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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1665
DEVELOPMENT OF A MODIFIED TESLA TURBINE
Palle Anirudh1, Shashank D. L.2
1Graduate, Dept. of Mechanical Engineering, Institute of Aeronautical Engineering, Telangana, India
2Graduate, Dept. of Mechanical Engineering, CVSR College of Engineering, Telangana, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - Modern history is adorned with alotofmachines
working in modified Rankine or Brayton cycle using the
principle of lift producing devices fixed to a rotor system. The
inception of a bladeless unit fixed to a rotor which follows the
principle of cohesion between the interactive medium of a
finite surface and infinite fluid was done by Nikola Tesla in the
early parts of the 19th century [12]. Usageofbladelessturbines
has a physical advantage of ease of production with less cost
making it a cost-efficient process in both mechanical and
thermal platforms. Further, interactionofthesurfaceandfluid
is subjected to the boundary layer interaction between them.
The efficiency of said systems are considerably higher in high
RPM’s where the surface interaction is conscripted. Thepower
loss occurs due to less surface interaction and significantly
lower RPM’s.
Key Words: Cohesion, Boundary Layer Interactions,
Surface Interactions, Rotor, Bladeless unit
1. INTRODUCTION
Tesla turbine also called as a bladeless turbine or a friction
turbine is an alternative to the traditional bladed turbine
that uses conventional energy such as fossil fuels, ignition
fuels transferring it onto the surface of the blades for power
production. Unlike the traditional method, one of a kind
innovative idea about the bladeless turbine called as Tesla
turbine was put forth by Nikola Tesla throughhispatent ‘The
Tesla turbine’ in 1913 [12].
Tesla turbine is a distinctive type of turbomachinery which
makes use of smooth disks instead of blades. The main
principle behind the working of Tesla turbine are the
properties of physics: Adhesion and Viscosity. As a contrast
to the traditional bladed turbine where the properties of
cohesion and adhesion produces an unenviable effecton the
efficiency of the turbine, they allow an efficient rotation of
the rotor in the Tesla turbine.
As the fluid is passed through a nozzle ontothesurfaceof the
disk the first layer of the fluid acts on the surface through
viscosity to cause the movement of the rotor called the
boundary layer effect and as the rotation takes place the
fluid loses energy thereby getting sucked into the exhaust
holes. The fluid in this experiment is compressed air sent
through the nozzle with high velocity where it swirls onto
the dimples present on the surface enabling the disk to
rotate as different from the bladed turbine where thefluid is
forced to impinge on the profile of the blade.
2. BACKGROUND STUDY
With an increase in the harmful means of energy production
and uses of polluting fluids invention of Tesla turbine paved
a path towards an effective low energy generation at lower
costs and easy manufacturing. Tesla turbine finds its
application not only in power generation for household
needs but also can be used to tap geothermal energy from
underground salt-brine all over the world [9].
In the disk turbine any relative velocityofthefluidfora fixed
inlet pressure across the disk causes a viscous drag force
that accelerates the rotor increasing the angular speed and
decreasing the viscous drag [1]. The torque calculated from
the experimentation decreases with increasing angular
speed and the output power, efficiency initially increases
with increasing angular speed before they reach maximum
[1]. Comparison of the performances has been illustrated
between the Tesla turbine and thebladelessturbinewhereit
is shown that the performance of one is inversely
proportional to other and each has a certain point beyond
which a switch over between the two is sought [2].
Investigation on rotor disc surface, performance was done
and came to an inference that the disc roughness equal to
0.28 indicated a smooth surface and the roughness equal to
below the indicated value did not result in any shear stress
generation whereas the maximum power generation were
obtained at 3 and 4 bar respectively equal to 42.5W and
71.5W [4]. For more effective momentumtransferfromfluid
to the disk and efficient rotation of the disks the flow should
be laminar [3].
Apart from using compressed air as a fluid working
characteristics and systematic flowbehaviorinsidetherotor
channels was studied using three organic fluids R404a,
R134a, R245fa where they show same efficiency tendency
and the performance of R245fa slightly undergoes R134a
due to lower critical pressure [5]. Designs for different
nozzle types have been made through 3-D plastic rapid
prototyping to explore the performance degradation in
turbines due to nozzle impedance mismatch and reveal that
with increase in the fractional volume of nano particle there
is a pressure drop in the radial direction and tangential
velocity at any point inside the computational domain tends
to increase [6].
