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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2360
DESIGN AND ANALYSIS OF COUNTER FLOW VORTEX TUBE
Mr. Santosh Kansal1, Mr. Prateek Sharma2
1Assistant Professor Mechanical Engineering IET DAVV Indore, MP, India
2Student of Mechanical Engineering specialization in Design and Thermal IET DAVV Indore, MP, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - Vortex tube is a mechanical device, without any
moving parts. It separates the compressed air stream in to a
low temperature flow and a high temperature flow, such
separation of flow in two regions low side and high side is
known as the temperature or energy separation effect. Vortex
tube has many applications, for example, electronic systems
cooling, machining processes cooling, in aviation and
environmental chambers. This paper presents the design,
analysis and modifications of parametric design based on
parameters and data found in the literature. This paper
describes the experimental study of the temperature
separation phenomenon in a vortex tube. Effects of (1) using
insulation on tube, (2) the cold and hot orifice diameter, (3)
tube length, (4) using different material, and (5) Surface
roughness on the temperature reduction of the tube were
experimentally investigated.
Key Words: Vortex Tube, design, analysis, temperature,
energy separation effect
1. INTRODUCTION
The Vortex Tube (VT) is a device that generates cold and hot
air from compressed air. It was invented by Georges J.
Ranque in 1933[1]. The German engineer Rudolf Hilsch
suggested the working vortex tube design in 1947 [2]. It is a
simple device having low cost, with no moving parts, no
electricity and there is a possibilitytoadjustthetemperature
[3,4]. The main drawbacks are its low thermal efficiency,the
noise and the availability of compressed air. Vortex Tube is
commonly used in aviation, space/mining suitscooling,spot
cooling, when compressed air is available, like cutting tools
of CNC machines, laboratory equipment,etc.Compressed air
is sent through the tangential inlet nozzle so that the vortex
motion can be created inside the tube, fig. 1.
Fig -1:Vortex Tube Block Diagram
2. WORKING PRINCIPAL
Compressed air is passed through the nozzle as shown in
previous image. Then air expands through the nozzle and
acquires high velocity and swirl motion is created in vortex
chamber. Then due to its design, the air moves towards the
partly closed valve end. As it reaches the valve, the Kinetic
Energy is converted into the pressure energy and state of
stagnation isreached.Butthestagnationpressureishigheras
compared to the pressure at left side; therefore the reversal
in flow takes place. During this process, heat is transferred
from reversed streamtoforwardstream.Therefore,reversed
air stream gets cooled below the inlet temperature of the air,
while forward air stream gets heated up. The cold stream
escapes through the back side orifice, while hot stream is
passed through the opening of the valve. By controlling the
opening and closing of the valve, the quantity of the air and
its temperature can be varied.[3]
3. LITERATURE REVIEW
The Vortex Tube can be used in a temperature control work
and is very effective and economical where the compressed
air is readily available [1]. There is no better advantage of
this where the characteristics like low weight, combination
of cooler and heater are desired and the compressed air
which is the only main cost present with it. Refrigeration
plays a major role in developing the countries, generally it is
preferred for food preservation, also for providing the
comfortable environment especially it is used for air
conditioning. It plays a vital role in storage of ice, blood,
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2361
medicines, preservation of photographic films,
archaeological documents etc. by usingFreonorR134a R-11
to R-50 as a refrigerant, which are the main sources of the
ozone layer depletion. After a very long time an extensive
research is carried out for an alternative refrigeration
system. The vortex tube is found to be an excellent solution
or alternate solution for refrigeration system.[2] The vortex
tube performance mainly depends onfollowing parameters,
firstly air or working parameters such as inlet pressure of
compressed air and secondly tube or geometric parameters
such as length of hot side tube, cold orificediameter,number
of nozzles, diameter of nozzle, valve angle and also material
of vortex tube affects Coefficient of Performance (COP).[3,4]
UV Kongre et al analyzed the vortex tube model in Ansys
software. In their work, the design and transient thermal
analysis were done by using ansys. Ansys gives much better
approximation of experimental data to modeling data. Also
different materials were tested for their utility for vortex
tube manufacturing sustainable for further future
development.[3] MV Dudhe et al experimentedresultsofthe
energy separation in vortex tubes for different nozzle
diameters keeping the rest geometrical parameters
constant. It is experimentally manifested that the nozzle
diameter greatly affects the separation performance and
efficiency. The most importantpointrevealedinthispaperis
that there is an optimum nozzle diameter that gives the best
performance of vortex tube. An experimental investigation
has been performed to realize the thorough behavior of a
vortex tube cooling system.Thecounterflowvortextube has
been designed, manufactured and tested.[4]
4. DESIGN
3D parts are designed in CAD Software. WeusedSolidworks
Premium 2020 because it is the most popular CAD software
right now which gives better results than other CAD
software.
