KR20170005745A - Open typed system for air cooling - Google Patents
Open typed system for air cooling Download PDFInfo
- Publication number
- KR20170005745A KR20170005745A KR1020150144156A KR20150144156A KR20170005745A KR 20170005745 A KR20170005745 A KR 20170005745A KR 1020150144156 A KR1020150144156 A KR 1020150144156A KR 20150144156 A KR20150144156 A KR 20150144156A KR 20170005745 A KR20170005745 A KR 20170005745A
- Authority
- KR
- South Korea
- Prior art keywords
- air
- nozzle
- compression
- expansion
- compression member
- Prior art date
Links
Images
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24F—AIR-CONDITIONING; AIR-HUMIDIFICATION; VENTILATION; USE OF AIR CURRENTS FOR SCREENING
- F24F5/00—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D25/00—Pumping installations or systems
- F04D25/02—Units comprising pumps and their driving means
- F04D25/08—Units comprising pumps and their driving means the working fluid being air, e.g. for ventilation
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24F—AIR-CONDITIONING; AIR-HUMIDIFICATION; VENTILATION; USE OF AIR CURRENTS FOR SCREENING
- F24F5/00—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater
- F24F5/0003—Exclusively-fluid systems
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24F—AIR-CONDITIONING; AIR-HUMIDIFICATION; VENTILATION; USE OF AIR CURRENTS FOR SCREENING
- F24F5/00—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater
- F24F5/0007—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater cooling apparatus specially adapted for use in air-conditioning
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24F—AIR-CONDITIONING; AIR-HUMIDIFICATION; VENTILATION; USE OF AIR CURRENTS FOR SCREENING
- F24F5/00—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater
- F24F5/0007—Air-conditioning systems or apparatus not covered by F24F1/00 or F24F3/00, e.g. using solar heat or combined with household units such as an oven or water heater cooling apparatus specially adapted for use in air-conditioning
- F24F5/001—Compression cycle type
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Life Sciences & Earth Sciences (AREA)
- Sustainable Development (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Jet Pumps And Other Pumps (AREA)
Abstract
Description
The present invention relates to a system for cooling air, and more particularly, to a system for cooling air efficiently by eliminating a complicated structure for circulating refrigerant and refrigerant by using the principle of the single thermal expansion and the Joule-Thomson principle To an open air cooling system.
Generally, in the air cooling system, a system is used in which a refrigerant is primarily cooled using a compression and expansion valve using a refrigerant, and a refrigerant is secondarily passed through an air fin tube to cool the air.
1, the air conditioner includes a
On the other hand, it is already known that the refrigerant used in this air conditioner is mainly used as the refrigerant gas, and the chemical substance emitted from the freon gas breaks the oxygen bond of the ozone and destroys the ozone layer in the stratosphere. In view of this, environment-friendly refrigerants have recently been introduced and used in many devices. However, this is also the reality that the refrigerant is prohibited from a certain point in time, or is expensive and has no market competitiveness because it is regulated by the Montreal Convention or the Kyoto Convention .
In other words, in order to realize a method of cooling the air while circulating the refrigerant through compression, condensation, expansion, evaporation, etc., it requires a lot of energy and electricity, requires complicated devices and expensive parts, There is a problem such as purchasing.
It is an object of the present invention, which is devised to overcome the above-described problems, to provide an apparatus and a method for supplying air of a surrounding ambient temperature by utilizing the principle of the Ji- And to provide an open air cooling system in which cooling air is discharged by repeating compression and expansion.
To achieve the above object, an open air cooling system according to the present invention includes: a blowing device; And a main body having a compression section that is compressed while the outside air supplied from the air blowing apparatus passes and an expansion section that diffuses and expands air that has passed through the compression section.
Here, the compressed portion is provided with an air compressing member for compressing air as it passes, and the air compressing member is a porous plug, a mesh type medium or a plurality of beads accommodated therein so as to compress air passing therethrough, And is in a mixed form.
