced from each other along an axis of the high pressure inlet pipe.
- the inlet pipe portion 20 x has a threaded end 20 x ′ that is connected, such as by bushing 46 , to a heat exchange tube or pipe 48 that has opposing threaded ends 48 a and 48 b that are respectively attached to the bushing 46 , at one end, and a coupling 50 that joins the threaded end 48 as well as a threaded end 21 ′ of the pipe portion 20 y. It will be clear, therefore, that the high pressure gas entering the pipe portion 20 x passes through the heat exchange pipe 48 and into the vortex tube 12 by means of a pipe or tube portion 20 y.
- the gas in the pipes or tubes 38 a - 38 e emanates from the mixing chamber 22 and is directed into the compartment or chamber 42 e and exits as the cooled gas stream 40 .
- the cooled air stream fills the chamber or compartment 42 e, it absorbs some of the heat from the heat exchanger pipe or tube 48 , as it passes through the pre-cooler 42 , and ultimately is outputted for use in cooling objects.
- the heat exchanger 48 therefore, becomes cooler in time, and high pressure gas that passes through pipe or tube portions 20 x, 20 y through the pre-cooling chamber 42 is likewise cooled by the removal of heat.
- the high pressure gas P enters the tube portion 20 x and is guided through the heat exchanger tube 48 and through the tube portion 20 y into the vortex tube 12 .
- the cooled air stream 36 exiting from the cooled air outlet end 12 a of the vortex tube is mixed with high pressure gas 34 in the mixing chamber 22 , as previously described.
- the gas stream 38 that exits the mixing chamber 22 tends to be at a temperature between of temperature of the high pressure gas and the cooled air stream.
- the mixing chamber 22 therefore, elevates the temperature of the cooled air stream 36 , although that stream is now at a higher pressure.
- the cooled air stream that enters the pre-cooling chamber 42 lowers the temperature within that chamber and there is a transfer of heat due to the cooling effect of the heat exchanger tube 48 .
- high pressure has P passing through the heat exchanger tube 48 is pre-cooled before it enters the vortex tube 12 at the high pressure input pipe portion 20 y.
- Such pre-cooled gas is then further cooled by the vortex tube 12 and this results in further cooling at the outlet of the mixing chamber 22 , and additional cooling of the heat exchanger tube 48 .
- Such a feedback-type arrangement continues to increasingly cool the heat exchanger tube 48 thereby resulting in a continued drop in temperature of the input gas pressure stream P prior to entry into the vortex tube 12 .
- the pre-cooling chamber 48 is, therefore, in the nature of an amplification device and it amplifies the cooling effect of the cooled output gas outputted by the vortex tube 12 and the gas exiting the mixing chamber 22 . This continues until an equilibrium is reached when the drop in the temperature in the pre-cooling chamber is such that decreases in temperature are compensated or offset by increases in heat transfer from the ambient atmosphere.
- the inlet air at high pressure enters at heat level Q 1 .
- the pre-cooling chamber 42 is at ambient and there are no change in temperature as the high pressure gas passes through the heat exchange or transfer tube 48 .
- the heat transfer tube 48 cools off and there is a change in heat ⁇ Q 1 as the high pressure gas passes though the heat exchanger tube 48 .
- the gas passing through the heat exchanger tube 48 is modified, therefore, by a change in heat ⁇ Q 1 as it enters the vortex tube 12 .
- the air in the vortex tube is further modified at the heated end by a decrease of heat ⁇ Q 2 at one end and an increase in heat at the other end at + ⁇ Q 3 .
- the outlet of the vortex tube 12 is at a heat level Q 4 as it enters the mixing chamber 22 where the heat level is increased by + ⁇ Q 4 , due to the addition of and mixing with the high pressure gas at ambient emanating directly from the high pressure side.
- the heat level Q 5 at the inlet to the heat exchanger 48 may experience slight rise in heat removed from the ambient high pressure gas at Q 1 . However, because the flow of Q 5 is relatively high through the pre-cooling chamber 48 the heat level Q 6 is approximately equal to Q 5 .
- a transition is shown between the temperature T of the stream 40 over time after the device is activated.
- the temperature is at T 1 .
