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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume 3 Issue 5, August 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470
@ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 473
Design Calculation of 1200W Horizontal Axis
Wind Turbine Blade for Rural Applications
Zin Mar Chan
Lecturer, Mechanical Engineering Department Technological University, Mandalay, Myanmar
How to cite this paper: Zin Mar Chan
"Design Calculation of 1200W Horizontal
Axis Wind Turbine Blade for Rural
Applications"
Published in
InternationalJournal
of Trend in Scientific
Research and
Development
(ijtsrd), ISSN: 2456-
6470, Volume-3 |
Issue-5, August 2019, pp.473-475,
https://doi.org/10.31142/ijtsrd25328
Copyright © 2019 by author(s) and
International Journalof Trendin Scientific
Research and Development Journal. This
is an Open Access article distributed
under the terms of
the Creative
CommonsAttribution
License (CC BY 4.0)
(http://creativecommons.org/licenses/by
/4.0)
ABSTRACT
This paper provides to design 1200W horizontal axis wind turbine blade for
rural application. The rotor blade is designtoproduce1200W power outputin
order to install at Mandalay Hill of Mandalay City in Myanmar at rated wind
velocity 7 m/s. The rotor diameter is 2.303m and tip speed ratio is 5. The
design process includes the determination of the blade airfoil, pitch angle and
chord length distribution along the blade span. By usingbladeelementtheory,
blade is divided into 10 elements with equal length forming 11 sections
throughout the blade. This paper is intended for commercial wind turbine in
rural applications. The wind generator can produce 1200W at wind velocity7
m/s. The use of wind energy for electricity is more economical than the
conventional electricitygeneration.Itisstronglyrecommendedthatthedesign
prototype is economic and competitive for commercialization at any windy
places in Myanmar.
KEYWORDS: wind turbine blade, blade element theory and commercial wind
turbine
I. INTRODUCTION
The wind is essentially air in motion, carrieswithitskineticenergy.Theamount
of energy contained in the wind at any given instant is proportional to the wind
speed at that instant. The temperature of the wind also influences the energy
content of the wind but is not important in the content of wind based energy
production system.
Winds are generated due to the atmospheric temperature
differences caused by different areas getting differentfluxes
of sunlight. Air mass tends to move from hotter to the cooler
regions, there by generating winds.Inturn,windmovements
cause atmospheric pressure differentials which lead to
turbulence and more winds.
A wind turbine is a device that converts kinetic energy from
the wind, also called wind energy, into mechanical energy in
a process known as wind power [2]. Wind turbines are
classified into two categories, according to the direction of
their rotational axis: Horizontal Axis Wind Turbine (HAWT)
and Vertical Axis Wind Turbine (VAWT). Horizontal Axis
Wind Turbines capture kinetic wind energy with a propeller
type rotor and their rotational axis is parallelto thedirection
of the wind. Vertical Axis Wind Turbines use straight or
curved bladed rotors with rotatingaxesperpendiculartothe
wind stream. They can capture wind from any direction [5].
A wind turbine consists of several main parts: the rotor,
generator, driven chain, control system and so on. The rotor
is driven by the wind and rotates at predefined speed in
terms of the wind speed, so that the generator can produce
electric energy output under the regulation of the control
system [3]. The wind turbine blade is a very important part
of the rotor. Extraction of energy from wind depends on the
design of blade [4]. In order to extract the maximum kinetic
energy from wind, researchers put much efforts on the
design of effective blade geometry [3].
Although the design procedure of the blade is different from
each designing and manufacturing company, the common
procedures are performing aerodynamic configuration
design, dynamic and static load analyses, structural design,
securing structural strength through static stress analysis,
prediction of fatigue life from the random load spectrum and
the modal analysis to prevent the resonance in order.
The following figure_1 shows main components of Small
Horizontal Axis Wind Turbine [6].
Figure1. Main Components of Small Horizontal Axis
Wind Turbine
II. MATERIAL AND METHOD
In this research, turbine blade is made of glass reinforced
plastic material. Number of blade mounted on rotor are 3
blades. So, choose the design tip-speed ratio to 5.One
IJTSRD25328
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 474
important factor that affects the power coefficients is the
drag. Drag affects the expected power coefficient via the
CD/CL ratio. For collection of maximum power coefficient, a
range of design speed ratio 1 ≤ λ ≤ 10 the theoretically
attainable power coefficient lie between 0.35 ≤ Cpmax ≤ 0.5,
then get the value of Cp to 0.4861.