Development of a Tesla turbine as a green energy
generator for household purposes such as to generate
electricity using water supply from tap without significant
head loss is an effective way to convert excessive energy
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1666
without disrupting the supply of water [7]. In order to attain
higher rotor efficiency, the quantity of water flow rate must
be made as low as possible that means a greater number of
disks and larger rotor [7]. The highest value of efficiency
appears when the distance or gap between the disksismade
minimum or approximately equal to the double boundary
layer thickness [11].
3. FABRICATION AND SET-UP
The bladeless turbine in the current analysis has been
slightly modified for increasing the effect of boundary layer
and principle of cohesion to work on the dimples of the
surface plate. As illustrated in Fig. 2, disks of 10cm diameter
with a series of variable depth dimples have been arranged
on the periphery of the disk in a slow radial and angular
schema against the direction of flow. Six exhaust holes of
diameter 4mm have been fabricatedaround thecenterofthe
plate at a distance of 18mm from the center with the help of
portable drilling machine.
Fig -1: 3-D model of shaft with 6 internally threaded holes.
Fig -2: 3-D model of disc with Dimples on the periphery.
Three spacers of 2.2mm thickness are placed between the
disks for increasing the cohesion of fluid flow over the space.
As shown in Fig. 1, we have managed to design and fabricate
a shaft with the steps of variable diameter 10mm, 33mm,
25mm, along the respective lengths with six 3mm internally
threaded holes on the side of the shaft for joining the lock
plate.
The lock plate is mounted on either side of the shaft for
stationary and stable movement of the disks without any
causes forvibration. The inlet chamber fixedontheL-shaped
cut made on the casing acts as a fluid inlet at high pressure
and velocity giving maximum adhesion to the disk surface
finally generating a maximum boundary layer. The whole
assembly is being held by two 9mm thick acrylic
thermoplastic sheet as a casing cover joined to the lock plate
by screws.
Fig -3: 3-D model of inlet chamber with fluid inlet at center.
Fig -4: 3-D model of casing with L-shaped cut section.
Fig -5: Fabricated Disc with Dimples.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1667
Fig -6: Fabricated casing with an L- shaped cut section.
Fig -7: Fabricated Inlet Chamber with fluid inlet at center.
4. PRINCIPLE OF WORKING
The fluid adherence to the wall of the disk caused by the
viscosity and turbulence of fluid give rise to shearstressthat
enables the disks to rotate. Tesla turbine consists of a series
of disks arranged in the pattern of an array onto a shaft with
the help of bearings that restrict the axial and vertical
movement of disks enabling only 2 degrees of freedom that
is the rotational movement in clockwise and anticlockwise
direction.
All this setup is housed in a casing provided with nozzles
that supplies high speed moving fluid and in case of this
experiment it is compressed air which is nearlytangential to
the rotor. As the fluid flows spirally onto the disks and
dimples creating a boundary layer effectduetoviscosityand
turbulence, it allows the rotor to rotate and further rotating
the shaft at higher RPM’s and slowly when the fluid had lost
its energy it exhausts through the exhaust holesprovided on
the disks near the shaft.
In this series of actions, the fluid slows down adding energy
to the disks causing the motion before it finally spirals
through the holes. As the fluid is injected tangentially the
component of velocity vector is zero for the referencesystem
corresponding to the disk surface so the only velocity
component seen is towards the center of the disk which
forces it through the discharge such that it looks likethefluid
is spiraling around the disk before it discharges out.
5. RESULTS AND DISCUSSION
Discs with dimples of various sizes ononesideofthediscare
made and are compared with the results of those without
dimples. It has been found that at a nominal inletpressure of
5 bar the plates with dimples rotate at 13448 RPM whereas
the plates without dimples rotate at 12000 RPM which
proves that the increment of total surface area of the fluid
adhesion by creating dimples during boundary flow has a
better effectiveness compared to that of a flat surface plate
without any dimples.
Table -1: Table shows the variations in Speed, Power and
Torque with respect to pressure for disks with dimples.
PRESSURE SPEED
(RPM)
POWER TORQUE
1 3500 48.963 0.13359
2 7500 209.842 0.26718
3 9500 398.711 0.40078
4 11400 637.945 0.53438
5 13448 979.301 0.66798
Table -2: Table shows the variations in Speed, Power and
Torque with respect to pressure for disks without dimple.