- the cooled air 36 from the vortex tube 12 circulates through the mixing chamber 22 and the pre-cooling chamber 42 , there is a gradual drop in the temperature of the heat exchanger tube 48 and the amount of heat exchange results in a drop in temperature of the gas exiting the pre-cooling chamber 48 into the input pipe portion 20 y of the vortex tube.
- the drop of temperature continues until time t 2 when the temperature has dropped to T 2 , where the temperature remains as long as the device operation is maintained.
- the temperature does not drop below T 2 because a equilibrium state is reached between the amount of heat removed from the flowing gases and the amount of heat that is transferred to the device from the ambient atmosphere.
- the greater the differential in the temperatures between the temperature T 2 and the ambient the greater the heat added from the ambient atmosphere and that is the reason why a steady state condition is reached in time.
- FIG. 3 it will be clear that the differences in heat levels between the embodiments shown in FIG. 2 is ⁇ Q 1 imparted by the pre-cooling chamber 48 .
- the greater the efficiency of the pre-cooling chamber therefore, the greater the quantity ⁇ Q 1 and the greater the temperature drop in the outlet stream of cooled air 40 . Constructions to optimize the efficiency of the heat exchanger 42 , 48 are well known to those skilled in the art.
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Abstract
A temperature adjustable airflow device includes a vortex tube having a high pressure gas inlet and cooled and heated outlets. A mixing chamber is provided having first and second ends, one gas inlet end at the first end and a gas outlet end at the second end, and an intermediate gas inlet end between the first and second ends. A high pressure inlet conduit is connected to the high pressure gas inlet of the vortex tube and to the gas inlet of the mixing chamber. The cooled or the heated vortex tube outlet is connected to the intermediate gas inlet end, the mixing chamber mixing high pressure gas with cooled or heated gas, respectively, from the vortex tube to enhance the pressure of the cooled or heated gas emanating from the vortex tube. The arrangement allows cooled or heated gas from the vortex tube to be output for a given application at a higher pressure that would normally be available.
Description
- 1. Field of the Invention
- This invention generally relates to vortex tubes and, more specifically, to a modified temperature adjustable airflow device.
- 2. Description of the Prior Art
- Vortex tubes, known since the 1930s, are mechanical devices that convert gas tinder pressure into hot and cold gas streams. It has no moving parts.
- Generally, a typical vortex tube has two openings, one at each end and an intermediate inlet tube for introducing gas under a high pressure into a spiral flow path. While there are different explanations for the way in which vortex tubes work, it is known that when a gas is introduced under high pressure, it is separated into two different streams, a first gas stream exiting one end of the tube being heated air while the gas stream exiting the other end is cooled air. The gases that exit at two opposing ends of the tube being heated and cooled gas streams, are at lower pressures that the pressure of the inlet gas. While vortex tubes are not an efficient as traditional air-conditioning equipment, they are commonly used for inexpensive sport cooling, when compressed air is available. Commercial models, for example, are designed for industrial applications to produce temperature drops of approximately 45° C. (80° F.) from the temperature of the high pressure gas.
- In some instances, it may be preferable to modify the output of the cold air stream exiting, at one end of the vortex tube, by either increasing its pressure or increasing its temperature somewhat. This has been done in the past by adjusting a stopcock within the heated end of the tube that regulates the extent of flow through the heated end. However, because the air exiting this tube can be hot, this is a disadvantage and make cause injury to a user. Also, while such and adjustment at the hot end of the tube may raise the temperature of the gas at the cooled end of the tube, it is not always practical to use this approach to increase the pressure of the cold air exiting the tube.
- As indicated, while has been conventional in the prior art to control the temperature of the discharged cold stream by providing a valve at the hot discharge end of the vortex tube, not only is such placement of a valve at the hot end of the tube inconvenient and potentially dangerous to the user who may be exposed to elevated temperatures, but the closing of the valve necessarily increases the volume of the cold discharge stream. As disclosed in U.S. Pat. No. 3,192,728 such an approach will function to a limited extent. However, this approach will tend to decrease the efficiency of the unit as the valve decreases the volume of the stream to counteract the decrease in the temperature of the stream.
- In U.S. Pat. No. 4,240,261 a temperature-adjustable vortex tube assembly is disclosed. However, this assembly includes a complicated mechanism for mixing the hot and cold discharge streams in an attempt to obtain a desired temperature while maintaining the flow volume of the mixture constant. The device is expensive to fabricate and the efficiency of the unit is reduced because of the manner in which the discharged streams flow in parallel to a common end of the device necessarily resulting in temperature interchanges between the hot and cold streams along such parallel flow paths.