In this research, like blade material of glass reinforce plastic,
high speed design of NACA 4412 airfoil was used, which can
give very good results in angle of attack.
III. DESIGN CONSIDERATION OF WIND TURBINE
BLADE
In design calculation of blade, consider the tower weight
depending on the basics of the roughness of the terrain. The
site location of turbine is Mandalay Hillof MandalayDivision
in Myanmar at 240m from the sea level. So the total height
for 5m tower height from sea level at Mandalay Hill is
245m.The most physical feature of Mandalay is 64m from
the sea level. Specification data to design wind turbineblade
are shown in Table 1.
Table1. Specification Data for Wind Turbine Blade
Description Symbol Value Unit
average wind speed Vavg 2.4 m/s
reference height from sea
level for Mandalay
Havg 64 m
total height from sea level H 245 m
power output P 1200 W
system efficiency E 0.35 -
density of air ρ 1.2 kg/m3
assumed turbine efficiency ηt 0.8 -
generator efficiency ηg 0.9 -
no; of blade B 3 -
lift coefficient CL 1.1725 -
Calculation of rotor diameter,
δ
avg
avg
H
H
VV








= (1)
Vrated = 2 V (2)
gpr
e
ηCρv
2P
A 3= (3)
π
A4
D
×
= (4)
Table2. Selection of Rotor Diameter
E Cp A d
0.3 0.4166 19.44 4.97
0.31 0.4305 18.81 4.89
0.32 0.4444 18.22 4.81
0.33 0.4583 17.66 4.74
0.34 0.4722 17.15 4.67
0.35 0.4861 16.66 4.6
Calculation of tip speed ratio in each section,
R
r
λλ i
i ×= (5)
Where,
R = rotor radius
λ = design tip-speed ratio
Table3. Selection of Number of Blade
λ 1 2 3 4 5-8 8-15
B 6-20 4-12 3-6 2-4 2-3 1-2
Calculation of blade chord length,
BC
SPr
c
L
i
i
×
×
= (6)
Where,
SP = shape parameters at each section
B = no. of blade
CL = lift coefficient
Calculation of blade pitch angle of each section,
]
λ
1
3
2
[tanΦ
i
1
i ×= − (7)
dii αΦβ −= (8)
Where, αd = angle of attack
iΦ = Incident Angle
Calculation of linearization blade chord length,
0.1083r0.0705c ii +−= (9)
Where, ri = radius of blade element
Calculation of linearization blade pitch angle of eachsection,
18.687422.4142rβ ii +−= (10)
Table4. Results of Blade Chord, Incident Angle and Pitch Angle at each Section of NACA 4412
Cross Section No.
Radius of Blade Element,
ri
TSR,
λi
Chord Length,
ci
Incident Angle,
iΦ
Pitch Angle,
iβ
1 0.06 0.130 0.062 79 72.162
2 0.284 0.617 0.291 47 40.164
3 0.509 1.105 0.522 31.1 24.26
4 0.733 1.591 0.376 22.7 15.86
5 0.954 2.078 0.337 17.8 10.96
6 1.181 2.564 0.303 14.6 7.76
7 1.406 3.053 0.270 12.3 5.46
8 1.630 3.539 0.261 10.7 3.86
9 1.854 4.025 0.238 9.41 2.57
10 2.078 4.513 0.200 8.41 1.57
11 2.303 5.000 0.162 7.595 0.757
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 475
Table5. Results Data for Linearization of Blade Chords
Cross Section No. r(m) C(m)exact C(mm) Linearization Deviation (mm)
1 0,06 .062 431.4 -369
2 0.284 .291 406 -115
3 0.509 .522 380 142
4 0.733 .376 354 22
5 0.954 .337 329 8
6 1.181 .303 303 0
7 1.406 .270 277 -7
8 1.630 .261 251 10
9 1.854 .238 226 12
10 2.078 .2 200 0
11 2.303 .162 174 -12
Table6. Results Data for Linearization of Blade Angles
Cross Section No. r(m) (Deg) exact (Deg) Linearization Deviation (mm)
1 0.06 72.162 32.4286 39.733
2 0.284 40.162 28.354 11.808
3 0.509 24.26 24.261 0
4 0.733 15.86 20.186 -4.326
5 0.957 10.96 16.112 -5.152
6 1.181 7.762 12.037 -4.275
7 1.406 5.46 7.944 -2.484
8 1.630 3.86 3.870 0
9 1.854 2.57 -0.204 2.774
10 2.078 1.57 -4.278 5.843
11 2.303 0.757 -8.372 9.192
Figure2. Wind Turbine Blade design
IV. CONCLUSIONS
Turbine blades were designed based on Blade Element
Momentum theory. The wind generatorcanproduce1200W
at wind velocity 7m/s. To increase performance of the blade
design, the blade with NACA4412 airfoil is more suitable
than the others. NACA4412 is occurred at angle of attack 6°.
