Title: YOGESH BABBAR
1COMPUTATIONAL ANALYSIS OF RAM AIR PARACHUTE
CANOPY USING PANEL METHODS
- YOGESH BABBAR
- B.E 3rd year
- Aeronautical Engineering Department
- Punjab Engineering College, Chandigarh
Yogesh Babbar
PEC, Chandigarh
2Keywords
- Ram Air Parachute
- Parafoil
- Canopy
- Panel Methods
- Coefficient of Lift (CL)
- Coefficient of Lift (CD)
- Coefficient of Pressure (CP)
- CFD
-
Yogesh Babbar
PEC, Chandigarh
3Introduction A Ram Air Parachute
- Patented by Jalbert in 1966
- Better maneuverability as compared to drag
parachute - Category- Flexible wing aircraft
- Applications- cargo, military, recreation, sports
Yogesh Babbar
PEC, Chandigarh
4Principle of Operation
Yogesh Babbar
PEC, Chandigarh
5Current Research status
- Full parachute research is mainly based on
experiments - Work is due in structure canopy interactions.
- Various degree of freedom models are being
formulated. - Effect of leading edge cut is being formulated.
- CFD is being used to simulate the flow
Yogesh Babbar
PEC, Chandigarh
6Present Work( A Summary)
- Comparison of CL and CD for the Canopy using
lifting line theory and Source Panel methods
based on potential flow theory - The values of CL from theory have been directly
compared to the panel code values. - The comparison between theoretical and Panel Code
values for CD has been made under two cases - CASE1 Excluding Skin Friction
- CASE2 Including Skin Friction
Yogesh Babbar
PEC, Chandigarh
7Actual Geometry
Yogesh Babbar
PEC, Chandigarh
8Analyzed Geometry
Yogesh Babbar
PEC, Chandigarh
9Features
- Span 1.224m
- Chord 0.545m
- Radius of Curvature 0.8 span 0.9792m
- Planform area 0.66708 m2
- Aspect Ratio (b2/S) 2.248( low)
- Airfoil section ClarkY 18 thick
Yogesh Babbar
PEC, Chandigarh
10Assumptions
- Flow is assumed to be incompressible.
- The canopy is assumed to be closed at the front.
- The bumps at the surface are assumed to be
absent. - The skin friction drag is estimated theoretically
based on Reynolds number assuming turbulent flow
Yogesh Babbar
PEC, Chandigarh
11Theoretical formulation
Yogesh Babbar
PEC, Chandigarh
12Basic airfoil drag Pressure drag Skin
Friction drag
(30) (70)Total
Basic airfoil drag as given by Lingard0.015
CDo Basic Airfoil Drag
Yogesh Babbar
PEC, Chandigarh
13Panel Code
- Input
- 1. Geometry
- 2. Flow conditions
- Processing
- 1. Create panels on the surface
- 2. Obtain CP for each panel
- 3. Integrate to obtain coefficients
- Output
- Coefficient of Lift (CL)
- Coefficient of Drag (CD)
Yogesh Babbar
PEC, Chandigarh
14CD from Panel Code
- Panel Code cannot account for skin friction drag
- Case I Theoretical value of CD directly compared
to CD from Panel Code - Theoretical estimation of skin friction
- Total CD obtained after adding the CD due to skin
friction - Case II value of CD compared to new value of CD
Yogesh Babbar
PEC, Chandigarh
15Skin Friction Drag (Theoretical Estimation)
This value of skin friction drag is added to the
CD from panel code to get the total CD which can
be compared to the CD from theory( CASE II)
Yogesh Babbar
PEC, Chandigarh
16Results Color Plots for CL
Angle of attack0o Angle of Side
Slip0o Angle of attack10o Angle of Side
Slip0o Angle of attack0o Angle of Side
Slip6o
Color Bar
Yogesh Babbar
PEC, Chandigarh
17Coefficient of Lift (CL)
Yogesh Babbar
PEC, Chandigarh
18Coefficient of Drag( CD)CASE I( Excluding Skin
friction Drag)
Yogesh Babbar
PEC, Chandigarh
19Coefficient of Drag( CD)CASE II( Including Skin
friction Drag)
Yogesh Babbar
PEC, Chandigarh
20Highlights and Conclusions
- The theoretical and computational CD Vs a curves
diverge at high angles of attack - Theoretical Values in CASE I and CASE II differ
be a constant value of 0.0105. - Computational Values of CASE I and CASE II differ
be a constant value of 0.0108 - The good agreement in the comparison is subjected
to the assumption( Pressure drag 30 of Basic
Airfoil drag) - This analysis has limitations of being used in a
limited number of cases.
Yogesh Babbar
PEC, Chandigarh
21CFD Results( The Real Parachute)
Flow Conditions Angle of attack
5o Angle of side slip 0o Free stream
velocity 12 m /s
CL0.435 ( 0.5 from panel code) CD0.15 ( 0.05
from Panel code) Possible reasons for
variation LE cut, Bumps, Turbulence,
Yogesh Babbar
PEC, Chandigarh
22Future Work
- Work is underway for analyzing a 3-DoF model of
Parafoil Payload system - CFD work is underway for analyzing more realistic
conditions - Structure Canopy interactions can be further
investigated - Effect of Leading Edge cut can be further
investigated - CFD can also be utilized for a completer higher
degree of freedom models.
Yogesh Babbar
PEC, Chandigarh
23References
- Lingard J. S, (1995) Ram Air Parachute Design,
13th AIAA Aerodynamic Decelerator Conference,
Clearwater Beach. - Nicolaides JD, Speelman III RJ, Menard GLC. A
review of parafoil applications. Journal of
Aircraft Vol7 no 5, pp 423-431. - Aliabadi SK, Garrard WL, Kalro V, Mittal S,
Tezduyar TE, Stein KR. (1995)Parallel finite
element computations of the dynamics of large ram
air parachutes. AIAA Paper 95-1581, 13th
Aerodynamic Decelerator and Systems 33rd
conference, Clearwater, FL, 278293. - Fundamentals of aerodynamics by J. D. Anderson
Jr., McGraw-Hill,3rd edition, New York. - Joshua Aaron Bowman, Determinations of Parafoil
lift and drag coefficients using both three
dimensional modeling and experimental methods by,
Graduate College, Iowa State university, USA. - Om Prakash, (2003) Aerodynamics and Longitudional
Stability of Parafoil Payload system,Department
of Aerospace Engineering, Indian Institute of
Technology Bombay, Mumbai, India
Yogesh Babbar
PEC, Chandigarh
24Thank You
Questions Please!
Yogesh Babbar B.E. 3rd Year Dept. of Aeronautical
Engineering Punjab Engineering College Chandigarh
yogeshbabbar_at_gmail.com