In one specific embodiment, the main body includes: a first compression portion having a compression space into which air supplied to the air blowing device flows, and a first nozzle through which air in the compression space passes; A first air compression member into which air having passed through the first nozzle flows and is compressed, a second nozzle through which compressed air passes through the first air compression member, a first nozzle through which air passing through the second nozzle diffuses and expands, A compression / expansion unit having an expansion space and a third nozzle through which air in the first expansion space passes; A second compression unit including a second air compression member into which air having passed through the third nozzle flows and is compressed and a fourth nozzle through which compressed air passes while passing through the second air compression member; And an expansion part having a second inflation space through which the air that has passed through the inflow is diffused and expanded and then is discharged to the outside.
At least one of the first air compression member and the second air compression member may be a porous plug, a mesh type medium or a plurality of beads, or at least two of them may be mixed.
Further, the porous plug or mesh-like medium or bead is at least one of copper, copper alloy, aluminum, aluminum alloy, graphene, charcoal and activated carbon.
The first nozzle, the second nozzle, the third nozzle and the fourth nozzle are at least one perforated hole.
At least one of the first nozzle, the second nozzle, the third nozzle, and the fourth nozzle may be processed to have the same diameter on both sides or to be expanded in diameter so that air is diffused and jetted, Is reduced in diameter so as to be injected at a higher pressure.
Also, the compression / expansion part is divided into a partition wall in which the second nozzle is machined, and the first air compression member is arranged in one side space having a large area or a long side on the side, and the other side space So that the first expansion space is formed.
The fourth nozzle-side surface of the second expansion space is an inclined surface that is inclined at an angle smaller than the vertical angle on the side surface in order to prevent the generation of vortex of the air that has passed through the fourth nozzle.
And the cross-sectional area of the compression / expansion portion is wider than the cross-sectional area of the first compression portion so that the air having passed through the first nozzle diffuses and flows into the first air compression member, And the cross-sectional area of the expanding portion is in the form of at least one of the shapes wider than the cross-sectional area of the second compression portion so that air passing through the fourth nozzle diffuses.
As described above, according to the present invention, by circulating ambient air at room temperature and cooling it while repeatedly compressing and expanding, it is possible to lower the temperature of the surrounding space without using a specific gas or refrigerant like a conventional air conditioner.
Further, since only a general blowing fan or a turbo fan is driven instead of using a number of precise parts including a high-pressure compressor as in the past, the electric power can be saved remarkably, and the cost for maintenance due to simple parts and structure can be reduced There is an effect that can be.
Further, since ambient air is used without using refrigerant such as helium or freon which hinders the environment, there is an effect of being environmentally friendly without any generation of waste that damages the environment such as ozone layer destruction.
BRIEF DESCRIPTION OF THE DRAWINGS The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate preferred embodiments of the invention and, together with the description, serve to further the understanding of the technical idea of the invention, Should not be interpreted.
Fig. 1 is a schematic view showing the basic structure of a general air conditioner.
Figure 2 is a general isenthalf diagram.
3 is a Ts diagram of a general refrigeration cycle.
4 is a schematic configuration diagram of a general refrigeration cycle.
5 is a diagram schematically illustrating a basic structure of a general Gipford-McMahon cycle.
6 is a graph relating to general thermal expansion.
7 is a diagram showing the basic principle of an open air cooling system according to the present invention.
Figure 8 is a cross-sectional side view of a preferred embodiment of an open air cooling system implemented on the basis of the basic principles of Figure 7;
FIG. 9 is a location-specific thermal distribution diagram showing the simulation results of the air cooling system of FIG.
FIG. 10 is a graph showing the temperature change by length in FIG.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings. However, the detailed description of known functions and configurations incorporated herein will be omitted when it may unnecessarily obscure the subject matter of the present invention.
<Configuration>
Figure 2 is a general isenthalf diagram. 3 is a T-s diagram of a general refrigeration cycle. 4 is a schematic configuration diagram of a general refrigeration cycle. 5 is a graph relating to general thermal expansion. FIG. 6 is a diagram schematically showing a basic structure of a general Gipford-Macmaon cycle.