- U.S. Pat. No. 3,208,229 discloses a vortex tube, wherein it is proposed that the inner surface of the tube be roughened to produce turbulence and mixing of the gases that reduce the efficiency of the tube. Furthermore, a control ring is used in conjunction with the blades at the far end of the heated tube to enable the tube to be shortened without loss of efficiency.
- In U.S. Pat. No. 4,339,926 a vortex tube is disclosed that seeks to overcome the disadvantages of prior art vortex tubes. The patent seeks to provide a more simple and inexpensive vortex tube that has a relatively short length relative to the diameter of the tube while still maintaining the optimum temperature differentials at the end of the tubes but without the use of blades or control rings as described in prior references.
- In U.S. Pat. No. 2,819,590 a ventilated suit refrigeration unit is disclosed in which the heated and cooled streams of gas emanating from the vortex tube are mixed by two air flow regulated
valves 44, 45 interconnected through a rod 51 that may be regulated by a thermostat 58. - In U.S. Pat. No. 6,289,679 a non-freeze enhancement for a vortex tube is disclosed in which the hot air flow is permitted to heat the vortex tubes inlet at a cross-section and diaphragm and warm the vortex cold fraction in its discharge pass that result in increasing the unit's performance reliability. As will be noted, for example, from
FIG. 1 aline 34 connects theheated end 20 of the vortex tube to the heat exchanger at the cooled side. However, the inlet air flow on the pressure, at 40 is not diverted to either side of the vortex tube. - In order to overcome the above disadvantages inherent in prior art devices, it is an object of the invention to provide a temperature adjustable airflow device that overcomes the inherent disadvantages of such prior know devices.
- It is another object of the invention to provide a temperature adjustable airflow device that is simple construction and economical to the manufactures.
- It is still another object of the invention to provide a temperature adjustable airflow device that utilizes a vortex tube and is easy and safe to use to adjust the temperature of the gas output of the device.
- It is still another object of the invention to provide a temperature adjustable airflow device as in a previous object that provides accurate control of the temperature of the outlet gas of the vortex tube.
- It is still another object of the invention to provide a temperature adjustable airflow device as in a previous object that allows the adjustment of the temperature of the output gas without unduly reducing the efficiency of the device.
- It is still another object of the invention to provide a temperature adjustable airflow device of the type of the discussion that includes a temperature feedback loop for pre-cooling high pressure gas prior to entry into a vortex tube.
- It is yet another object of the invention to provide temperature adjustable airflow device as in the previous object that provides a temperature adjustable airflow device that provides an air stream colder than the stream of cold gas typically available at the output of a vortex tube, and at a higher pressure, by providing a pre-cooling chamber that is cooled by the colder gas exiting the vortex tube that pre-cools the gas in the high pressure input line prior to entry into the high pressure inlet of the vortex tube.
- In order to achieve the above objects the present invention utilizes a relative conventional vortex tube that has two opposing ends one of which releases cooled gas while the other produces heated gas relative to an ambient temperature of a high pressure gas that input into the vortex device. The one of the two vortex tubes that releases the cooled gas is tapped into a mixing chamber that has a gas mixing compartment. A bypass tube connects the high pressure tube that feeds the vortex tube to the mixing compartment of the mixing chamber, an adjustable valve being placed within the bypass tube to allow gas flowing within the bypass tube to be freely transmitted or partially blocked or fully blocked. The high pressure gas that is fed by the bypass tube and the cooled gas that is output of the vortex tube are mixed within the mixing chamber and fed to the outlet of the mixing chamber. The mixed gas will achieve a temperature that is between the ambient temperature of the high pressure gas and the temperature of the cooled gas exiting the vortex tube. This matter, the temperature at the outlet of the mixing chamber can be adjusted while maintaining a relatively high pressure or flow speed of the temperature modified gas.
- In accordance with one presently preferred embodiment, a temperature feedback loop is provided for pre-cooling the high pressure gas being fed into the vortex tube so that the temperature of the cooled air is lower than the temperature that would normally be obtainable by using a conventional vortex tube. This is achieved, for example, by means of a pre-cooling chamber that is cooled by the cold air exiting the vortex tube for cooling the high pressure input gas into a vortex tube.