PRESSURE SPEED
(RPM)
POWER TORQUE
1 4500 62.95 0.13359
2 6000 167.874 0.26718
3 8000 335.756 0.40078
4 10000 559.601 0.53438
5 12000 839.400 0.66798
As a comparison between table 1 and table2itisclearlyseen
that modified disk with the dimples on the surface enhances
the speed of rotation as the pressure is increased from 1 bar
to 5 bar and so is the power generated that is obtained with
dimples at 5 bar pressure and 14000 rpm is more when
compared to power generated at 5bar pressure and 12000
rpm. Further clarity of the above deductions can be seen in
the graphs below.
Chart -1: Distribution of Power with respect to Torque as
L1 represents line for disk with dimples and L2 represents
line for disk without dimples.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1668
Chart -2: Distribution of Speed with respect to Torque as
L1 represents the line for disk with dimples and L2
represents the line for disk without dimples.
Chart -3: Distribution of Speed with respect to Power as
L1 represents the line for disk with dimples and L2 as a
line for disk without dimples.
6. CONCLUSION
The experimental analysis and a comparative study on
bladeless turbines with and without changes in the profile
and topography have been done and the following
conclusions have been achieved. The current investigation
proposes to promote the boundary interaction between the
surface and the fluid by multiple optimized techniques. An
experimental setup is also proposed to verify the claim of
higher surface interactions. It is estimated thatduetohigher
boundary interaction between surface and fluid the rate of
power production might increase as a function of torque
produced in the system under variable parameters of
pressure, velocity and density. For low inlet pressure,
around the range of 1 bar-2 bar (gauge). The bladeless
turbine without any enhancements rotate at higher RPM. As
the physics transits to compressibleflow,thespeedandRPM
recorded for the enhanced plates are higher compared to
that of the non-modified plates. Numerical analysis hasbeen
done and the results are validated by cross referring with
practical experimental values. It has been found that the
theoretical value has an error percentage of around3-5% in
comparison with the experimental value, which is normal in
nature.
REFERENCES
[1] Hoya G.P. & Guha A, “The design of a test rig and study of
the performance and efficiency of a Tesla disc turbine”,
Proceedings of the Institution of Mechanical Engineers,
Part A: Journal of Power and Energy, Vol. 223, 2009.
[2] Harikishan Gupta E., Shyam P. Kodali, “Design and
Operation of Tesla Turbomachine- A state of the Art
Review”, International Journal of Advanced Transport
Phenomena, Vol. 02, No. 01, pp 7-14, 2013.
[3] H.S. Couto, J.B.F. Duate & D. Bastos-Netto, “The Tesla
Turbine Revisited”, Proceedings of 8th Asia-Pacific
International Symposium on Combustion and Energy
Utilization, Oct 10-12, 2006.
[4] K. Rusin, W. Wroblewski & M. Strozik, Experimental and
Numerical Investigation on Tesla Turbine, Proceedings of
XXIII Fluid Mechanics Conference (KKMP 2018)
[5] L. Ciappi, D. Fiaschi, P. Niknam, L. Talluri
“Computational Investigation of Flow Inside a Tesla
Turbine Motor”, Journal of Energy, 2019, DOI:
https://doi.org/10.1016/j.energy.2019.01.158.
[6] Nikhil Bankar, Anil Chavan, Sanket Dhole, Prashant
Patunkar “Development of Hybrid Tesla Turbine and
Current Trends in Application of Tesla Turbine”,
International Journal of Technological Research in
Engineering, Vol. 3, Issue 7, 2016.
[7] S.J. Foo, W.C. Tan & M. Shahril, “Development of Tesla
Turbine for Green Energy Application”, Proceedings of
National Conference of Mechanical Engineering Research
and Post Graduate Studies (2nd NCMER 2010).
[8] Tamir A. Emran, Ryan C. Alexander, Chris T. Stallings,
Mark A. DeMay, Matthew J. Traum “Method to Accurately
Estimate Tesla Turbine Stall Torque for Dynamometer or
Generator Load Selection”, Proceedings of ASME Early
Career Technical Conference, ASME ECTC, 2010, ASME
Early Career Technical Journal.
[9] V. Carey “Assessment of Tesla Turbine Performancefor
Small Scale Rankine Combined Heat and Power Systems”,
Journal of Engineering for Gas Turbines and
Power132(12), 2010.
[10] Warren Rice “An Analytical and Experimental
Investigation of Multiple Disk Turbine”, Journal of
Engineering for Gas Turbines and Power, Vol. 87, Issue 1,
1965.