Following dimensions are used-
Hot tube length- 100mm
Hot tube outer and inner diameter- 15mm and 12mm
respectively
Generator diameter inner and outer- 20mm and 25mm
Nozzle diameter- 5mm
Cold tube diameter- 10mm
Valve diameter- 10mm
Full length- 134mm
After the modeling of each part, they were transferred to
the assembly window and all the parts were assembled.
Fig -2: Assembled model in Solidworks
5. ANALYSIS IN ASNSYS
After the assembly of model it was exported in IGS(Initial
graphics exchange specification) file format. It was done to
import it in other CAD/CAE softwares. Then the IGS file was
imported in Ansys workbench software. We used Ansys
workbench 17.0 version.
For this we used Fluent flow analysis system.
5.1 EXTRACTED FLUID DOMAIN
After our geometry imported indesignmodeller window, we
used Fill cavity method, After the fill cavity method, we got
our fluid body. The following picture(Fig.3) is the fluid
domain of our geometry.
Fig -3: Extracted fluid domain model
5.2 MESHING
Then we updated the geometry and moved into Meshing
window. We used tetrahedron meshing method.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2362
Fig -4: Meshing model
5.3 FLUENT SOLVER
After the successful meshing we updated our geometry and
moved into Fluent Solver window. Then we checked the
Energy equation for temperature measurements.
We are using turbulent flow, that’s why we used K-epsilon
model and checked viscous heating forpropervortexflow as
shown in Fig.5.
Fig -5: Setup in Fluent Solver
5.4 BOUNDARY CONDITIONS
NAMED SELECTIONS CONDITIONS
Inlet Pressure – 4 bar
Velocity - 0.1 m/s
Temperature – 295k
Hot outlet Guage Pressure – 0 bar
Rest default
Cold outlet Guage Pressure – 0 bar
Rest default
Wall Stationary wall
No slip
Roughness 0
Material name - Steel
6. RESULT
6.1 STEEL MATERIAL WITH ORIGINAL
DIMENSIONS
Cellzone conditions and boundary conditions were applied
as shown previous..
Max Temperature obtained – 316k
Min Temperature obtained – 280k
Fig -6: Result 1(Steel material)
6.2 STEEL MATERIAL AND LENGTH INCREASED
BY 40mm
Now the length is increased by 40mm, therefore the hot
tube length which was previously 100mm, now became
140mm.
Max Temperature obtained – 322k
Min Temperature obtained – 270k
Fig -7: Result 2(Length increased)
6.3 COPPER MATERIAL WITH ORIGINAL
DIMENSIONS
Now copper material was defined when applying cellzone
conditions.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2363
Max Temperature obtained – 320k
Min Temperature obtained – 270k
Fig -8: Result 3(Copper material)
6.4 GLASS WOOL INSULATION
Glass wool insulation of 8mm thickness used.
Max Temperature obtained – 322k
Min Temperature obtained – 268k
Fig -9: Result 4(Insulation)
6.5 SURFACE ROUGHNESS WITH ORIGINAL
DIMENSIONS
Surface roughness of 0.1 RA(roughness average) defined
inside the tube inner section.