Cut-in speed (2 m/s) at which the wind turbine is allowed to
start revolving. Cut-out speed (20 m/s) at which the wind
turbine is allowed to deliver power due to safety precaution
at suitable wind speed.
V. ACKNOWLEDGEMENTS
The author is deeply grateful to Dr. Kyaw Aung, Professor
and Head of Mechanical Engineering Department,
Technological University (Mandalay) for his willingness to
share his ideas helpful suggestions on this paper writing.
VI. REFERENCES
[1] Wai Wai Phyo, Design Construction and Flow Analysis
of Horizontal Axis Wind Turbine Blade (400w),Master
Thesis, (2018).
[2] Navin, P., et al: Design and Development of Horizontal
Small Wind Turbine Blade for Low Wind Speeds,
International Journal of Engineering Science &
Advanced Technology, 4(1)(2014) PP 075-084
[3] Han, C.: Aerodynamic Analysis of Small HorizontalAxis
Wind Turbine Blades by Using 2D and 3D CFD
Modelling, (2011).
[4] Nitin, T., Mittal, N.D. and Siraj, A.: Design and Finite
Element Analysis of Horizontal Axis Wind Turbine
Blade, International Journal of Applied Engineering
Research, 1(3) (2010) PP 500-507.
[5] Ion, P., Wind Turbine Design, Internationals
Polytechnique, Canada, (2009).
[6] Danish Wind Industry Association: 1998-2002,
http://www.windpower.org

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Design Calculation of 1200W Horizontal Axis Wind Turbine Blade for Rural Applications

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume 3 Issue 5, August 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470 @ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 473 Design Calculation of 1200W Horizontal Axis Wind Turbine Blade for Rural Applications Zin Mar Chan Lecturer, Mechanical Engineering Department Technological University, Mandalay, Myanmar How to cite this paper: Zin Mar Chan "Design Calculation of 1200W Horizontal Axis Wind Turbine Blade for Rural Applications" Published in InternationalJournal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-3 | Issue-5, August 2019, pp.473-475, https://doi.org/10.31142/ijtsrd25328 Copyright © 2019 by author(s) and International Journalof Trendin Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative CommonsAttribution License (CC BY 4.0) (http://creativecommons.org/licenses/by /4.0) ABSTRACT This paper provides to design 1200W horizontal axis wind turbine blade for rural application. The rotor blade is designtoproduce1200W power outputin order to install at Mandalay Hill of Mandalay City in Myanmar at rated wind velocity 7 m/s. The rotor diameter is 2.303m and tip speed ratio is 5. The design process includes the determination of the blade airfoil, pitch angle and chord length distribution along the blade span. By usingbladeelementtheory, blade is divided into 10 elements with equal length forming 11 sections throughout the blade. This paper is intended for commercial wind turbine in rural applications. The wind generator can produce 1200W at wind velocity7 m/s. The use of wind energy for electricity is more economical than the conventional electricitygeneration.Itisstronglyrecommendedthatthedesign prototype is economic and competitive for commercialization at any windy places in Myanmar. KEYWORDS: wind turbine blade, blade element theory and commercial wind turbine I. INTRODUCTION The wind is essentially air in motion, carrieswithitskineticenergy.Theamount of energy contained in the wind at any given instant is proportional to the wind speed at that instant. The temperature of the wind also influences the energy content of the wind but is not important in the content of wind based energy production system. Winds are generated due to the atmospheric temperature differences caused by different areas getting differentfluxes of sunlight. Air mass tends to move from