The open air cooling system according to the present invention has a basic structure of the Gifford-Mcmahon cycle without Joule-Thomson (JT) refrigeration and displacer, Principle. Therefore, in order to understand the principle of the present invention, the principle of the refrigeration method and the thermal expansion of the line-Thomson will be briefly described.
First, the Joule-Thomson (J-T) freezing method is a method of obtaining a low temperature by using the line-Thomson effect generated when the high-pressure gas is freely expanded to low pressure. The J-T refrigerator using this method has a simple structure, and is free from mechanical vibration or friction, and can be stably operated for a long time. However, the J-T refrigerator internally generates a lot of entropy due to the irreversibility of the J-T expansion process. This is less efficient than a regenerative cryocooler using a reverse-brayton cycle refrigerator or a regenerative heat exchanger that expands the gas using an expander There is a disadvantage.
However, since JT refrigerators using mixed refrigerants as working fluids can greatly reduce the irreversibility that occurs internally, a well-designed mixed-refrigerant JT chiller can achieve sufficient efficiency to compete with the other types of chillers mentioned above have. Therefore, in the case of a refrigeration cycle in which a mechanical expander can not be used due to hydraulic problems arising from the expansion of the two-phase fluid, the mixed refrigerant JT refrigerator can be used in place of a retro-Brayton cycle or regenerative heat exchanger have. In addition, it is composed of other refrigerators and multi-stages in order to obtain very low temperature with a simple structure and is used in hybrid form. As such, J-T refrigerators are also used in various fields today.
Hereinafter, the development process of the J-T refrigerator will be described.
The JT refrigeration system is based on the Linde-Hamson cycle, a refrigeration cycle using the JT effect. Here, the JT effect refers to a phenomenon in which the temperature changes along an isenthalpic curve (see FIG. 2) when the actual gas expands freely while passing through an insulated narrow passage such as a capillary, an orifice, or the like. That is, except for helium (He), hydrogen (H 2 ) and neon (Ne), the temperature of most gases becomes low when they are freely expanded at high pressure or room temperature. Therefore, the lower the temperature, the larger the JT effect, so the lower the temperature through precooling, the larger the JT effect can be.
A refrigerating cycle (Linde-Hampson) cycle using the J-T effect can be represented by a T-s diagram as shown in FIG. 3, and a schematic diagram of the system of this cycle can be shown in FIG. In this cycle, the refrigerant at normal temperature and high pressure is precooled by heat exchange with low-temperature and low-pressure refrigerant that has undergone the expansion process while passing through the heat exchanger, and the precooled refrigerant is heat- After cooling the object to be cooled (③-> ④), it is used to pre-cool the supply refrigerant while passing through the heat exchanger (④-> ⑤). After that, the refrigerant exiting the heat exchanger is compressed again through the compressor and circulated (⑤-> ①) or discharged to the outside and discarded.
At this time, a system circulating through a compressor is called a closed cycle, and a system in which a gas is supplied from a high-pressure reservoir and is used for refrigeration and then discharged to the outside is called an open cycle. Here, the closed cycle is advantageous in that continuous use of gas can be maintained because a constant pressure ratio can be maintained because no gas is consumed because the gas charged in an appropriate amount is continuously circulated and used. However, there are many considerations such as the heat generated during the compression of the gas and the problem of the working fluid being dissolved in the oil, thus making the whole system large and complicated. On the other hand, since the open cycle does not use a compressor, it is advantageous in that it can be configured simply and in a small size even when the pressure ratio of high and low pressure is designed to be very large for rapid cooling. However, since the gas in the high-pressure reservoir is continuously consumed during the operation, it is difficult to maintain a constant pressure ratio for a long period of operation, and the refrigeration performance is gradually reduced.