Max Temperature obtained – 323k
Min Temperature obtained – 274k
Fig -10: Result 5(Surface roughness)
7. CONCLUSION
In our work we found that pressure is directly proportional
to the efficiency. Higher the pressure, higher is the
difference of hot flow and cold flow. We have used 4 bar
pressure in all the experiments. Generally 2 to 7 bar of
compressed air is used based on the designofthetube.Some
high grade industrial vortex tube can even sustain the
pressure of 12 to 15 bar.
From the above experiment , we have discovered that
copper gives better result compared to steel due to copper
conductivity is higher than steel.
Effect of tube length is also directly proportional to
efficiency but it is limited to some degree, as larger tube
length results in moist air at the end of outlets.
Effect of insulation is as expected, insulation decrease
temperature drop from tube wall to surroundings and
efficiency obtained is better.
Some value of roughness inside the tube gave better
result as compared to smooth surface finish. The reason is
that heat transfer increases due to the effect of increase in
the contact area.
If more than one inlets are used, then the resulting
efficiency achieved will be higher as more amount of high
pressurized air enters into the chamber.
Nozzle diameter should be balanced to achieve proper
tangential motion. Generally small diameter is always
desirable to avoid pressure loss but also not too small which
hinders the proper tangential flow.
ACKNOWLEDGEMENT
I owe a great thanks to many people who helped and
supported me during this research. Words will be always
inadequate to express my profound sense of gratitude tomy
project coordinator Mr. Santosh Kansal for his unfailing
support and invaluable suggestions at every point of time.
Last but not the least I would like to express a sense of
gratitude and love to my beloved parents and my friends for
their manual support, strength and help for everything.
REFERENCES
[1] Pramod Bajarang Vhankade, “Design and Manufacturing
of Vortex Tube “ ,International Journal of Science and
Research (IJSR) ISSN (Online): 2319-7064 2015
[2] Nitin V Galwade, Prof. Tushar Koli, Prof. Sayyad L.B,
“Design and Fabrication of Vortex Tube“ International
Journal of Scientific & Engineering Research Volume9,Issue
3, 56 ISSN 2229-5518 March 2018
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2364
[3] U. V. Kongre, M. D. Kurve, P. R Angaitkar, S. R. Ade,
“Design and analysis of vortex tube refrigeration”,
International Research Journal of Engineering and
Technology (IRJET) e-ISSN: 2395-0056Volume:05Issue:04
| www.irjet.net p-ISSN: 2395-0072 , IRJET Apr-2018
[4] U. V. Kongre, M. V. Dudhe, A. N. Petkar, V. S. Kamble ,S. M.
Kamble , “Investigation of vortex tube refrigeration with
novel material “ , © IJCRT | Volume 6 | ISSN: 2320-2882
2018
[5] Dhruv Manilawala , Saurav Koul , KiranMarudwar,Keval
Oswal, “Design, Manufacturing and Testing of Vortex Tube”,
International Journal of Future Generation Communication
and Networking Vol. 13, No. 2s, (2020)
[6] Mustafa Abdulhussain “A review on the vortex tube
geometrical affecting parameters”Journal ofMechanical and
Energy Engineering, Vol. 4(44), No. 1, 2020
[7] F. P. Branco, E. D. Buchelt, F. M. Barbosa, B. P.Rosa,andD.
J. Laporte “Design And Study Of Dimensional Parameters
Influence On Vortex Tube Behavior”Universidade Católica
Dom Bosco Departamento de Engenharia Mecânica Bairro
Jardim Seminário CP. 79117-900, Campo Grande, MS, Brasil
[8] Upendra Behera a , P.J. Paul a , S. Kasthurirengan b , R.
