Authors: Sundram , Rahul Kumar
DOI Link: https://doi.org/10.22214/ijraset.2022.47087
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In this project “Aerofoil Design and Analysis” an attempt has made to make a complete study on lift and drag coefficient of various aerofoil sections using CFD. The primary goal of this project is to learn and analyse the aerodynamic performance of wings. The objective of this study is to improve aerofoil design using the software CATIA, And Fluent Analysis using the software ANSYS. Aerofoil is a principal part of any airplane construction. How much lift force and drag force is sufficient to balance the weight of the plane is decided by the aerofoil. Aerofoils are basically divided into two categories - they are Asymmetrical and Symmetrical aerofoils. Based on their drag and lift coefficient’s variation with angle of attack, stall angle of attack and magnitude of the coefficients they are divided. Here the NACA aerofoil is modified by adding dimples on the upper half of the wing and compared with the simple one. The comparison is made on different speed and pressure on the wing and the coefficient of lift and drag.
The only means of locomotion in the beginning, when man was still living in the lap of nature, was his legs. We have gradually progressed to speedier and more opulent modes of transportation, the most recent of which being air travel. As the aeroplanes were developed, they gained far more popularity than any other long distance travelling vehicle because it was the fastest way to travel and transport available. This led to rapid discovery in air transport field, to get the best out of the aerodynamics of the plane to conserve fuel and make it faster or whatever the need be. All of this is achieved by modifications made in the aerofoil design which with our project we aim to achieve.
The legendary Wright brothers conducted some of the first study on the curvatures or camber of a wing, known as an airfoil.
Airfoils were originally hand-built for each aircraft while powered flight was yet in its infancy. Prior to World War I, there was no standardised airfoil that could be used on a variety of planes, and few individuals were working on developing one.
The British government had previously done some study at the National Physical Laboratory (NPL), which resulted in a series of Royal Aircraft Factory airfoils.
Since World War II, it has also developed a reputation as a war machine. This increased popularity of air travel has resulted in numerous new inventions and research projects aimed at developing faster and more cost-effective planes. This endeavour is an attempt to figure out how to get the most performance out of a segment of an airfoil.
A cross-section of a plane's wing is referred to as an airfoil. Its primary function is to give an aeroplane lift during take-off and flight. However, it has a side effect known as drag, which works against the plane's velocity. The amount of lift a plane requires is determined by its intended function. Lift is required by heavier planes, whereas lightweight planes require less. As a result, the airfoil section is calculated based on the aircraft's use. The plane's vertical acceleration is also determined by the lift force, which is determined by the plane's horizontal velocity. With all other factors being equal, faster moving air has lower pressure than slower moving air, according to Bernoulli's principle, stated by Daniele Bernoulli, one of the most important pioneers in the field of fluid dynamics. This difference is what allows the slower moving air to push up against the bottom of the wing with greater force than the faster moving air is pushing down against the top of the wing. In level flight, this upward force is just enough to counteract the downward force caused by gravity.
B. Aerodynamic Forces and Coefficients
The force acting on the airfoil, perpendicular to the direction of the flow is defined as a lift force. The force acting on the airfoil, parallel to the direction of the flow is defined as a drag force. Dimensional analysis reveals that the nondimensional coefficients depends on the angle of attack, the Reynolds number, the Mach number and on the airfoil shape.
The National Advisory Committee for Aeronautics (NACA) a US based committee became a pioneer in the field of aerodynamics engineering, they created airfoil forms for aircraft wings (NACA). Following the word "NACA," a series of numerals explain the shape of the NACA airfoils. NACA initially developed the numbered airfoil system which was further refined by the United States Air Force at Langley Research Centre.
We are using Ansys for the analysis purposes. It offers structural analysis software solutions that enable engineers of all levels and backgrounds to solve complex structural engineering problems faster and more efficiently. With their suite of tools, we can perform finite element analyses (FEA), customize and automate solutions for structural mechanics challenges and analyse multiple design scenarios. By using Ansys early in the design cycle, businesses can save costs, reduce the number of design cycles and bring products to market faster.
Catia is used for designing the components that are being utilised in the project. CATIA is the world's most popular engineering and design software for 3D CAD product design. It is used in a range of industries to design, simulate, analyse, and create items, including aerospace, automotive, consumer goods, and industrial machinery, to mention a few.