Therefore, when the refrigeration cycle using the JT effect can not discharge the working fluid to the outside or is applied to a large-scale refrigeration system requiring continuous operation for a long time at a fixed position, it is configured as a closed cycle, Or in a small refrigeration system such as cooling of a moving device. Typical applications are closed circu- lar cycles such as large liquefaction plants, recondensers, and mixed refrigerant JT chillers that use active gas as a working fluid. The open cycle is used to cool small infrared sensors used in missiles and military equipment, Cooling of small electronic devices, probes for cryogenic surgery and the aerospace sector.
As shown in FIG. 5, the basic structure of the gefod-McMahon cycle is such that a warm piston and a cold piston are disposed on both sides and a porous regenerator And a compression space is provided between the heat exchanger and the warm piston, and an expansion space is provided between the heat exchanger and the cold piston.
Based on this basic structure, the principle is first to maintain the temperature of Ta in the state of the first ⓐ without compressing the internal gas.
Next, in the state where the warm piston is pressed, the inner gas is compressed and passes through the porous heat exchanger.
Next, when the cold piston is pressed back while the cold piston is backward, the gas inside is passed through the heat exchanger and compressed to the maximum.
Finally, when the cold piston rises back again, the gas expands to the maximum temperature T L and then falls.
Using helium gas for this principle can reach a cryogenic temperature of 4K. However, in order to realize this, it must be a closed cycle.
On the other hand, adiabatic expansion is a phenomenon in which the volume of a substance is increased without exchanging heat with the outside (see FIG. 6), and the three-phase substance (gas, liquid, solid) Increasing the temperature increases the volume. In other words, the temperature of the three-phase material is lowered when the material is expanded in the state of being insulated from the outside. Particularly, the thermal expansion is remarkable in the gas.
Expressing this expression, in the first law of thermodynamics,
ΔQ = ΔU + ΔW
ΔQ = ΔU + PΔV
(ΔQ: heat energy supplied to the gas, ΔU: increase in gas internal energy, ΔW: gas externally, P: pressure, ΔV: volume change)
(U: internal energy, n: mole number, R: gas constant, T: absolute temperature) is obtained by substituting the energy of ideal gas U = 3 / 2nRT,
0 = 3 / 2nR? T + P? V
Thus, when the volume expands (V> 0), the temperature decreases (ΔT <0)
The principle of this thermal expansion is applied to a cryocooler, and this cryocooler is made to reach a cryogenic temperature by thermally expanding helium or nitrogen.
Hereinafter, the open air cooling system according to the present invention will be described in detail.
7 is a diagram showing the basic principle of an open air cooling system according to the present invention. Figure 8 is a cross-sectional side view of a preferred embodiment of an open air cooling system implemented on the basis of the basic principles of Figure 7; FIG. 9 is a location-specific thermal distribution diagram showing the simulation results of the air cooling system of FIG. FIG. 10 is a graph showing the temperature change by length in FIG.
The basic principle of the open air cooling system according to the present invention, which is created based on the above-described basic structure of the line-Thomson refrigeration system and the Gifford-Mcmahon cycle and the principle of the monotonic expansion, Air is forcedly injected from one side to the surrounding room while being passed through the heat exchanger, and the compressed air is rapidly expanded to be cooled, and then discharged to the other side. In particular, the air cooling system of the present invention is characterized in that surrounding air is used without using a refrigerant of a specific gas such as helium or Freon, and air of normal temperature is introduced from one side and air cooled to the other side is discharged. Structure. It is also possible to cool the air in the structure excluded from the displacer that moves with the piston in the GipoD-McMahon cycle.
The open air cooling system of the present invention, which is manufactured on the basis of these basic principles and features, comprises a
The
The
Further, the nozzle is arranged between the porous plug and the expanding portion, and configured to discharge the compressed air through the porous plug to the expanding portion.
The expanding portion has a large expansion space so that it can expand while rapidly diffusing the air discharged from the nozzle. Each of the compression unit, the nozzle and the expansion unit may be arranged in sequence, or a plurality of compression units, a nozzle, and an expansion unit may be arranged in connection with each other.
