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Siva V Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42
www.ijera.com 40 | P a g e
Analysis of Ground Effect on a Symmetrical Airfoil
Siva V*
*Assistant Professor, Department of Aeronautical Engineering, Sri Ramakrishna Engineering College,
Coimbatore- 641 022.
ABSTRACT
A Detailed Study and Computational Fluid Dynamics investigation was conducted to ascertain and highlight the
different ways in which ground effect phenomena are present around a symmetrical aerofoil-NACA 0015- when
in close proximity to the ground. The trends in force and flow field behaviour were observed at various ground
clearances, for different angle of attack. The analysis was carried out by varying the angle of attack from 00
to
100
and ground clearance of the trailing edge from minimum possible value to one chord length. It was found
that high values of pressure coefficient are obtained on the lower surface when the airfoil is close to the ground.
This region of high pressure extended almost over the entire lower surface for higher angles of attack. As a
result, higher values of lift coefficient are obtained when the airfoil is close to the ground. The flow accelerates
over the airfoil due to flow diversion from the lower side and higher mean velocity is observed near the suction
peak location. The pressure distribution on the upper surface did not change significantly with ground clearance
for higher angles of attack. The lift was found to drop at lower angles of attack at some values of ground
clearance due to suction effect on the lower surface as the result of formation of a convergent–divergent passage
between the airfoil and the ground plate. The values of drag coefficient were also noted for different ground
clearance, which is found to be decreasing as the airfoil is approaching to a closer ground clearance. This ground
effect is analyzed using FLUENT 5/6 code.
Keywords – Computational Fluid Dynamics, Gambit, Fluent 5/6 Code
I. INTRODUCTION
In Over the last 20 years, research interest in the
various flow phenomena associated with bodies in
close proximity to the ground, has been growing. The
aerodynamic behaviour of such bodies is distinctly
different from that which would be seen about the
body if it were placed far from the ground. These
distinct flow characteristics are generically referred
to as ‘ground effect’.
Ground effect is caused by ground interference
with airflow patterns around an aircraft when the
aircraft is within one wingspan of the surface. If the
approach airspeed is too fast, the aircraft will tend to
float down the runway, delaying touchdown of the
aircraft. Various studies have been undertaken in the
past to examine and explain the effect of ground
effect on wings or aerofoils, through analytical,
numerical and experimental methods. Additionally,
various studies have sought to explain ground effect
wings or aerofoils, mainly through numerical and
experimental means. However this project will
demonstrate a simplistic assertion and the influence
ground effect on a symmetrical aerofoil using CFD
analysis. That is the primary aim of this study.
The main objectives of the present work are:
(a) to study the complete phenomena of ground
effect.
(b) to study the pressure distribution over the
aerofoil surface at different ground clearances
and angles of attack
(c) to measure the lift and drag forces over the
surface for different ground
clearance and angle of attack.
1.1 Lift and Drag
The lift and drag produced by a wing define the
performance and general attributes of the craft that it
supports. A wing moving through the air produces a
resultant force. Lift is defined as the component of
the resultant force perpendicular to the velocity
vector of the wing. Induced drag is defined as the
component of the resultant force parallel to the
velocity vector of the wing. There are also other
forms of drag, which are collectively referred to as
parasite or profile drag, which is the drag created by
the friction of the object moving through the air. The
total drag of an object moving through the air is the
sum of induced drag and parasite drag. Both lift and
drag are functions of a number of variables, the
density of the air, the velocity of the object through
the air and the geometry of the object.
1.2 Downwash
In order to conserve the momentum of the air
mass moving around a wing, the flow field before
and after the wing is distorted. This phenomenon is
known as downwash. As downwash changes the flow
around the wing, it affects the relationships of lift and
drag to the angle of incidence. Downwash can be
RESEARCH ARTICLE OPEN ACCESS
Siva V Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42
www.ijera.com 41 | P a g e
represented as a vertical flow component of the free
stream velocity and is designated (w).
1.3 Gambit
The gambit software is a pre processor for a
fluent code. This is used to design and mesh the
working domain. The work domain is generated with
the help of our geometry and control volume. The
control volume is created by inlet and outlet faces
perpendicular to the flow. So the flow entering
normal to the inlet face will automatically behave as
the free stream air.
1.4 Fluent
The mesh generated in gambit is solved using the
appropriate solver, turbulence model and boundary
layer. FLUENT is a commercial CFD code that
solves the RANS equations on hybrid unstructured
grids. It uses a second order upwind discretization
based on the SIMPLE pressure velocity coupling and
the formation can accommodate incompressible
flows.