- With the above additional objects and advantages in view, as will hereinafter appear, this invention comprises the devices, combinations and arrangements of parts hereinafter described by way of example, and illustrated in the accompanying drawings of presently preferred embodiments, in which:
-
FIG. 1 is a schematic representation of a temperature adjustable airflow device in accordance with the present invention, shown partially exploded to indicate the manner in which the device is assembled; and -
FIG. 2 is a schematic representation of a temperature adjustable airflow device that includes a pre-cooling chamber as part of a temperature feedback loop for using the cold air from the vortex tube to pre-cool the high pressure gas entering into the vortex tube. -
FIG. 3 is a heat flow diagram representing the heat transfers in the embodiment illustrated inFIG. 2 ; and -
FIG. 4 is a time temperature chart illustrating the incremental drop in temperature outlet for the embodiment illustrated inFIG. 2 . - Referring specifically to the single Figure, a temperature adjustable airflow device in accordance with the invention is generally designated by the
reference numeral 10. - The
device 10 includes avortex tube 12 having acold end outlet 12 a, ahot end outlet 12 b, and aspiral chamber 12 c. The internal construction of the vortex tube is conventional and the details need not to be described. All of the patents that mentioned in the background of the invention are incorporated herein for the teachings of the details of the vortex tubes, and any such construction can be used. The specific construction or details of the vortex tube are not critical and the subject invention may be used with any conventional or modified vortex tube of the type well known to those skilled in the art. - The
vortex tube 12 has at each of theends internal threads 14. Acold air pipe 16 is provided with anexternal tread 16 a at one end and anexternal tread 16 b at the other end, the external treads being dimensioned and configured to threadably mesh with theinternal treads 14 of the vortex tube, effectively enlarging or extending the ends of the vortex tube. Whether the vortex tube has an adequate length along direction AV theextension tube 16 may not be required. The same is true of thehot pipe 18 that likewise has external treads 18 a shown at the end that meshes with the vortex tube. - As with the conventional vortex tubes, a high
pressure inlet pipe 20 is in fluid-flow communication with the interior of the vortex tube and thechamber 12 c. The details of thechamber 12 c are not shown as these are well known to those skilled in the art. The highpressure inlet pipe 20 has an outlet 20 a that is joined to thevortex tube 12, or may be integrally formed therewith. The highpressure inlet pipe 20 also has aninlet 20 b that can be connected to a source of high pressure gas in any conventional manner. - One feature of the invention is the provision of a mixing
chamber 22 that has a high pressure inlet opening 22 a, a coldinlet gas opening 22 b and anoutlet opening 22 c. Abypass tube 24 has afirst tube section 24 a in fluid flow communication with the highpressure inlet pipe 20 and atube portion 24 b fluid flow communication with the mixingchamber 22. Anadditional tube portion 24 c may be provided that aligns the outlet end of the bypass tube with an axis AC of the mixingchamber 22 although, clearly, the twoportions adjustable valve 26 between the twoportions tube portion 24 a may flow freely into thetube portion 24 b, or may be partially or fully closed to block, wholly or partially, the flow of gas between theportions pressure gauge 28 is advantageously provided that is connected to theadjustable valve 26 or to one of the twoportions tube 30 to provide an indication of the level of pressure in thebypass tube 24. - While the
tube 24 is shown as a bypass tube connected to the same supply of high pressure gas supplying theinlet pipe 20, it is also possible, and contemplated by the invention, that two separate entries of high pressure are provided, each separately supplying high pressure to theinlet pipe 20 and to thetube 24, which would no longer be a bypass tube as shown inFIGS. 1 and 2 . - Within the interior of the mixing
chamber 22 there is provided a mixing compartment, shown as being generally elongated along the chamber axis AC. - The
cold pipe 16, and specifically its external tread and theremote end 16 b are dimensioned to mesh with internal threads at the cold gas inlet opening 22 b. All of the threaded connections are preferably sealed in any conventional manner to prevent the escape of gas through these joints. In this connection, it is also possible to attach the various tubes and pipes shown and discussed above by means other than treated connections. Thus, these tubes may be attached to each other by the conventional means such as welding, adhesive, etc. - The gas that feeds the mixing
