Team 5 Aerodynamics PDR #2
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Transcript of Team 5 Aerodynamics PDR #2
November 18, 2003 Aero PDR #2 1
Team 5 Aerodynamics PDR #2Team 5 Aerodynamics PDR #2
• Scott Bird• Mike Downes• Kelby Haase• Grant Hile• Cyrus Sigari• Sarah Umberger• Jen Watson
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PreviewPreview
• Airfoil Sections and Geometry
• Aerodynamic mathematical model
• Launch Conditions• Endurance
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Walk-AroundWalk-Around
Data Boom
Conformal Pod
Engine
Landing Gear
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Aircraft 3-viewAircraft 3-view
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Wing GeometryWing Geometry
• Wing– Airfoil NACA 2412– Aspect Ratio 7– Span 14 (ft)– Chord 2 (ft)– Planform Area 28 (ft^2)– Taper Ratio 0 (deg)– Dihedral 0 (deg)– Sweep Angle 0 (deg)
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Horizontal Tail GeometryHorizontal Tail Geometry
• Horizontal Tail– Airfoil NACA 0012– Aspect Ratio 5– Span 7 (ft)– Chord (average) 1.38 (ft)– Planform Area 9.64 (ft^2)– Taper Ratio 0.8– Sweep Angle 5 (deg)
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Vertical Tail GeometryVertical Tail Geometry
• Vertical Tail– Airfoil NACA 0012– Aspect Ratio 2– Span 2.8 (ft)– Chord (average) 1.38 (ft)– Planform Area 3.9 (ft^2)– Taper Ratio 0.73 – Sweep Angle 10 (deg)
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Lift MethodologyLift Methodology
• Used XFOIL to get NACA 2412 2-D data
– Converted 2-D data to 3-D data for wing CLo and CLα
• Used XFOIL to get NACA 0012 horizontal tail data
– Used method described in Roskam Part VI, CH8 for CLδe
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Aerodynamic Mathematical Model of LiftAerodynamic Mathematical Model of Lift
• CL= CLo + CLα * α + CLδe * δe
• CLα = Cl α / (1 + (Cl α / (π * e * A))) [rad-1]
• CL = Cl * (CLα/Cl α)
• CLδe = CLα_ht * ηht * Sht / Sref * τe [rad-1]
– ηht = f (Sht_slip, Sht, Pavailable, U, Dp, qbar)
– (Roskam Part VI, CH8)
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Aerodynamic Mathematical Model of DragAerodynamic Mathematical Model of Drag
• Summation of individual components for CDo
– Wing, fuselage, horizontal tail, vertical tail
• CD=CDo + k * CL * CL
• CDo = Σ CDo(i)
– CDo(i) = (Cf * FF * Q * Swet) / Sref
• k = 1 / (pi * AR * e)
CDo(i)
CDo_wing 0.0104
CDo_horizontal tail 0.0039
CDo_vertical tail 0.0013
CDo_fuselage 0.0204
CDo_total 0.036
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Moment MethodologyMoment Methodology
• Used method described in Roskam, Chapter 3 of AAE 421 Book to find individual components of moment equation
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Aerodynamic Mathematical Model of MomentsAerodynamic Mathematical Model of Moments
• CM = CMo + CMα * α + CMδe * δe– (α and δe in degrees)
• CM0 = Cmac_wf + CL0_wf*(xbar_cg - xbar_acwf) + CLalpha_h*eta_h*(S_h/S)*(xbar_ach - xbar_cg)*epsilon
• CMalpha = (x/cw)*CLalpha_wf*(xbar_cg - xbar_acwf) - CLalpha_h*eta_h*(S_h/S)*(xbar_ach - xbar_cg)*(1 – depsilon/dalpha)
• CMdele = -CLalpha_h*eta_h*Vbar_h*tau_e
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Aerodynamic Mathematical Model SummaryAerodynamic Mathematical Model Summary
• CL= 0.1764 + 7.941 (rad-1)* α + 1.925 (rad-1)* δe– α and δe are in radians
• CD = .036 + .0522 * (.1764 + 7.941 (rad-1) * α)2
• Cm= - 0.0280 - 0.1562* α - 0.0898* δe
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Launch ConditionsLaunch Conditions
Known Values• W = 49.6 lbs• S = 28 ft2
• ρ = 0.0023328 slug/ft3 (at 600 ft)
• CLmax:To = 0.8*CLmax = 1.44
•
VTO = 39 ft/s
sft
CLS
WV
TO
TOTO 39
max
122.1
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Launch Conditions from EOMLaunch Conditions from EOM
ThrustDrag
Friction
Normal
Weight
WSCxx
Bhpxm
FrictionDragThrustmaF
Dop
horizontal
2
21550
Our Airplane
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Launch Conditions from EOM integrationLaunch Conditions from EOM integration
• STO = 76 ft– Constriant
of 127 ft
• tTO = 3.7 s
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EnduranceEndurance
Known Values• Bhp = 3.7 hp
• ηp = 0.40
• Cbhp = 0.0022 lb/s-hp
• Wi = 49.6 lbf
• Wf = 43.6 lbf – Using 1 gallon @ 6 lbf
• L/D = 10.39 • 12*.866 (86.6% of L/Dmax when flying @ Vmin power)
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EnduranceEndurance
• V = [2*W/( ρ*S)*(K/(3*CDo))1/2] ½
• (Raymer, eq 17.33)
– K = 1 / ( pi * AR * e )– Vmin@min power = 32.5 ft/s
• E = (L/D)*[(550*ηp)/(Cbhp*V)]*ln(Wi/Wf) • (Raymer eq 17.31)
E = 75.5 minutes
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Future WorkFuture Work
• Resize flaps for landing
• Verify known values
– Cbhp
• Weight reduction from extra fuel (Endurance)
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Review of Today’s PresentationReview of Today’s Presentation
• Wing Geometry and Size
• 3-view of aircraft
• Aerodynamic mathematical model
• Launch Conditions
• Endurance
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QuestionsQuestions
Questions??
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ReferencesReferences
• Roskam– AAE 421 Book
• Raymer– Aircraft Design: A Conceptual Approach
• AAE 251 Book– Introduction to Aeronautics: A Design Perspective
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Putting EOMs into MATLABPutting EOMs into MATLAB
• Put state space EOMs into MATLAB• Used ode45 command to integrate EOMs• Inputs to the code are initial conditions for position
and velocity – Used x(0) = 0.1ft and v(0) = 1ft/s to eliminate singularities
• Code output position and velocity as a function of time
xy
xy
2
1
WSCyy
Bhp
mxy
yxy
Dop
2221
2
55012
21
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EOM file in MATLABEOM file in MATLAB
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