[11] Warren Rice “Tesla Turbomachinery”, Proceedings of
IV International Nikola Tesla Symposium, 1991.
[12] U.S Patent 1,061,206 (1913).

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IRJET- Development of a Modified Tesla Turbine

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1665 DEVELOPMENT OF A MODIFIED TESLA TURBINE Palle Anirudh1, Shashank D. L.2 1Graduate, Dept. of Mechanical Engineering, Institute of Aeronautical Engineering, Telangana, India 2Graduate, Dept. of Mechanical Engineering, CVSR College of Engineering, Telangana, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - Modern history is adorned with alotofmachines working in modified Rankine or Brayton cycle using the principle of lift producing devices fixed to a rotor system. The inception of a bladeless unit fixed to a rotor which follows the principle of cohesion between the interactive medium of a finite surface and infinite fluid was done by Nikola Tesla in the early parts of the 19th century [12]. Usageofbladelessturbines has a physical advantage of ease of production with less cost making it a cost-efficient process in both mechanical and thermal platforms. Further, interactionofthesurfaceandfluid is subjected to the boundary layer interaction between them. The efficiency of said systems are considerably higher in high RPM’s where the surface interaction is conscripted. Thepower loss occurs due to less surface interaction and significantly lower RPM’s. Key Words: Cohesion, Boundary Layer Interactions, Surface Interactions, Rotor, Bladeless unit 1. INTRODUCTION Tesla turbine also called as a bladeless turbine or a friction turbine is an alternative to the traditional bladed turbine that uses conventional energy such as fossil fuels, ignition fuels transferring it onto the surface of the blades for power production. Unlike the traditional method, one of a kind innovative idea about the bladeless turbine called as Tesla turbine was put forth by Nikola Tesla throughhispatent ‘The Tesla turbine’ in 1913 [12]. Tesla turbine is a distinctive type of turbomachinery which makes use of smooth disks instead of blades. The main principle behind the working of Tesla turbine are the properties of physics: Adhesion and Viscosity. As a contrast to the traditional bladed turbine where the properties of cohesion and adhesion produces an unenviable effecton the efficiency of the turbine, they allow an efficient rotation of the rotor in the Tesla turbine. As the fluid is passed through a nozzle ontothesurfaceof the disk the first layer of the fluid acts on the surface through viscosity to cause the movement of the rotor called the boundary layer effect and as the rotation takes place the fluid loses energy thereby getting sucked into the exhaust holes. The fluid in this experiment is compressed air sent through the nozzle with high velocity where it swirls onto the dimples present on the surface enabling the disk to rotate as different from the bladed turbine where thefluid is forced to impinge on the profile of the blade. 2. BACKGROUND STUDY With an increase in the harmful means of energy production and uses of polluting fluids invention of Tesla turbine paved a path towards an effective low energy generation at lower costs and easy manufacturing. Tesla turbine finds its application not only in power generation for household needs but also can be used to tap geothermal energy from underground salt-brine all over the world [9]. In the disk turbine any relative velocityofthefluidfora fixed inlet pressure across the disk causes a viscous drag force that accelerates the rotor increasing the angular speed and decreasing the viscous drag [1]. The torque calculated from the experimentation decreases with increasing angular speed and the output power, efficiency initially increases with increasing angular speed before they reach maximum [1]. Comparison of the performances has been illustrated between the Tesla turbine and thebladelessturbinewhereit is shown that the performance of one is inversely proportional to other and each has a certain point beyond which a switch over between the two is sought [2]. Investigation on rotor disc surface, performance was done and came to an inference that the disc roughness equal to 0.28 indicated a smooth surface and the roughness equal to below the indicated value did not result in any shear stress generation whereas the maximum power generation were obtained at 3 and 4 bar respectively equal to 42.5W and 71.5W [4]. For more effective momentumtransferfromfluid to the disk and efficient rotation of the disks the flow should be laminar [3]. Apart from using compressed air as a fluid working characteristics and systematic flowbehaviorinsidetherotor channels was studied using three organic fluids R404a, R134a, R245fa where they show same efficiency tendency and the performance of R245fa slightly undergoes R134a due to lower critical pressure [5]. Designs for different nozzle types have been made through 3-D plastic rapid prototyping to explore the performance degradation in turbines due to nozzle impedance mismatch and reveal that with increase in the fractional volume of nano particle there is a pressure drop in the radial direction and tangential velocity at any point inside the computational domain tends to increase [6]. Development of a Tesla turbine as a green energy generator for household purposes such as to generate electricity using water supply from tap without significant head loss is an effective way to convert excessive energy