Karunanithi b , S.N. Ram b , K. Dinesh b , S. Jacob “CFD
analysis andexperimental investigationstowardsoptimizing
the parameters of Ranque–Hilsch vortex tube“ Department
of Aerospace Engineering, Indian Institute of Science,
Bangalore 560 012, India
[9] Penka Zlateva. Krystin Yordanov, diyan M. Dimitrov
“Numerical simulation of temperature separation
phenomena inside vortex tube” technical university of
Varna, Dep. Heat Engineering, Bulgaria ,2014
[10] Wasan Naksanee, Rathassak Prommas ” An
Experimental Investigation to Reduce the Temperature of
Hot Air by means of a Vortex Tubefed with Low Inlet Air
Pressure and a Specific Snail Nozzle Geometry
Article in International Journal of Engine” International
Journal of Engineering and Technology · June 2018

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DESIGN AND ANALYSIS OF COUNTER FLOW VORTEX TUBE

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2360 DESIGN AND ANALYSIS OF COUNTER FLOW VORTEX TUBE Mr. Santosh Kansal1, Mr. Prateek Sharma2 1Assistant Professor Mechanical Engineering IET DAVV Indore, MP, India 2Student of Mechanical Engineering specialization in Design and Thermal IET DAVV Indore, MP, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Vortex tube is a mechanical device, without any moving parts. It separates the compressed air stream in to a low temperature flow and a high temperature flow, such separation of flow in two regions low side and high side is known as the temperature or energy separation effect. Vortex tube has many applications, for example, electronic systems cooling, machining processes cooling, in aviation and environmental chambers. This paper presents the design, analysis and modifications of parametric design based on parameters and data found in the literature. This paper describes the experimental study of the temperature separation phenomenon in a vortex tube. Effects of (1) using insulation on tube, (2) the cold and hot orifice diameter, (3) tube length, (4) using different material, and (5) Surface roughness on the temperature reduction of the tube were experimentally investigated. Key Words: Vortex Tube, design, analysis, temperature, energy separation effect 1. INTRODUCTION The Vortex Tube (VT) is a device that generates cold and hot air from compressed air. It was invented by Georges J. Ranque in 1933[1]. The German engineer Rudolf Hilsch suggested the working vortex tube design in 1947 [2]. It is a simple device having low cost, with no moving parts, no electricity and there is a possibilitytoadjustthetemperature [3,4]. The main drawbacks are its low thermal efficiency,the noise and the availability of compressed air. Vortex Tube is commonly used in aviation, space/mining suitscooling,spot cooling, when compressed air is available, like cutting tools of CNC machines, laboratory equipment,etc.Compressed air is sent through the tangential inlet nozzle so that the vortex motion can be created inside the tube, fig. 1. Fig -1:Vortex Tube Block Diagram 2. WORKING PRINCIPAL Compressed air is passed through the nozzle as shown in previous image. Then air expands through the nozzle and acquires high velocity and swirl motion is created in vortex chamber. Then due to its design, the air moves towards the partly closed valve end. As it reaches the valve, the Kinetic Energy is converted into the pressure energy and state of stagnation isreached.Butthestagnationpressureishigheras compared to the pressure at left side; therefore the reversal in flow takes place. During this process, heat is transferred from reversed streamtoforwardstream.Therefore,reversed air stream gets cooled below the inlet temperature of the air, while forward air stream gets heated up. The cold stream escapes through the back side orifice, while hot stream is passed through the opening of the valve. By controlling the opening and closing of the valve, the quantity of the air and its temperature can be varied.[3] 3. LITERATURE REVIEW The Vortex Tube can be used in a temperature control work and is very effective and economical where the compressed air is readily available [1]. There is no better advantage of this where the characteristics like low weight, combination of cooler and heater are desired and the compressed air which is the only main cost present with it. Refrigeration plays a major role in developing the countries, generally it is preferred for food preservation, also for providing the comfortable environment especially it is used for air conditioning. It plays a vital role in storage of ice, blood,