II. WORKING PRINCIPLE
An aerofoil is a phrase used to describe the cross-sectional shape of an object that provides an aerodynamic force when propelled through a fluid such as air. Aerofoils are used on aeroplanes as wings or propeller blades to provide lift and propulsion. Both of these forces are generated in the opposite direction of the air flow. Drag occurs as a result of the formation of lift/thrust and acts in the same direction as the airflow.
Bernoulli’s theorem describes the fundamental principle of an aerofoil. Basically, total pressure equals static pressure + dynamic pressure (due to the weight of air above) (due to the motion of air).
When air passes over the top surface of an aerofoil, it has to travel quicker, gaining dynamic pressure in the process. The loss of static pressure causes a pressure difference between the upper and lower surfaces, which is known as lift and works against an aircraft's weight (or thrust that opposes drag).
More lift is provided by increasing the angle of attack (the angle between the chord line and the relative air flow). The aerofoil will stall when it reaches the crucial angle of attack (usually approximately 14 degrees).
A second method crosses the streamlines using Euler's Equations (from which the Bernoulli equation is derived). The higher velocity and acceleration over the top of the wing need a lower pressure above the wing than the ambient pressure due to the curve of the wing.
The path that a fluid molecule takes is known as a streamline. The fluid velocity is parallel to every point along the streamline.
It may thus be demonstrated that the pressure below the wing is greater than the pressure above the wing using either of the two ways. The difference in pressure causes an upward lifting force on the wing, allowing the plane to fly.
P: Pressure of the fluid. p: Density.
v: Velocity of the fluid relative to the airfoil. g: Magnitude of acceleration.
z: Height of the point.
Take point 1 to be well in front of the wing on the streamline P1 = P ambient is the pressure here. Take point 2 to be outside the boundary layer, above the curved surface of the wing. gz1 and gz2 are believed to be insignificant in comparison to the other elements of the equation (i.e., the effects due to gravity are small compared to the effects due to kinematics and pressure).
There are a number of terms involved while dealing with aerofoils:
The designer can vary the performance of an aerofoil by changing each of the above aspects so that it is appropriate for the task at hand.
In this project an effort has been made to have a detailed study and modification on lift and drag coefficient of various Airfoil section. We tried to differentiate between the two types i.e. Symmetrical and Asymmetrical Airfoil on the basis of their lift and drag coefficient, Variation with angle of contact, stall angle of attack and magnitude of the coefficients. Modelling of Symmetrical and Asymmetrical Airfoil in ANSYS has been studied, also the lift force on various foil on each angle of attack is determined and the horizontal velocity required for vertical acceleration during take-off for the foil has been calculated.
Due to the rise and availability of fuel and construction cost, transportation cost is increasing day by day in all modes. Airways have become more efficient mode of transportation today, this motivated us to study the design of airfoil and modification of few airfoil has been carried out so as to enhance the lift force and reduce the drag coefficient which would result in increasing the efficiency of aeroplanes and simultaneously reducing the fuel cost, which would lead to a major saving in construction cost of runways i.e., with small runway a flight with our designed airfoil can take off more easily and efficiently.
IV. LITERATURE REVIEW
"Control Theory based airfoil design using Euler's equations", a paper describing the optimising techniques based on the control theory for airfoil design. Results are presented for both the inverse problem and drag minimisation  “An Investigation of the effect of aspect ratio on Airfoil performance.” Describing the effect of aspect ratio on the overall performance of airfoil. This paper deals with the changes in shapes with respect to the changing of coordinates  They investigated and presented the creation of an airfoil profile in a CAD environment using the control purpose of the camber profile in the article. The state of the profile could be effectively changed using a method for modifying the quality of control focuses. The shape of the cambered airfoil was formed without affecting the fundamental geometry of the airfoil. The NACA 4412 airfoil profile was investigated and its usefulness for wind turbine edge investigation was discovered. GAMBIT 2.4.6 is used to form the geometry.