The core of CFD system FLUENT is numerical
iterative solver. it solves equation describing the
airflow of the model case by conservation of
momentum, mass and energy. Geometric model of
the flow must be discretize in the form of
computational mesh and equations are solved on this
mesh subsequently.
II. INDENTATIONS AND
EQUATIONS
The derivatives are written in the following way
for convenience:
CLα = dCL / dα (1)
CMα = dCM / dα (2)
CLh = dCL / dh (3)
CMh = dCM / dh (4)
The aerodynamic centre, also known in
aircraft, is the point where CM remains constant with
changing pitch angle. It is denoted (aerodynamic)
centre in pitch here. Its definition is:
Xα = CMα / CLα (5)
The (aerodynamic) centre in height is the point
where CM remains constant with changing height. It
is defined as:
Xh = CMh / CLh (6)
III. TABLES AND FIGURES
EDGE NAME BOUNDART TYPE
INLET VELOSITY INLET
OUTLET PRESSURE OUTLET
TOP WALL
GROUND WALL
AEROFOIL WALL
Table.1 Boundary type for each edge
Table.2 Number of cells and elements for each angle
of attack
Figure1. Mesh generated using size function
Figure 2.Meshed aerofoil
Figure.3 10 degree velocity distribution
Angle of
attack
No of cells No of
elements
No of
nodes
0 525847 798112 272265
2.5 238530 360740 122210
5 238430 360590 122160
7.5 238238 360361 121545
10 238432 360593 122161
Siva V Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42
www.ijera.com 42 | P a g e
Figure.4 10 degree pressure distribution
Figure.5 7.5degree.h/c =0.2 velocity distribution
Figure.6 7.5degree,h/c=0.2 pressure distribution
IV. CONCLUTIONS
Result have been presented for computation of
flow past a NACA 0015 airfoil using flow governing
equations in conjunction with a spalart-allmaras
turbulence model for closure. The flow over an airfoil
with respect to the ground is analysed using
FLUENT and results have been plotted and
discussed. Though the results were deviated slightly
from the known concept and we could able to justify
it still and a detailed analysis have to be carried out to
bring a optimum result.
The important conclusions from the present work
are:
1. A suction effect is observed on the lower surface at
certain ground clearances at angles of attack up to 50
,
due to the formation of a convergent–divergent
passage between the airfoil and the ground, causing a
local drop in lift force.
2. For very low ground clearances, the lift force was
found to be always high, due to higher pressure on
the lower surface of the airfoil. At higher angles of
attack, high values of pressure coefficient were
recorded on the lower surface with the high pressure
region extending almost till the trailing edge of the
airfoil, which resulted in higher lift force. The
pressure distribution on the upper surface did not
show significant variation with ground clearance,
especially for higher angles of attack; hence, the
higher lift force was mainly due to modification of
pressure distribution on the lower surface.
3. A reduction in pressure on the suction side was
observed at higher angles of attack, causing an
adverse pressure gradient on the upper surface, a
retarded flow and hence a thick wake region. At very
low ground clearances, the airfoil and the ground
plate boundary layers were found to merge which
resulted in a higher momentum loss and hence a
relatively higher drag for higher angles of attack.
REFERENCES
[1]. Ahmed.M.R and Sharma.S.D (2004) ‘An
investigation on the aerodynamics of a
symmetrical airfoil in ground effect’
Experimental Thermal and Fluid Science.
[2]. Anderson.J.D Jr, (2001) ‘Fundamentals of
Aerodynamics, third ed., Mc Graw-Hill’ p.
283, 284, 334, 335.
[3]. Barlow.J.B, Ranzenbach. R, (1994) ‘Two-
dimensional airfoil in ground effect, an
experimental and computational study’,
Society of Automotive Paper No. 94-2509.
[4]. Chang C.H, Chun H.H, (2002)
‘Longitudinal stability and dynamic motions
of a small passenger WIG craft’, Ocean
Engineering 29,pp 1145-1162
[5]. Chen C.K., Hsiun C.M, (1996)
‘Aerodynamic characteristics of a two
dimensional airfoil with ground effect’, J.
Aircraft 33 (2) p.386–392.
[6]. Ollila R.G., (1980) ‘Historical review of
WIG vehicles’, J. Hydronaut. 14 (3) p. 65–
76.
