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MAE 5540 - Propulsion Systems
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MAE 5540 - Propulsion Systems
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MAE 5540 - Propulsion Systems
Coordinate TransformationsCoordinate Transformations:
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ji r
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{i, j} fixed in space
MAE 5540 - Propulsion Systems
Coordinate Transformations:(cont;d)
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• A Matrix "trick" for coordinate transform in 2-D
Coordinate Transformations
MAE 5540 - Propulsion Systems
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MAE 6530, Propulsion Systems II
RS 101: SummaryExternal Forces Acting on Rocket
2
•Lift – acts perpendicular to flight path (non-conservative)•Drag – acts along flight path (non-conservative)•Thrust – acts along longitudinal axis of rocket (non-conservative)•Gravity – acts downward (conservative)
Becauseliftactsperpendiculartoflightpath,dragistheprimarydissipativeforceactingonairframe
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MAE 6530, Propulsion Systems II 4
Types of Aerodynamic Drag (2)
Drag Mechanisms Acting on Launch Vehicles (LVs)• Subsonic
o Viscous drag–Wetted Area Skin Friction–Flow Separation (small for LVs)
o Pressure drag (form drag)– Forebody– Interference (fin roots)– Base
o Induced (lift drag, small for LVs)• Supersonic
o Wave drago Compressive drag due to lift
• “Dither” Drag due to unsteady a modulation• Total drag
MAE 6530, Propulsion Systems II
5
Skin Friction Drag
dAτwall
Flow Momentum lost due to surface viscosity
CF =τwall ⋅dA
surf∫∫q ⋅ Awet
Awet
CDF=
Awet
Aref
⋅CF →
CF = skin friction coefficient
Awet = forebody wetted surface area
Aref = vehicle reference area, π4⋅Dmax
2
MAE 6530, Propulsion Systems II
Forebody Form (Pressure) Drag
9
• Subsonic form drag directly related to boundary layer development along body. • Knowing friction drag, subsonic form drag (CD0 ) correlated with skin friction
coefficient (CF) and body fineness ratio (L/D)
CD0 =κ ⋅AwetAref⋅CF
⎛
⎝
⎜⎜⎜⎜⎜
⎞
⎠
⎟⎟⎟⎟⎟
High l/t Profile
lt
Low l/t Profile
lt
k
Drew and Jenn, “Pressure Drag Calculations on Axisymmetric Bodies of Arbitrary Mold Line,” AIAA 90-0280, 28th Aerospace Sciences Meeting, 8-11 Jan., 1990, Reno NV.
MAE 6530, Propulsion Systems II 10
• Boundary Layer on Vehicle Base Area Separates
• Low Pressure Separated Region Forms• Low Pressure Causes a Large net Pressure
Difference• Especially significant on Launch Vehicle
after motor burnout
Base Drag
MAE 6530, Propulsion Systems II
Base Drag (3)
12
Base Drag
Base Drag
Burning Rocket Pressurizes Base Area, Eliminating Base Drag
MAE 6530, Propulsion Systems II
Base Drag (4)
13
• Effect of “Boat Tailing” – Boat tail used on the rear end of rocket to reduce the base drag force by reducing area against which aft end pressure suction acts
• Effect of “Boat Tailing” – Boat tail Also serves to reduce the severity of the flow separation by reducing the exit turning angle
CDboattail≈CDbase ⋅
dD
⎛
⎝⎜⎜⎜⎞
⎠⎟⎟⎟⎟
2
MAE 6530, Propulsion Systems II
Fin “Dither” Drag
14
• Even along Ballistic Trajectory where nominal a ~ 0, fins can contribute induced drag to configuration due to unsteady “dither” or fin misalignment
• Shed Vortex from base is Unsteady and Contributes to Pitch Oscillations to Vehicle
•”Dither” Drag due to Small angle of attack oscillations results in RMS drag contribution
20 ft.
7.5 ft.
5 ft.
9.5 ft.
M2-F1
"Vortex Street"
Figure 4: Von Karman "Vortex Street" Formation Trailing M2-F1 Aircraft
“Vortex Street” trailing M2-F1
δα>0
δα= 0
δα<0
MAE 6530, Propulsion Systems II
Fin “Dither” Drag (2)
15
δα>0
δα= 0
δα<0
Dither” = Unsteady Induced Drag Component
Asurf = Planform area
CLα= Lift−curve slope
AR = Aspect ratio
δαdither = RMS angle of attack dither
CD "dither"=AsurfAref
⎛
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2
MAE 6530, Propulsion Systems II
Fin Leading Edge Drag
18
• Stagnation Pressure Coefficient calculated based on Mach number Normal to leading edge of fins
• Scaled by leading edge area, W•t• Assumed fin thickness, t
Cpmax =qc− p∞q
=p∞ ⋅ 1+
γ−12M⊥
2⎛
⎝⎜⎜⎜
⎞
⎠⎟⎟⎟⎟
γγ−1− p∞
γ2p∞M⊥
2=1+ γ−1
2⋅ M∞ ⋅cosθL.E .( )2
⎛
⎝⎜⎜⎜
⎞
⎠⎟⎟⎟⎟
γγ−1−1
γ2⋅ M∞ ⋅cosθL.E .( )2
CDL .E .( )totalfins
=Wi ⋅tiAref
⎛
⎝
⎜⎜⎜⎜⎜
⎞
⎠
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∑ ⋅ CPmax( )subsonic{ }
i=
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⎛
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⎞
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i
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MAE 6530, Propulsion Systems II
Total Drag Correlation Model
19
CD( )total=CDF +CD0 +CDbase +CDDither +CDL .E .
Skin FrictionDrag
Nose/BodyProfile Pressure
Drag
Base AreaWake Drag
Unsteady DitherDrag, Fins Fins, Leading
Edge Pressure Drag
• Medium Fidelity Engineering Model for “First Cut” Drag Coefficient Estimator.
• Calculates Subsonic Drag Coefficient in Incompressible Flight Regime ~ Mach 0.3
• Rigorously, each term of the above equation should be scaled for compressibility at Higher Mach numbers
• Operationally, Bulk scaling of is often used CD( )total
• Does not Model Wave Drag
MAE 6530, Propulsion Systems II
Correcting for Compressibility
20
wdpdfdd
wavepressurefriction
cccc
DDDD
,,, ++=
++= Only at transonic andsupersonic speedsDwave= 0 for subsonic speedsbelow Mdrag-divergence
Profile DragProfile Drag coefficient relatively constant with M∞ at subsonic speeds
Credit: D. R. KirkFIT, 2011
Supersonic CDVaries as …
Subsonic CDVaries as ~…
MCR
Viscosity Effects
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