hotter to the cooler regions, there by generating winds.Inturn,windmovements cause atmospheric pressure differentials which lead to turbulence and more winds. A wind turbine is a device that converts kinetic energy from the wind, also called wind energy, into mechanical energy in a process known as wind power [2]. Wind turbines are classified into two categories, according to the direction of their rotational axis: Horizontal Axis Wind Turbine (HAWT) and Vertical Axis Wind Turbine (VAWT). Horizontal Axis Wind Turbines capture kinetic wind energy with a propeller type rotor and their rotational axis is parallelto thedirection of the wind. Vertical Axis Wind Turbines use straight or curved bladed rotors with rotatingaxesperpendiculartothe wind stream. They can capture wind from any direction [5]. A wind turbine consists of several main parts: the rotor, generator, driven chain, control system and so on. The rotor is driven by the wind and rotates at predefined speed in terms of the wind speed, so that the generator can produce electric energy output under the regulation of the control system [3]. The wind turbine blade is a very important part of the rotor. Extraction of energy from wind depends on the design of blade [4]. In order to extract the maximum kinetic energy from wind, researchers put much efforts on the design of effective blade geometry [3]. Although the design procedure of the blade is different from each designing and manufacturing company, the common procedures are performing aerodynamic configuration design, dynamic and static load analyses, structural design, securing structural strength through static stress analysis, prediction of fatigue life from the random load spectrum and the modal analysis to prevent the resonance in order. The following figure_1 shows main components of Small Horizontal Axis Wind Turbine [6]. Figure1. Main Components of Small Horizontal Axis Wind Turbine II. MATERIAL AND METHOD In this research, turbine blade is made of glass reinforced plastic material. Number of blade mounted on rotor are 3 blades. So, choose the design tip-speed ratio to 5.One IJTSRD25328
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 474 important factor that affects the power coefficients is the drag. Drag affects the expected power coefficient via the CD/CL ratio. For collection of maximum power coefficient, a range of design speed ratio 1 ≤ λ ≤ 10 the theoretically attainable power coefficient lie between 0.35 ≤ Cpmax ≤ 0.5, then get the value of Cp to 0.4861. In this research, like blade material of glass reinforce plastic, high speed design of NACA 4412 airfoil was used, which can give very good results in angle of attack. III. DESIGN CONSIDERATION OF WIND TURBINE BLADE In design calculation of blade, consider the tower weight depending on the basics of the roughness of the terrain. The site location of turbine is Mandalay Hillof MandalayDivision in Myanmar at 240m from the sea level. So the total height for 5m tower height from sea level at Mandalay Hill is 245m.The most physical feature of Mandalay is 64m from the sea level. Specification data to design wind turbineblade are shown in Table 1. Table1. Specification Data for Wind Turbine Blade Description Symbol Value Unit average wind speed Vavg 2.4 m/s reference height from sea level for Mandalay Havg 64 m total height from sea level H 245 m power output P 1200 W system efficiency E 0.35 - density of air ρ 1.2 kg/m3 assumed turbine efficiency ηt 0.8 - generator efficiency ηg 0.9 - no; of blade B 3 - lift coefficient CL 1.1725 - Calculation of rotor diameter, δ avg avg H H VV         = (1) Vrated = 2 V (2) gpr e ηCρv 2P A 3= (3) π A4 D × = (4) Table2. Selection of Rotor Diameter E Cp A d 0.3 0.4166 19.44 4.97 0.31 0.4305 18.81 4.89 