[7]. Robert C. Nelson, (1998) Flight Stability
and Automatic Control, 2nd ed., McGraw-
Hill.

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Analysis of Ground Effect on a Symmetrical Airfoil

  • 1. Siva V Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42 www.ijera.com 40 | P a g e Analysis of Ground Effect on a Symmetrical Airfoil Siva V* *Assistant Professor, Department of Aeronautical Engineering, Sri Ramakrishna Engineering College, Coimbatore- 641 022. ABSTRACT A Detailed Study and Computational Fluid Dynamics investigation was conducted to ascertain and highlight the different ways in which ground effect phenomena are present around a symmetrical aerofoil-NACA 0015- when in close proximity to the ground. The trends in force and flow field behaviour were observed at various ground clearances, for different angle of attack. The analysis was carried out by varying the angle of attack from 00 to 100 and ground clearance of the trailing edge from minimum possible value to one chord length. It was found that high values of pressure coefficient are obtained on the lower surface when the airfoil is close to the ground. This region of high pressure extended almost over the entire lower surface for higher angles of attack. As a result, higher values of lift coefficient are obtained when the airfoil is close to the ground. The flow accelerates over the airfoil due to flow diversion from the lower side and higher mean velocity is observed near the suction peak location. The pressure distribution on the upper surface did not change significantly with ground clearance for higher angles of attack. The lift was found to drop at lower angles of attack at some values of ground clearance due to suction effect on the lower surface as the result of formation of a convergent–divergent passage between the airfoil and the ground plate. The values of drag coefficient were also noted for different ground clearance, which is found to be decreasing as the airfoil is approaching to a closer ground clearance. This ground effect is analyzed using FLUENT 5/6 code. Keywords – Computational Fluid Dynamics, Gambit, Fluent 5/6 Code I. INTRODUCTION In Over the last 20 years, research interest in the various flow phenomena associated with bodies in close proximity to the ground, has been growing. The aerodynamic behaviour of such bodies is distinctly different from that which would be seen about the body if it were placed far from the ground. These distinct flow characteristics are generically referred to as ‘ground effect’. Ground effect is caused by ground interference with airflow patterns around an aircraft when the aircraft is within one wingspan of the surface. If the approach airspeed is too fast, the aircraft will tend to float down the runway, delaying touchdown of the aircraft. Various studies have been undertaken in the past to examine and explain the effect of ground effect on wings or aerofoils, through analytical, numerical and experimental methods. Additionally, various studies have sought to explain ground effect wings or aerofoils, mainly through numerical and experimental means. However this project will demonstrate a simplistic assertion and the influence ground effect on a symmetrical aerofoil using CFD analysis. That is the primary aim of this study. The main objectives of the present work are: (a) to study the complete phenomena of ground effect. (b) to study the pressure distribution over the aerofoil surface at different ground clearances and angles of attack (c) to measure the lift and drag forces over the surface for different ground clearance and angle of attack. 1.1 Lift and Drag The lift and drag produced by a wing define the performance and general attributes of the craft that it supports. A wing moving through the air produces a resultant force. Lift is defined as the component of the resultant force perpendicular to the velocity vector of the wing. Induced drag is defined as the component of the resultant force parallel to the velocity vector of the wing. There are also other forms of drag, which are collectively referred to as parasite or profile drag, which is the drag created by the friction of the object moving through the air. The total drag of an object moving through the air is the sum of induced drag and parasite drag. Both lift and drag are functions of a number of variables, the density of the air, the velocity of the object through the air and the geometry of the object. 1.2 Downwash In order to conserve the momentum of the air mass moving around a wing, the flow field before and after the wing is distorted. This phenomenon is known as downwash. As downwash changes the flow around the wing, it affects the relationships of lift and drag to the angle of incidence. Downwash can be RESEARCH ARTICLE OPEN ACCESS