chamber 22 by means of thebypass tube 24 is designated by thereference numeral 34, this being high pressure gas that is at ambient temperature. Thecold pipe 16 injects a cold stream ofgas 36 into themixing compartment 32, at a point intermediate the outlet end of thetube portion 22 c and theoutlet tube 38 of the mixingchamber 22. - The specific configuration of the mixing
chamber 22 is not critical, although it is preferable that the end of thecold pipe 16 at 16 b be positioned or is located closer to the outlet opening 22 c than is thetube portion 24 c. In the presently preferred embodiment, the mixingchamber 22 is in the form of cylindrical hollow tubular member that is sealed or closed with the exceptions of openings described. The mixing chamber has an axial length “1” along the axis AC and has a diameter “d”. The cold andhot pipes vortex tube 12 axis AV, and the axes AC and AV are preferably relative to each other inclined at an angle α as shown. The angle α is 45° in the present preferred embodiment, although this angle may be varied considerably, with different degrees of advantage. It is also preferred that thecold air stream 36 be injected at a distance approximately 1.5-2 inches from the outlet to 38. This distance can, also, be modified slightly with different degrees of advantage. The angle of 45° is generally preferred and provides improved results. Thus, while the highpressure air stream 34 generally enters along the axis AC shown, the lower pressurecold air stream 36 as injected at angle of 45° relative to thehigh pressure stream 34, the gas is being mixed within the mixing chamber and exit as astream 40 that may be at higher pressure than the pressure of thestream 36 but it has been elevated temperature somewhat depending on the adjustment of thevalve 26, between the temperatures of the ambient andcold streams - Referring now to
FIG. 3 , another present preferred embodiment of the invention is illustrated that is generally is designated by thereference numeral 10′. As it will be more fully described below, the difference between the device illustrated inFIG. 2 and the one illustrated inFIG. 1 is that the device illustrated inFIG. 2 includes a temperature amplification device, utilizing a feedback loop, that is used for a lower temperature of the usable out-stream of gas. - In
FIG. 2 , apre-cooler housing 42 is provided that may be made of plastic or other temperature insulating or heat-flow resistant material. Thepre-cooler housing 42 has an inlet opening 42 a and anoutlet opening 42 b, shown at opposing or opposite sides of the housing. A pair of opposingopenings openings pre-cooling housing 42 has an internal chamber, cavity orcompartment 42 e that serves as a heat exchange chamber, as it will become more evident from the discussion that follows. - The
mixer 22 is connected, at its inlet end with abypass tube valve 26. As indicated, thevalve 26 can be used to adjust the pressure and, therefore, the gas flow velocity from the inlet to themixer chamber 22. The coldair inlet tube 16 transfers the cooledair 36 from the cooledair end 12 a of thevortex tube 12 as previously described. Thehigh pressure gas 34 is mixed with the cooledair 36 and the mixed gas is channeled by means ofpipe portions 38 a-38 e to the inlet opening 42 c of the cooling chamber. The highpressure inlet tube 20 is now formed of spacedsections inlet pipe portion 20 x has a threadedend 20 x′ that is connected, such as by bushing 46, to a heat exchange tube orpipe 48 that has opposing threaded ends 48 a and 48 b that are respectively attached to thebushing 46, at one end, and acoupling 50 that joins the threadedend 48 as well as a threaded end 21′ of thepipe portion 20 y. It will be clear, therefore, that the high pressure gas entering thepipe portion 20 x passes through theheat exchange pipe 48 and into thevortex tube 12 by means of a pipe ortube portion 20 y. The gas in the pipes ortubes 38 a-38 e emanates from the mixingchamber 22 and is directed into the compartment orchamber 42 e and exits as the cooledgas stream 40. However, because the cooled air stream fills the chamber orcompartment 42 e, it absorbs some of the heat from the heat exchanger pipe ortube 48, as it passes through the pre-cooler 42, and ultimately is outputted for use in cooling objects. Theheat exchanger 48, therefore, becomes cooler in time, and high pressure gas that passes through pipe ortube portions pre-cooling chamber 42 is likewise cooled by the removal of heat. - The operation of the device illustrated in