Using Quansi – 3D analysis codes, devised a method for optimising Turbine Airfoil. He overcame the difficulty of 3D modelling by modelling numerous 2D airfoil sections and combining their figures in a radial manner with second-order polygons. Providing in depth study of three airfoils namely RAE2822, ONERA M6 (D section) and NACA4412 .The findings reveal the rate at which aerodynamic properties converge in relation to geometric design factors, implying that geometric tolerance may not always be adequate to ensure convergence of certain parameters. Its show that the pleated corrugated aerofoil produces a comparable higher lift coefficient then that of Profiled aerofoil NACA 0012. The lift to drag ratio of these aerofoil is higher in between 4 to 8 degrees and it also has highest gliding ratio compared to the traditional aerofoil NACA 0012. The conclusion shows that the performance parameters of the bio-mimicked corrugated dragonfly wing is better than NACA 0012. This study presents the optimization of better and efficient aerofoil in wing design of eagle- sized flapping wing aircraft, Which will also capable of Hovering flight. And it is proved that for an angle of attack of 0 degrees, with a maximum lift coefficient of 0.542 and a drag coefficient of 0.005 is good enough, for low-speed long range operational flapping aircraft. Also, it needed a very good lift and drag ratio for efficient and predictive aerofoil for this flapping wing Aircraft. This paper presents both the Aerodynamic design and optimization of the Natural Laminar Flow (NLF) wing and the high lift configuration considering the mutual effects of both flap devices. And it is Proved that use of NLF technology at cruise design point leads to a reduction of 40 drag counts with respect to the turbulent aircraft. Also, some extra gains could be obtained by the Optimization of the wing tip device. Also, it has been observed the use of the droop nose increases significantly the stall margin and improves the drag coefficient while take off condition. The identification of the modal properties which are the mode shaped and the corresponding natural frequencies of the aircraft wing structure was measured. Here they compared for two different materials applied towards the wing structures which are the aluminium alloy AA-7075-T6 and AA-2024-T3 which currently being widely used by the aircrafts. And it is verified that both suitable to be used in building the wing structures as both do have alike properties but in term of strength levels, AA-7075- T6 are quite higher compared to AA-2024-T3. Natural frequencies for AA-7075-T6 were much lower compared to AA-2024-T3 which make AA7075-T6 much more suitable material for aircraft wing structure. This presents the difference between Asymmetrical and symmetrical aerofoil. And proved that symmetrical aerofoil has nearly equal drag coefficient as of asymmetrical aerofoil for same length and camber of aerofoil. Also, Asymmetrical have higher lift coefficient. Simulation based experiment given result of pressure distribution, Coefficient of drag, coefficient of lift, lift to drag ratio, vector profile and wake generation. They designed the standard NACA-0015 in ANSYS design modeler and further modified by adding dimple and a gurney flap at the lower end of the airfoil sheet. Then analysed the result by changing the dimensions of the modification. Research was done at various angles of attack from 0? to 20? at two different chordal Reynolds, Rec = 2.5 x 105 and 3.6 x 105. The torque coefficient is finally improved by an optimized use of the Gurney flap and the semi-circular dimple. Selection of wing parameters. Considerations for choice of wing parameters – airfoil section, aspect ratio, sweep, taper ratio, twist, incidence, dihedral and vertical location. The major goal of this study is to investigate and analyse the aerodynamic effects of dimples on the horizontal axis wind turbine blade's surface. When dimples are added to the blade surface of a wind turbine its efficiency improves.
The properties of airfoil lift, drag, and stall caused by flow separation were examined in this study. Keep in mind that airfoils aren't just for aeroplanes. The research described here can be applied to a variety of fluid dynamics scenarios: F1 car wings, helicopter blades, propeller blades, hydrofoils, and wind turbine blades. Turbine blades are an illustration of this. Published on 1 September 2004. This paper presents a study on parameterization methods for airfoil shape optimization within a CAD based design framework. The objective of the paper is to study the effect of different methods on airfoil shape optimization when using computational fluid dynamics (CFD). Two airfoils are studied in this paper to analyse their flexibility and robustness in producing optimal shapes when used in optimization study.