  • 2. Siva V Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42 www.ijera.com 41 | P a g e represented as a vertical flow component of the free stream velocity and is designated (w). 1.3 Gambit The gambit software is a pre processor for a fluent code. This is used to design and mesh the working domain. The work domain is generated with the help of our geometry and control volume. The control volume is created by inlet and outlet faces perpendicular to the flow. So the flow entering normal to the inlet face will automatically behave as the free stream air. 1.4 Fluent The mesh generated in gambit is solved using the appropriate solver, turbulence model and boundary layer. FLUENT is a commercial CFD code that solves the RANS equations on hybrid unstructured grids. It uses a second order upwind discretization based on the SIMPLE pressure velocity coupling and the formation can accommodate incompressible flows. The core of CFD system FLUENT is numerical iterative solver. it solves equation describing the airflow of the model case by conservation of momentum, mass and energy. Geometric model of the flow must be discretize in the form of computational mesh and equations are solved on this mesh subsequently. II. INDENTATIONS AND EQUATIONS The derivatives are written in the following way for convenience: CLα = dCL / dα (1) CMα = dCM / dα (2) CLh = dCL / dh (3) CMh = dCM / dh (4) The aerodynamic centre, also known in aircraft, is the point where CM remains constant with changing pitch angle. It is denoted (aerodynamic) centre in pitch here. Its definition is: Xα = CMα / CLα (5) The (aerodynamic) centre in height is the point where CM remains constant with changing height. It is defined as: Xh = CMh / CLh (6) III. TABLES AND FIGURES EDGE NAME BOUNDART TYPE INLET VELOSITY INLET OUTLET PRESSURE OUTLET TOP WALL GROUND WALL AEROFOIL WALL Table.1 Boundary type for each edge Table.2 Number of cells and elements for each angle of attack Figure1. Mesh generated using size function Figure 2.Meshed aerofoil Figure.3 10 degree velocity distribution Angle of attack No of cells No of elements No of nodes 0 525847 798112 272265 2.5 238530 360740 122210 5 238430 360590 122160 7.5 238238 360361 121545 10 238432 360593 122161
  • 3. Siva V Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 10, (Part - 2) October 2015, pp.40-42 www.ijera.com 42 | P a g e Figure.4 10 degree pressure distribution Figure.5 7.5degree.h/c =0.2 velocity distribution Figure.6 7.5degree,h/c=0.2 pressure distribution IV. CONCLUTIONS Result have been presented for computation of flow past a NACA 0015 airfoil using flow governing equations in conjunction with a spalart-allmaras turbulence model for closure. The flow over an airfoil with respect to the ground is analysed using FLUENT and results have been plotted and discussed. Though the results were deviated slightly from the known concept and we could able to justify it still and a detailed analysis have to be carried out to bring a optimum result. The important conclusions from the present work are: 1. A suction effect is observed on the lower surface at certain ground clearances at angles of attack up to 50 , due to the formation of a convergent–divergent passage between the airfoil and the ground, causing a local drop in lift force. 2. For very low ground clearances, the lift force was found to be always high, due to higher pressure on the lower surface of the airfoil. At higher angles of attack, high values of pressure coefficient were recorded on the lower surface with the high pressure region extending almost till the trailing edge of the airfoil, which resulted in higher lift force. The pressure distribution on the upper surface did not show significant variation with ground clearance, especially for higher angles of attack; hence, the higher lift force was mainly due to modification of pressure distribution on the lower surface. 3. A reduction in pressure on the suction side was observed at higher angles of attack, causing an adverse pressure gradient on the upper surface, a retarded flow and hence a thick wake region. At very low ground clearances, the airfoil and the ground plate boundary layers were found to merge which resulted in a higher momentum loss and hence a relatively higher drag for higher angles of attack. REFERENCES [1]. Ahmed.M.R and Sharma.S.D (2004) ‘An investigation on the aerodynamics of a symmetrical airfoil in ground effect’ Experimental Thermal and Fluid Science. [2]. Anderson.J.D Jr, (2001) ‘Fundamentals of Aerodynamics, third ed., Mc Graw-Hill’ p. 283, 284, 334, 335. [3]. Barlow.J.B, Ranzenbach. R, (1994) ‘Two- dimensional airfoil in ground effect, an experimental and computational study’, Society of Automotive Paper No. 94-2509. [4]. Chang C.H, Chun H.H, (2002) ‘Longitudinal stability and dynamic motions of a small passenger WIG craft’, Ocean Engineering 29,pp 1145-1162 [5]. Chen C.K., Hsiun C.M, (1996) ‘Aerodynamic characteristics of a two dimensional airfoil with ground effect’, J. Aircraft 33 (2) p.386–392. [6]. Ollila R.G., (1980) ‘Historical review of WIG vehicles’, J. Hydronaut. 14 (3) p. 65– 76. [7]. Robert C. Nelson, (1998) Flight Stability and Automatic Control, 2nd ed., McGraw- Hill.