Hereinafter, the
The
The
First, in the
Further, the
The compression /
The first
The size of the first
The
At least one of the
The
The
Meanwhile, the
Here, the second
In addition, the
Meanwhile, the
In order to further lower the temperature of the cooled air, at least one of the compression /
As a result of the simulation of the open air cooling system according to the present invention constructed as described above, the temperature distribution of the finally discharged air is significantly lower than the temperature of the introduced air as shown in FIG. That is, the ambient temperature at room temperature supplied from the
As described above, those skilled in the art will appreciate that the present invention may be embodied in other specific forms without departing from the spirit or essential characteristics thereof. It is therefore to be understood that the above-described embodiments are to be considered in all respects as illustrative and not restrictive. The scope of the present invention is defined by the appended claims, rather than the detailed description, and all changes or modifications derived from the meaning and scope of the claims and equivalents of the claims are to be construed as being included within the scope of the present invention do.
100: blower
200:
210: first compression section
211: compression space
212: first nozzle
220: compression / expansion part
221: first air compression member
222:
223: Second nozzle
224: first expansion space
225: third nozzle
230: second compression section
231: second air compression member
232: fourth nozzle
240: Expansion part
241: second inflation space
242: sloping surface.
Claims (10)
Wherein the compression section includes an air compression member for compressing air as it passes,
Wherein the air compression member is a porous plug, a mesh-type medium or a plurality of beads is accommodated in order to compress air passing therethrough, or at least two of them are mixed.
The main body 200 includes a first compression unit 210 having a compression space 211 into which air supplied to the air blowing apparatus 100 is introduced and a first nozzle 212 through which air in the compression space 211 passes, ),
A first air compression member 221 through which the air having passed through the first nozzle 212 flows and is compressed, a second nozzle 223 through which compressed air passes through the first air compression member 221, Expanding portion 220 having a first expansion space 224 through which air that has passed through the second nozzle 223 diffuses and expands and a third nozzle 225 through which air in the first expansion space 224 passes, ),
A second air compression member 231 through which the air having passed through the third nozzle 225 flows and is compressed and a fourth nozzle 232 through which compressed air passes through the second air compression member 231, A second compression unit 230,
And an expansion unit (240) having a second expansion space (241) through which the air that has passed through the fourth nozzle (232) flows and diffuses and expands and then is discharged to the outside.
At least one of the first air compression member 221 and the second air compression member 231 may be a porous plug, a mesh type medium or a plurality of beads may be accommodated, or at least two of them may be mixed Open air cooling system.
Wherein the porous plug or mesh medium or bead is at least one of copper, copper alloy, aluminum, aluminum alloy, graphene, charcoal and activated carbon.
Wherein the first nozzle (212), the second nozzle (223), the third nozzle (225) and the fourth nozzle (232) are at least one perforated hole.
At least one of the first nozzle 212, the second nozzle 223, the third nozzle 225 and the fourth nozzle 232 may be formed so that both sides thereof have the same diameter, An open air cooling system in which the diameter is machined to an expanded form or the diameter is reduced so that the incoming air is injected at a higher pressure.
The compression / expansion unit 220 is partitioned by the partition wall 222 in which the second nozzle 223 is formed, and the first air compression member 221 is disposed in a space having a large area or a long side face, And the other side space having a narrow area or a short side length is a first expansion space (224).
One surface of the second expansion space 241 on the side of the fourth nozzle 232 is an inclined surface 242 inclined at an angle smaller than a vertical angle on the side surface in order to prevent generation of vortex of air passing through the fourth nozzle 232 An open air cooling system.