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2361 medicines, preservation of photographic films, archaeological documents etc. by usingFreonorR134a R-11 to R-50 as a refrigerant, which are the main sources of the ozone layer depletion. After a very long time an extensive research is carried out for an alternative refrigeration system. The vortex tube is found to be an excellent solution or alternate solution for refrigeration system.[2] The vortex tube performance mainly depends onfollowing parameters, firstly air or working parameters such as inlet pressure of compressed air and secondly tube or geometric parameters such as length of hot side tube, cold orificediameter,number of nozzles, diameter of nozzle, valve angle and also material of vortex tube affects Coefficient of Performance (COP).[3,4] UV Kongre et al analyzed the vortex tube model in Ansys software. In their work, the design and transient thermal analysis were done by using ansys. Ansys gives much better approximation of experimental data to modeling data. Also different materials were tested for their utility for vortex tube manufacturing sustainable for further future development.[3] MV Dudhe et al experimentedresultsofthe energy separation in vortex tubes for different nozzle diameters keeping the rest geometrical parameters constant. It is experimentally manifested that the nozzle diameter greatly affects the separation performance and efficiency. The most importantpointrevealedinthispaperis that there is an optimum nozzle diameter that gives the best performance of vortex tube. An experimental investigation has been performed to realize the thorough behavior of a vortex tube cooling system.Thecounterflowvortextube has been designed, manufactured and tested.[4] 4. DESIGN 3D parts are designed in CAD Software. WeusedSolidworks Premium 2020 because it is the most popular CAD software right now which gives better results than other CAD software. Following dimensions are used- Hot tube length- 100mm Hot tube outer and inner diameter- 15mm and 12mm respectively Generator diameter inner and outer- 20mm and 25mm Nozzle diameter- 5mm Cold tube diameter- 10mm Valve diameter- 10mm Full length- 134mm After the modeling of each part, they were transferred to the assembly window and all the parts were assembled. Fig -2: Assembled model in Solidworks 5. ANALYSIS IN ASNSYS After the assembly of model it was exported in IGS(Initial graphics exchange specification) file format. It was done to import it in other CAD/CAE softwares. Then the IGS file was imported in Ansys workbench software. We used Ansys workbench 17.0 version. For this we used Fluent flow analysis system. 5.1 EXTRACTED FLUID DOMAIN After our geometry imported indesignmodeller window, we used Fill cavity method, After the fill cavity method, we got our fluid body. The following picture(Fig.3) is the fluid domain of our geometry. Fig -3: Extracted fluid domain model 5.2 MESHING Then we updated the geometry and moved into Meshing window. We used tetrahedron meshing method.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2362 Fig -4: Meshing model 5.3 FLUENT SOLVER After the successful meshing we updated our geometry and moved into Fluent Solver window. Then we checked the Energy equation for temperature measurements. We are using turbulent flow, that’s why we used K-epsilon model and checked viscous heating forpropervortexflow as shown in Fig.5. Fig -5: Setup in Fluent Solver 5.4 BOUNDARY CONDITIONS NAMED SELECTIONS CONDITIONS Inlet Pressure – 4 bar Velocity - 0.1 m/s Temperature – 295k Hot outlet Guage Pressure – 0 bar Rest default Cold outlet Guage Pressure – 0 bar Rest default Wall Stationary wall No slip Roughness 0 Material name - Steel 6. RESULT 6.1 STEEL MATERIAL WITH ORIGINAL DIMENSIONS Cellzone conditions and boundary conditions were applied as shown previous.. Max Temperature obtained – 316k Min Temperature obtained – 280k Fig -6: Result 1(Steel material) 6.2 STEEL MATERIAL AND LENGTH INCREASED BY 40mm Now the length is increased by 40mm, therefore the hot tube length which was previously 100mm, now became 140mm. Max Temperature obtained – 322k Min Temperature obtained – 270k Fig -7: Result 2(Length increased) 6.3 COPPER MATERIAL WITH ORIGINAL DIMENSIONS Now copper material was defined when applying cellzone conditions.