FIG. 2 will now be described. Initially, the high pressure gas P enters thetube portion 20 x and is guided through theheat exchanger tube 48 and through thetube portion 20 y into thevortex tube 12. As all the temperatures are initially at ambient temperature, there is a little or not heat transfer to the initial stream of the high pressure gas stream as it enters the vortex tube. However, the cooledair stream 36 exiting from the cooled air outlet end 12 a of the vortex tube is mixed withhigh pressure gas 34 in the mixingchamber 22, as previously described. Since the highpressure gas stream 34 is typically at a higher temperature than the temperature of the cooledgas stream 36, thegas stream 38 that exits the mixingchamber 22 tends to be at a temperature between of temperature of the high pressure gas and the cooled air stream. The mixingchamber 22, therefore, elevates the temperature of the cooledair stream 36, although that stream is now at a higher pressure. The cooled air stream that enters thepre-cooling chamber 42 lowers the temperature within that chamber and there is a transfer of heat due to the cooling effect of theheat exchanger tube 48. As theheat exchanger tube 48 cools, high pressure has P passing through theheat exchanger tube 48 is pre-cooled before it enters thevortex tube 12 at the high pressureinput pipe portion 20 y. Such pre-cooled gas is then further cooled by thevortex tube 12 and this results in further cooling at the outlet of the mixingchamber 22, and additional cooling of theheat exchanger tube 48. Such a feedback-type arrangement continues to increasingly cool theheat exchanger tube 48 thereby resulting in a continued drop in temperature of the input gas pressure stream P prior to entry into thevortex tube 12. Thepre-cooling chamber 48 is, therefore, in the nature of an amplification device and it amplifies the cooling effect of the cooled output gas outputted by thevortex tube 12 and the gas exiting the mixingchamber 22. This continues until an equilibrium is reached when the drop in the temperature in the pre-cooling chamber is such that decreases in temperature are compensated or offset by increases in heat transfer from the ambient atmosphere. - Referring to
FIGS. 3 and 4 , the heat and temperature parameters can be explained in term of the device shown inFIG. 2 . Thus, the inlet air at high pressure enters at heat level Q1. As indicated, initially, thepre-cooling chamber 42 is at ambient and there are no change in temperature as the high pressure gas passes through the heat exchange or transfertube 48. However, in time, theheat transfer tube 48 cools off and there is a change in heat −ΔQ1 as the high pressure gas passes though theheat exchanger tube 48. The gas passing through theheat exchanger tube 48 is modified, therefore, by a change in heat −ΔQ1 as it enters thevortex tube 12. The air in the vortex tube is further modified at the heated end by a decrease of heat −ΔQ2 at one end and an increase in heat at the other end at +ΔQ3. The outlet of thevortex tube 12 is at a heat level Q4 as it enters the mixingchamber 22 where the heat level is increased by +ΔQ4, due to the addition of and mixing with the high pressure gas at ambient emanating directly from the high pressure side. The heat level Q5 at the inlet to theheat exchanger 48 may experience slight rise in heat removed from the ambient high pressure gas at Q1. However, because the flow of Q5 is relatively high through thepre-cooling chamber 48 the heat level Q6 is approximately equal to Q5. - In
FIG. 4 , a transition is shown between the temperature T of thestream 40 over time after the device is activated. At t1, the temperature is at T1. As the cooledair 36 from thevortex tube 12 circulates through the mixingchamber 22 and thepre-cooling chamber 42, there is a gradual drop in the temperature of theheat exchanger tube 48 and the amount of heat exchange results in a drop in temperature of the gas exiting thepre-cooling chamber 48 into theinput pipe portion 20 y of the vortex tube. The drop of temperature continues until time t2 when the temperature has dropped to T2, where the temperature remains as long as the device operation is maintained. As indicated, the temperature does not drop below T2 because a equilibrium state is reached between the amount of heat removed from the flowing gases and the amount of heat that is transferred to the device from the ambient atmosphere. Clearly, the greater the differential in the temperatures between the temperature T2 and the ambient the greater the heat added from the ambient atmosphere and that is the reason why a steady state condition is reached in time. However, examiningFIG. 3 it will be clear that the differences in heat levels between the embodiments shown inFIG. 2 is −ΔQ1 imparted by thepre-cooling chamber 48. The greater the efficiency of the pre-cooling chamber, therefore, the greater the quantity −ΔQ1 and the greater the temperature drop in the outlet stream of cooledair 40. Constructions to optimize the efficiency of theheat exchanger - It would be obvious to those having skill in the art that many changes may be made to the details of the above-described embodiments without departing from the underlying principles of the invention. The scope of the present invention should, therefore, be determined only by spirit and the scope of the disclosure and the state of the prior art.