0.32 0.4444 18.22 4.81 0.33 0.4583 17.66 4.74 0.34 0.4722 17.15 4.67 0.35 0.4861 16.66 4.6 Calculation of tip speed ratio in each section, R r λλ i i ×= (5) Where, R = rotor radius λ = design tip-speed ratio Table3. Selection of Number of Blade λ 1 2 3 4 5-8 8-15 B 6-20 4-12 3-6 2-4 2-3 1-2 Calculation of blade chord length, BC SPr c L i i × × = (6) Where, SP = shape parameters at each section B = no. of blade CL = lift coefficient Calculation of blade pitch angle of each section, ] λ 1 3 2 [tanΦ i 1 i ×= − (7) dii αΦβ −= (8) Where, αd = angle of attack iΦ = Incident Angle Calculation of linearization blade chord length, 0.1083r0.0705c ii +−= (9) Where, ri = radius of blade element Calculation of linearization blade pitch angle of eachsection, 18.687422.4142rβ ii +−= (10) Table4. Results of Blade Chord, Incident Angle and Pitch Angle at each Section of NACA 4412 Cross Section No. Radius of Blade Element, ri TSR, λi Chord Length, ci Incident Angle, iΦ Pitch Angle, iβ 1 0.06 0.130 0.062 79 72.162 2 0.284 0.617 0.291 47 40.164 3 0.509 1.105 0.522 31.1 24.26 4 0.733 1.591 0.376 22.7 15.86 5 0.954 2.078 0.337 17.8 10.96 6 1.181 2.564 0.303 14.6 7.76 7 1.406 3.053 0.270 12.3 5.46 8 1.630 3.539 0.261 10.7 3.86 9 1.854 4.025 0.238 9.41 2.57 10 2.078 4.513 0.200 8.41 1.57 11 2.303 5.000 0.162 7.595 0.757
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD25328 | Volume – 3 | Issue – 5 | July - August 2019 Page 475 Table5. Results Data for Linearization of Blade Chords Cross Section No. r(m) C(m)exact C(mm) Linearization Deviation (mm) 1 0,06 .062 431.4 -369 2 0.284 .291 406 -115 3 0.509 .522 380 142 4 0.733 .376 354 22 5 0.954 .337 329 8 6 1.181 .303 303 0 7 1.406 .270 277 -7 8 1.630 .261 251 10 9 1.854 .238 226 12 10 2.078 .2 200 0 11 2.303 .162 174 -12 Table6. Results Data for Linearization of Blade Angles Cross Section No. r(m) (Deg) exact (Deg) Linearization Deviation (mm) 1 0.06 72.162 32.4286 39.733 2 0.284 40.162 28.354 11.808 3 0.509 24.26 24.261 0 4 0.733 15.86 20.186 -4.326 5 0.957 10.96 16.112 -5.152 6 1.181 7.762 12.037 -4.275 7 1.406 5.46 7.944 -2.484 8 1.630 3.86 3.870 0 9 1.854 2.57 -0.204 2.774 10 2.078 1.57 -4.278 5.843 11 2.303 0.757 -8.372 9.192 Figure2. Wind Turbine Blade design IV. CONCLUSIONS Turbine blades were designed based on Blade Element Momentum theory. The wind generatorcanproduce1200W at wind velocity 7m/s. To increase performance of the blade design, the blade with NACA4412 airfoil is more suitable than the others. NACA4412 is occurred at angle of attack 6°. Cut-in speed (2 m/s) at which the wind turbine is allowed to start revolving. Cut-out speed (20 m/s) at which the wind turbine is allowed to deliver power due to safety precaution at suitable wind speed. V. ACKNOWLEDGEMENTS The author is deeply grateful to Dr. Kyaw Aung, Professor and Head of Mechanical Engineering Department, Technological University (Mandalay) for his willingness to share his ideas helpful suggestions on this paper writing. VI. REFERENCES [1] Wai Wai Phyo, Design Construction and Flow Analysis of Horizontal Axis Wind Turbine Blade (400w),Master Thesis, (2018). [2] Navin, P., et al: Design and Development of Horizontal Small Wind Turbine Blade for Low Wind Speeds, International Journal of Engineering Science & Advanced Technology, 4(1)(2014) PP 075-084 [3] Han, C.: Aerodynamic Analysis of Small HorizontalAxis Wind Turbine Blades by Using 2D and 3D CFD Modelling, (2011). [4] Nitin, T., Mittal, N.D. and Siraj, A.: Design and Finite Element Analysis of Horizontal Axis Wind Turbine Blade, International Journal of Applied Engineering Research, 1(3) (2010) PP 500-507. [5] Ion, P., Wind Turbine Design, Internationals Polytechnique, Canada, (2009). [6] Danish Wind Industry Association: 1998-2002, http://www.windpower.org