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1666 without disrupting the supply of water [7]. In order to attain higher rotor efficiency, the quantity of water flow rate must be made as low as possible that means a greater number of disks and larger rotor [7]. The highest value of efficiency appears when the distance or gap between the disksismade minimum or approximately equal to the double boundary layer thickness [11]. 3. FABRICATION AND SET-UP The bladeless turbine in the current analysis has been slightly modified for increasing the effect of boundary layer and principle of cohesion to work on the dimples of the surface plate. As illustrated in Fig. 2, disks of 10cm diameter with a series of variable depth dimples have been arranged on the periphery of the disk in a slow radial and angular schema against the direction of flow. Six exhaust holes of diameter 4mm have been fabricatedaround thecenterofthe plate at a distance of 18mm from the center with the help of portable drilling machine. Fig -1: 3-D model of shaft with 6 internally threaded holes. Fig -2: 3-D model of disc with Dimples on the periphery. Three spacers of 2.2mm thickness are placed between the disks for increasing the cohesion of fluid flow over the space. As shown in Fig. 1, we have managed to design and fabricate a shaft with the steps of variable diameter 10mm, 33mm, 25mm, along the respective lengths with six 3mm internally threaded holes on the side of the shaft for joining the lock plate. The lock plate is mounted on either side of the shaft for stationary and stable movement of the disks without any causes forvibration. The inlet chamber fixedontheL-shaped cut made on the casing acts as a fluid inlet at high pressure and velocity giving maximum adhesion to the disk surface finally generating a maximum boundary layer. The whole assembly is being held by two 9mm thick acrylic thermoplastic sheet as a casing cover joined to the lock plate by screws. Fig -3: 3-D model of inlet chamber with fluid inlet at center. Fig -4: 3-D model of casing with L-shaped cut section. Fig -5: Fabricated Disc with Dimples.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1667 Fig -6: Fabricated casing with an L- shaped cut section. Fig -7: Fabricated Inlet Chamber with fluid inlet at center. 4. PRINCIPLE OF WORKING The fluid adherence to the wall of the disk caused by the viscosity and turbulence of fluid give rise to shearstressthat enables the disks to rotate. Tesla turbine consists of a series of disks arranged in the pattern of an array onto a shaft with the help of bearings that restrict the axial and vertical movement of disks enabling only 2 degrees of freedom that is the rotational movement in clockwise and anticlockwise direction. All this setup is housed in a casing provided with nozzles that supplies high speed moving fluid and in case of this experiment it is compressed air which is nearlytangential to the rotor. As the fluid flows spirally onto the disks and dimples creating a boundary layer effectduetoviscosityand turbulence, it allows the rotor to rotate and further rotating the shaft at higher RPM’s and slowly when the fluid had lost its energy it exhausts through the exhaust holesprovided on the disks near the shaft. In this series of actions, the fluid slows down adding energy to the disks causing the motion before it finally spirals through the holes. As the fluid is injected tangentially the component of velocity vector is zero for the referencesystem corresponding to the disk surface so the only velocity component seen is towards the center of the disk which forces it through the discharge such that it looks likethefluid is spiraling around the disk before it discharges out. 5. RESULTS AND DISCUSSION Discs with dimples of various sizes ononesideofthediscare made and are compared with the results of those without dimples. It has been found that at a nominal inletpressure of 5 bar the plates with dimples rotate at 13448 RPM whereas the plates without dimples rotate at 12000 RPM which proves that the increment of total surface area of the fluid adhesion by creating dimples during boundary flow has a better effectiveness compared to that of a flat surface plate without any dimples. Table -1: Table shows the variations in Speed, Power and Torque with respect to pressure for disks with dimples. PRESSURE SPEED (RPM) POWER TORQUE 1 3500 48.963 0.13359 2 7500 209.842 0.26718 3 9500 398.711 0.40078 4 11400 637.945 0.53438 5 13448 979.301 0.66798 Table -2: Table shows the variations in Speed, Power and Torque with respect to pressure for disks without dimple. PRESSURE SPEED (RPM) POWER TORQUE 1 4500 62.95 0.13359 2 6000 167.874 0.26718 3 8000 335.756 0.40078 4 10000 559.601 0.53438 5 12000 839.400 0.66798 As a comparison between table 1 and table2itisclearlyseen that modified disk with the dimples on the surface enhances the speed of rotation as the pressure is increased from 1 bar to 5 bar and so is the power generated that is obtained with dimples at 5 bar pressure and 14000 rpm is more when compared to power generated at 5bar pressure and 12000 rpm. Further clarity of the above deductions can be seen in the graphs below. Chart -1: Distribution of Power with respect to Torque as L1 represents line for disk with dimples and L2 represents line for disk without dimples.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1668 Chart -2: Distribution of Speed with respect to Torque as L1 represents the line for disk with dimples and L2 represents the line for disk without dimples. Chart -3: Distribution of Speed with respect to Power as L1 represents the line for disk with dimples and L2 as a line for disk without dimples. 6. CONCLUSION The experimental analysis and a comparative study on bladeless turbines with and without changes in the profile and topography have been done and the following conclusions have been achieved. The current investigation proposes to promote the boundary interaction between the surface and the fluid by multiple optimized techniques. An experimental setup is also proposed to verify the claim of higher surface interactions. It is estimated thatduetohigher boundary interaction between surface and fluid the rate of power production might increase as a function of torque produced in the system under variable parameters of pressure, velocity and density. For low inlet pressure, around the range of 1 bar-2 bar (gauge). The bladeless turbine without any enhancements rotate at higher RPM. As the physics transits to compressibleflow,thespeedandRPM recorded for the enhanced plates are higher compared to that of the non-modified plates. Numerical analysis hasbeen done and the results are validated by cross referring with practical experimental values. It has been found that the theoretical value has an error percentage of around3-5% in comparison with the experimental value, which is normal in nature. REFERENCES [1] Hoya G.P. & Guha A, “The design of a test rig and study of the performance and efficiency of a Tesla disc turbine”, Proceedings of the Institution of Mechanical Engineers, Part A: Journal of Power and Energy, Vol. 223, 2009. [2] Harikishan Gupta E., Shyam P. Kodali, “Design and Operation of Tesla Turbomachine- A state of the Art Review”, International Journal of Advanced Transport Phenomena, Vol. 02, No. 01, pp 7-14, 2013. [3] H.S. Couto, J.B.F. Duate & D. Bastos-Netto, “The Tesla Turbine Revisited”, Proceedings of 8th Asia-Pacific International Symposium on Combustion and Energy Utilization, Oct 10-12, 2006. [4] K. Rusin, W. Wroblewski & M. Strozik, Experimental and Numerical Investigation on Tesla Turbine, Proceedings of XXIII Fluid Mechanics Conference (KKMP 2018) [5] L. Ciappi, D. Fiaschi, P. Niknam, L. Talluri “Computational Investigation of Flow Inside a Tesla Turbine Motor”, Journal of Energy, 2019, DOI: https://doi.org/10.1016/j.energy.2019.01.158. [6] Nikhil Bankar, Anil Chavan, Sanket Dhole, Prashant Patunkar “Development of Hybrid Tesla Turbine and Current Trends in Application of Tesla Turbine”, International Journal of Technological Research in Engineering, Vol. 3, Issue 7, 2016. [7] S.J. Foo, W.C. Tan & M. Shahril, “Development of Tesla Turbine for Green Energy Application”, Proceedings of National Conference of Mechanical Engineering Research and Post Graduate Studies (2nd NCMER 2010). [8] Tamir A. Emran, Ryan C. Alexander, Chris T. Stallings, Mark A. DeMay, Matthew J. Traum “Method to Accurately Estimate Tesla Turbine Stall Torque for Dynamometer or Generator Load Selection”, Proceedings of ASME Early Career Technical Conference, ASME ECTC, 2010, ASME Early Career Technical Journal. [9] V. Carey “Assessment of Tesla Turbine Performancefor Small Scale Rankine Combined Heat and Power Systems”, Journal of Engineering for Gas Turbines and Power132(12), 2010. [10] Warren Rice “An Analytical and Experimental Investigation of Multiple Disk Turbine”, Journal of Engineering for Gas Turbines and Power, Vol. 87, Issue 1, 1965. [11] Warren Rice “Tesla Turbomachinery”, Proceedings of IV International Nikola Tesla Symposium, 1991. [12] U.S Patent 1,061,206 (1913).