Claims (20)
1. Temperature adjustable airflow device comprises a vortex tube having a high pressure gas inlet and cooled and heated outlets; a mixing chamber having first and second ends, one gas inlet end at said first end and a gas outlet end at said second end, and an intermediate gas inlet end between said first and second ends, a high pressure inlet conduit connected to said high pressure gas inlet of said vortex tube and to said gas inlet end of said mixing chamber, and said cooled vortex tube outlet being connected to said intermediate gas inlet end, said mixing chamber mixing high pressure gas with cooled gas from said vortex tube to enhance the pressure of cooled gas emanating from said vortex tube.
2. Device as defined in claim 1 , further comprising a gas valve for adjusting the pressure of gas entering said high pressure gas inlet of said mixing chamber.
3. Device as defined in claim 2 , further comprising indicator means for providing an indication of the pressure of the gas entering said high pressure gas inlet of said mixing chamber.
4. Device as defined in claim 1 , wherein said mixing chamber is in the form of an elongated cylindrical member having a length l, and said gas outlet end at said second end being spaced from said intermediate gas inlet end at distance within the range of 0.1 l-0.5 l.
5. A device as defined in claim 4 , wherein said distance is approximately 0.3 l.
6. A device as defined in claim 4 , wherein said distance is approximately 1.5-2.0 inches.
7. A device as defined in claim 1 , wherein said intermediate gas inlet end is arranged to introduce a cooled gas flow from said vortex tube into said mixing chamber at an angle α<90° in relation to a longitudinal axis of said mixing chamber.
8. A device as defined in claim 7 , wherein the gas flows introduced into said gas inlet at said first end and said intermediate gas inlet are introduced along directions defining an angle α less than 90°.
9. A device as defined in claim 8 , wherein a is approximately 45°.
10. Device as defined in claim 1 , further comprising means for pre-cooling high pressure gas entering said vortex tube high pressure has inlet.
11. Device as defined in claim 10 , wherein said pre-cooling means includes heat transfer means for cooling the high pressure gas entering said vortex tube with gas cooled by said vortex tube.
12. Device as defined in claim 11 , wherein said heat transfer means comprises a pre-cooling chamber, at least a portion of a conduit feeding high pressure gas to said vortex high pressure gas inlet extending through said pre-cooling chamber, cooled gas from said gas outlet end of said mixing chamber being directed into said pre-cooling chamber prior to being used to cool an object, whereby said gas form said outlet of said mixing chamber cooling said at least a portion of said conduit to pre-cool high pressure gas before it is directed into said vortex tube.
13. Device as defined in claim 12 , wherein a tube or conduit connects said mixing chamber gas outlet end at said second end to an inlet to said pre-cooling chamber.
14. Device as defined in claim 12 , wherein said pre-cooling chamber is formed of thermally insulated material.
15. Device as defined in claim 12 , wherein said pre-cooling chamber is formed of plastic.
16. Device as defined in claim 12 , wherein said pre-cooling chamber is formed of a material having a low thermal conductivity.
17. Device as defined in claim 12 , wherein said at least one portion of said conduit is formed of a material having high thermal conductivity.
18. Device as defined in claim 12 , wherein said at least one portion of said conduit has an enhanced surface area to promote heat transfer.
