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Taylor, Chapters 2, 3.

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MAE 5540 - Propulsion Systems

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MAE 5540 - Propulsion Systems

Coordinate Transformations:(cont;d)

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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

MAE 5540 - Propulsion Systems

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MAE 6530, Propulsion Systems II3

Types of Aerodynamic Drag

M = 1

+ Base Drag

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

⎜⎜⎜⎜⎜

⎟⎟⎟⎟⎟⋅CL

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π ⋅ AR

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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⎛

⎝⎜⎜⎜

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2⋅ M∞ ⋅cosθL.E .( )2

⎝⎜⎜⎜

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⎪⎪⎪⎪⎪⎪⎪

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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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…. TWO DEGREES OF FREEDOM
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Independent Variables: F
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