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2363 Max Temperature obtained – 320k Min Temperature obtained – 270k Fig -8: Result 3(Copper material) 6.4 GLASS WOOL INSULATION Glass wool insulation of 8mm thickness used. Max Temperature obtained – 322k Min Temperature obtained – 268k Fig -9: Result 4(Insulation) 6.5 SURFACE ROUGHNESS WITH ORIGINAL DIMENSIONS Surface roughness of 0.1 RA(roughness average) defined inside the tube inner section. Max Temperature obtained – 323k Min Temperature obtained – 274k Fig -10: Result 5(Surface roughness) 7. CONCLUSION In our work we found that pressure is directly proportional to the efficiency. Higher the pressure, higher is the difference of hot flow and cold flow. We have used 4 bar pressure in all the experiments. Generally 2 to 7 bar of compressed air is used based on the designofthetube.Some high grade industrial vortex tube can even sustain the pressure of 12 to 15 bar. From the above experiment , we have discovered that copper gives better result compared to steel due to copper conductivity is higher than steel. Effect of tube length is also directly proportional to efficiency but it is limited to some degree, as larger tube length results in moist air at the end of outlets. Effect of insulation is as expected, insulation decrease temperature drop from tube wall to surroundings and efficiency obtained is better. Some value of roughness inside the tube gave better result as compared to smooth surface finish. The reason is that heat transfer increases due to the effect of increase in the contact area. If more than one inlets are used, then the resulting efficiency achieved will be higher as more amount of high pressurized air enters into the chamber. Nozzle diameter should be balanced to achieve proper tangential motion. Generally small diameter is always desirable to avoid pressure loss but also not too small which hinders the proper tangential flow. ACKNOWLEDGEMENT I owe a great thanks to many people who helped and supported me during this research. Words will be always inadequate to express my profound sense of gratitude tomy project coordinator Mr. Santosh Kansal for his unfailing support and invaluable suggestions at every point of time. Last but not the least I would like to express a sense of gratitude and love to my beloved parents and my friends for their manual support, strength and help for everything. REFERENCES [1] Pramod Bajarang Vhankade, “Design and Manufacturing of Vortex Tube “ ,International Journal of Science and Research (IJSR) ISSN (Online): 2319-7064 2015 [2] Nitin V Galwade, Prof. Tushar Koli, Prof. Sayyad L.B, “Design and Fabrication of Vortex Tube“ International Journal of Scientific & Engineering Research Volume9,Issue 3, 56 ISSN 2229-5518 March 2018
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 07 | July 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 2364 [3] U. V. Kongre, M. D. Kurve, P. R Angaitkar, S. R. Ade, “Design and analysis of vortex tube refrigeration”, International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056Volume:05Issue:04 | www.irjet.net p-ISSN: 2395-0072 , IRJET Apr-2018 [4] U. V. Kongre, M. V. Dudhe, A. N. Petkar, V. S. Kamble ,S. M. Kamble , “Investigation of vortex tube refrigeration with novel material “ , © IJCRT | Volume 6 | ISSN: 2320-2882 2018 [5] Dhruv Manilawala , Saurav Koul , KiranMarudwar,Keval Oswal, “Design, Manufacturing and Testing of Vortex Tube”, International Journal of Future Generation Communication and Networking Vol. 13, No. 2s, (2020) [6] Mustafa Abdulhussain “A review on the vortex tube geometrical affecting parameters”Journal ofMechanical and Energy Engineering, Vol. 4(44), No. 1, 2020 [7] F. P. Branco, E. D. Buchelt, F. M. Barbosa, B. P.Rosa,andD. J. Laporte “Design And Study Of Dimensional Parameters Influence On Vortex Tube Behavior”Universidade Católica Dom Bosco Departamento de Engenharia Mecânica Bairro Jardim Seminário CP. 79117-900, Campo Grande, MS, Brasil [8] Upendra Behera a , P.J. Paul a , S. Kasthurirengan b , R. Karunanithi b , S.N. Ram b , K. Dinesh b , S. Jacob “CFD analysis andexperimental investigationstowardsoptimizing the parameters of Ranque–Hilsch vortex tube“ Department of Aerospace Engineering, Indian Institute of Science, Bangalore 560 012, India [9] Penka Zlateva. Krystin Yordanov, diyan M. Dimitrov “Numerical simulation of temperature separation phenomena inside vortex tube” technical university of Varna, Dep. Heat Engineering, Bulgaria ,2014 [10] Wasan Naksanee, Rathassak Prommas ” An Experimental Investigation to Reduce the Temperature of Hot Air by means of a Vortex Tubefed with Low Inlet Air Pressure and a Specific Snail Nozzle Geometry Article in International Journal of Engine” International Journal of Engineering and Technology · June 2018