chp 4 hypersonics 4
TRANSCRIPT
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Viscous Interactions
4.1 Leading-Edge Interactions
4.2 High-Altitude Vehicle Aerodynamics Scaling
4.3 Shock-Boundary Layer Interactions;
Shock-Shock Interactions
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Leading-Edge Interactions
or Viscous Interactions
• Consider a flat plate in a hypersonic stream
• Boundary layer displaces the flow:
– Shock wave forms
– Pressure rise compresses the BL, introduces an
axial pressure gradient
– Changes growth of BL, which affects shock
• Use theory to determine scaling of this effect
Shock Wave
Boundary Layer Displacement, !*
M >> 1
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Leading-Edge Interactions
or Viscous Interactions
• CFD solutions:
Adiabatic Wall
M = 6, Re = 284,000 based on plate length
Cold Wall: Tw/Te=2
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Viscous Interactions
• Use approximate variation of pressure with flow
turning angle to derive variation of displacement
thickness with M and Re
Adiabatic Wall Cold Wall
Strong
Weak
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Viscous Interactions
• Comparison of theory with CFD:
Adiabatic Wall Cold Wall
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Viscous Interactions
• Comparison of theory with CFD:
Adiabatic Wall Cold Wall
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Viscous Interactions:
Vehicle Scaling
• Aerodynamic coefficients scale differently:
• Viscous interactions tend to increase drag, but not
change lift much
– L/D should scale with
– CD should increase with
– Effect is larger for vehicles with large wetted area
• Approach free-molecular limit at very low density
(large )
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Viscous Interactions:
Vehicle Scaling
From Anderson (1989) and Stollery (1972)
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Shock-Shock Interactions
• Edney classified shock interactions into 6 types:
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Shock-Shock Interactions:
Example
Mach 14.2, ReD=4000 Flow on a Cylinder with a 10o Shock Generator
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Shock-Shock Interactions:
Example
• Huge increase in surface pressure and heat flux
Surface Pressure and Heat Flux Relative to Undisturbed Flow
Note compression of BL
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Shock-Shock Interactions
• Huge localized pressure and heating augmentation
– Jet compresses boundary layer
– In reality, jet is unsteady
– Augmentation for turbulent flow, reacting gas is
difficult (impossible) to compute.
• Strength decreases with cylinder sweep
– Limited experiments in this area: Berry and Nowak
• S-SI must be avoided or designed around
– Bow shock – wing-leading edge interaction
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Shock-Boundary Layer
Interactions
• Shock impinges on a boundary layer
CFD of a 2D Shock-Boundary Layer Interaction
Compression of BL
Separation
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Shock-Boundary Layer
Interactions
• CFD of a 2-D Laminar Mach 6 SW-BL Interaction
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Shock-Boundary Layer
Interactions
• SBLI also cause high localized pressure & heating
• SBLI also occur on compression corners:
– If laminar, separation is large; shear layer
transitions at all but lowest Re
– Turbulent separation is much smaller, unsteady?
• Tend to be a much larger issue inside engines
• Difficult (impossible) to accurately compute high
Mach number turbulent interactions