The investigation on albatross a huge sea bird finding out how they use dynamic soaring by removing power from the vertical wind speed gradient. These birds take advantage of wind gradient which are formed due to interaction amid air and sea to fly thousands of kilometres without beating of wings. Lift coefficient of E423 was best in comparison with E420 E421 and E422. Lift coefficient of GOE 174 was found higher than GOE 176 and E423 from minus 12 to plus 10-degree AOA. The result shows that the albatross wing performs better than delta wing, rectangular wing and Albatross wing. It states investigation performed on NACA 0012 airfoil to analyse the effect of variation on Reynold’s number on airfoil with and without gurney flap. Lift decreases and drag increases when Reynolds number is decreased. For high Reynold’s number above critical range decrease in CL & increase in CB are negligible. For lower Reynold’s number the two vertices behind the GF seems to increase the effective camber of the airfoil, causing zero lift angle and reduced stall angle. It describes how we can improve the efficiency and reliability of a turbine. We can use CFD for this.
A lift driven vertical axis wind turbine generates peak power when it is rotating at high tip-speed ratios. At this blade encounter angle of attack over small range from 0 degree to 30 degree. Its ability of self-start is dependent upon its performance at low tip-speed ratio during which angle of attack is between 0 degree to 180 degree. The result obtained from CFD model show reduction in coefficient of tangential force at low angle of attack (less than 90 degree) of no more than 30%while at high angle of attack an improvement of tangential force of over 100% is observed. It tells the need to enhance the aerodynamic of any windy shapes. The lift and drag forces at various angle of attack of a NACA 0015 blade were investigated in a wind tunnel. The test section was 1.2 m x 2.4 m depth. The maximum wind speed is 25m/s dimensions of normal blade are 0.7m length and 0.2m chord. Dimensions of studied blade are 700mm span and a 195mm chord. The aerodynamic of the span wise NACA0015 aerofoil blades with and without wavy leading-edge design were examined under steady and unsteady wind conditions, with wavy leading-edge blades can generate a better lift. This paper present design and development of front and rear wings for an existing FSAE prototype which can generate a down force of 25 to 30 kg. Based on motorsport racing aerodynamic requirement, aerofoil S1223 was selected. At Re 1.84X 105 , down force of 34.8kg and drag force of 8.317kgf was generated. In this paper, the shape design optimisation using morphing aerofoil/wing techniques, namely the leading and/or trailing edge deformation of a natural laminar flow RAE 5243 aerofoil is investigated. The use of morphing technique; LTED on an existing aerofoil, can reduce significantly the transonic drag which will save operating and manufacturing cost as well as emission reduction.
In this new generation any physical problem is first analysed virtually. Then the prototype is made to test after the successful result in both, the actual model is built. There is many software available for modelling a 3D design and in our project, we have used Catia V5 to model this airfoil.
For the design of the profile of the airfoil the coordinates of the Standard NACA 64215 are imported from the official website of the NACA Airfoil tool, which is used to plot the profile of the airfoil. The starting point of the Airfoil is of 100mm chord length. The airfoil is tapered from one side and the profile is reduced to 33mm chord length. Because the previous survey of few researchers shows that the tapered wings have high lift coefficient and better efficiency. And the efficiency could also be increased by adding the winglets.
The analysis is done in a rectangular domain with a length of 150cm, breadth of 100cm, and width of 28cm. The meshing is generated unistructural tetrahedral mesh because of its ability to mesh easily for complex geometry and arbitrary position. To make the mesh finer, the edge sizing is done, and the airfoil face sizing is done.
To measure the exit flow finer mesh is generated at the tip of the airfoil in a rectangular domain and meshed to size of 0.004m taking it as the body of influence.
A. Mesh Properties
Table 1: Mesh properties
No division in edge sizing
Element size on face
No of Inflation layer
For the analysis, the model selected is the viscous spalart-allmaras turbulence model. The model was developed for the analysis of aerodynamic flow. This model blends from viscous sublayer to logarithmic formula based on y+. It is 1 equation eddy viscosity transport model.
The final result of the modified airfoil has a less drag coefficient than our modified airfoil but not much change in the lift coefficient. For years the try error method helped many researchers to make the aviation industry improve the flight more fuel-efficient. The airfoil can be further modified to get a better result.
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Copyright © 2022 Sundram , Rahul Kumar. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Paper Id : IJRASET47087
Publish Date : 2022-10-15
ISSN : 2321-9653
Publisher Name : IJRASET
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