19. Device as defined in claim 18 , wherein said conduit portion has longitudinal ribs to enhance surface area.
20. Device as defined in claim 12 , wherein said pre-cooling chamber is sealed to prevent escape of cooled gas entering from said mixing chamber except through said gas outlet of said pre-cooling chamber for cooling an object.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US12/345,110 US20100139292A1 (en) | 2008-12-08 | 2008-12-29 | Temperature adjustable airflow device |
PCT/US2009/067109 WO2010077637A1 (en) | 2008-12-08 | 2009-12-08 | Temperature adjustable airflow device |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US12054508P | 2008-12-08 | 2008-12-08 | |
US12/345,110 US20100139292A1 (en) | 2008-12-08 | 2008-12-29 | Temperature adjustable airflow device |
Publications (1)
Publication Number | Publication Date |
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US20100139292A1 true US20100139292A1 (en) | 2010-06-10 |
Family
ID=42229544
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US12/345,110 Abandoned US20100139292A1 (en) | 2008-12-08 | 2008-12-29 | Temperature adjustable airflow device |
Country Status (2)
Country | Link |
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US (1) | US20100139292A1 (en) |
WO (1) | WO2010077637A1 (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
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WO2016089573A1 (en) * | 2014-12-03 | 2016-06-09 | Universal Vortex, Inc. | Improved vortex tube |
RU2622449C1 (en) * | 2016-07-15 | 2017-06-15 | Федеральное государственное бюджетное образовательное учреждение высшего образования "Юго-Западный государственный университет" (ЮЗГУ) | Solar heat and cold supply system |
US20180259227A1 (en) * | 2014-12-03 | 2018-09-13 | Universal Vortex, Inc | Vortex tube |
CN110108057A (en) * | 2019-05-15 | 2019-08-09 | 武汉华工正源光子技术有限公司 | Optical communication module temperature production device for testing and method based on vortex tube |
CN112604540A (en) * | 2020-11-24 | 2021-04-06 | 德清县万诚晶体纤维有限公司 | High-temperature binder strong stirring equipment for refractory material |
CN113319130A (en) * | 2021-06-29 | 2021-08-31 | 燕山大学 | Continuous rolling plate temperature control method and device |
US11149991B2 (en) * | 2019-02-15 | 2021-10-19 | Yang Yoon Seon | Heating and cooling apparatus having moisture removal function for testing electrical characteristic of semiconductor element using probe system |
US11493239B2 (en) | 2018-09-28 | 2022-11-08 | Universal Vortex, Inc. | Method for reducing the energy necessary for cooling natural gas into liquid natural gas using a non-freezing vortex tube as a precooling device |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
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USD939359S1 (en) | 2019-10-01 | 2021-12-28 | The Procter And Gamble Plaza | Packaging for a single dose personal care product |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3858403A (en) * | 1974-01-30 | 1975-01-07 | Wilkerson Corp | Method and apparatus for drying gases |
US4339926A (en) * | 1981-08-03 | 1982-07-20 | E. D. Bullard Company | Vortex tube |
EP0684433A4 (en) * | 1993-02-22 | 1996-06-26 | Aleksandr Stepanovic Tatarinov | Process for controlling thermodynamic processes in a vortex tube, vortex tube for carrying out the said process and the use thereof. |
-
2008
- 2008-12-29 US US12/345,110 patent/US20100139292A1/en not_active Abandoned
-
2009
- 2009-12-08 WO PCT/US2009/067109 patent/WO2010077637A1/en active Application Filing
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2016089573A1 (en) * | 2014-12-03 | 2016-06-09 | Universal Vortex, Inc. | Improved vortex tube |
US20160158900A1 (en) * | 2014-12-03 | 2016-06-09 | Universal Vortex Inc. | Vortex Tube |
US20180259227A1 (en) * | 2014-12-03 | 2018-09-13 | Universal Vortex, Inc | Vortex tube |
RU2622449C1 (en) * | 2016-07-15 | 2017-06-15 | Федеральное государственное бюджетное образовательное учреждение высшего образования "Юго-Западный государственный университет" (ЮЗГУ) | Solar heat and cold supply system |
US11493239B2 (en) | 2018-09-28 | 2022-11-08 | Universal Vortex, Inc. | Method for reducing the energy necessary for cooling natural gas into liquid natural gas using a non-freezing vortex tube as a precooling device |
US11149991B2 (en) * | 2019-02-15 | 2021-10-19 | Yang Yoon Seon | Heating and cooling apparatus having moisture removal function for testing electrical characteristic of semiconductor element using probe system |
CN110108057A (en) * | 2019-05-15 | 2019-08-09 | 武汉华工正源光子技术有限公司 | Optical communication module temperature production device for testing and method based on vortex tube |
CN112604540A (en) * | 2020-11-24 | 2021-04-06 | 德清县万诚晶体纤维有限公司 | High-temperature binder strong stirring equipment for refractory material |
CN113319130A (en) * | 2021-06-29 | 2021-08-31 | 燕山大学 | Continuous rolling plate temperature control method and device |
Also Published As
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WO2010077637A1 (en) | 2010-07-08 |
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