The cross-sectional area of the compression / expansion part 220 may be larger than the cross-sectional area of the first compression part 210 so that the air having passed through the first nozzle 212 is diffused and introduced into the first air compression member 221, The cross sectional area of the second compression portion 230 is narrower than the cross sectional area of the compression / expansion portion 220 to recompress air passing through the third nozzle 225, 4 nozzles 232. The open air cooling system of claim 1, wherein the at least one of the first and second nozzles has a width that is less than the width of the second compressed portion.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020150095804 | 2015-07-06 | ||
KR20150095804 | 2015-07-06 |
Publications (1)
Publication Number | Publication Date |
---|---|
KR20170005745A true KR20170005745A (en) | 2017-01-16 |
Family
ID=57993660
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
KR1020150144156A KR20170005745A (en) | 2015-07-06 | 2015-10-15 | Open typed system for air cooling |
Country Status (1)
Country | Link |
---|---|
KR (1) | KR20170005745A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU199366U1 (en) * | 2020-03-12 | 2020-08-28 | Сергей Александрович Гордин | Joule-Thompson effect air conditioner indoor unit |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20000021120A (en) | 1998-09-25 | 2000-04-15 | 윤덕용 | Ultra low temperature freezer using reverse brayton cycle |
KR20040097582A (en) | 2003-05-12 | 2004-11-18 | 정규진 | Aaccumulate cold type air Refrigerating machines |
KR20090113809A (en) | 2009-10-13 | 2009-11-02 | 정방균 | Air cooler |
-
2015
- 2015-10-15 KR KR1020150144156A patent/KR20170005745A/en unknown
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20000021120A (en) | 1998-09-25 | 2000-04-15 | 윤덕용 | Ultra low temperature freezer using reverse brayton cycle |
KR20040097582A (en) | 2003-05-12 | 2004-11-18 | 정규진 | Aaccumulate cold type air Refrigerating machines |
KR20090113809A (en) | 2009-10-13 | 2009-11-02 | 정방균 | Air cooler |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU199366U1 (en) * | 2020-03-12 | 2020-08-28 | Сергей Александрович Гордин | Joule-Thompson effect air conditioner indoor unit |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Geng et al. | Review of experimental research on Joule–Thomson cryogenic refrigeration system | |
Yari | Performance analysis and optimization of a new two-stage ejector-expansion transcritical CO2 refrigeration cycle | |
Nakagawa et al. | Supersonic two-phase flow of CO2 through converging–diverging nozzles for the ejector refrigeration cycle | |
CN1289887C (en) | Thermo-siphon method for providing refrigeration | |
JP4832563B2 (en) | Refrigeration system | |
KR20170104428A (en) | Open typed system for air cooling | |
Bai et al. | Experimental investigation on the influence of ejector geometry on the pull-down performance of an ejector-enhanced auto-cascade low-temperature freezer | |
Qin et al. | Experimental characterization of an innovative refrigeration system coupled with Linde-Hampson cycle and auto-cascade cycle for multi-stage refrigeration temperature applications | |
CN101275790A (en) | Low-temperature refrigerating method using carbon dioxide as circulating working substance and heat pump system thereof | |
KR20180098815A (en) | Open typed system for air cooling | |
KR20170005745A (en) | Open typed system for air cooling | |
JP2013036621A (en) | Refrigeration cycle device | |
Radebaugh | Microscale heat transfer at low temperatures | |
KR20170044616A (en) | Open typed system for air cooling | |
KR20180098817A (en) | Open typed system for air cooling | |
KR20180098819A (en) | Open typed system for air cooling | |
KR20180098820A (en) | Open typed system for air cooling | |
KR20180098826A (en) | Open typed system for air cooling | |
KR20170044447A (en) | Open typed system for air cooling | |
JP5485602B2 (en) | Refrigeration system | |
US20050016184A1 (en) | Stirling cooling device, cooling chamber, and refrigerator | |
Shire et al. | Investigation of microscale cryocoolers | |
Bradley et al. | Temperature instability comparison of micro-and mesoscale Joule-Thomson cryocoolers employing mixed refrigerants | |
CN104296417A (en) | Refrigerator for heat pipe | |
KR200251008Y1 (en) | Refrigeration cycle device for refrigerator |