chp 4 hypersonics 4

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Hypersonic Educational Initiative 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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Page 1: Chp 4 Hypersonics 4

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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

Viscous Interactions

• Comparison of theory with CFD:

 Adiabatic Wall Cold Wall

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Hypersonic Educational Initiative

Viscous Interactions

• Comparison of theory with CFD:

 Adiabatic Wall Cold Wall

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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

Viscous Interactions:

Vehicle Scaling

From Anderson (1989) and Stollery (1972)

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Hypersonic Educational Initiative

Shock-Shock Interactions

• Edney classified shock interactions into 6 types:

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Hypersonic Educational Initiative

Shock-Shock Interactions:

Example

Mach 14.2, ReD=4000 Flow on a Cylinder with a 10o Shock Generator 

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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

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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Hypersonic Educational Initiative

Shock-Boundary Layer 

Interactions

• CFD of a 2-D Laminar Mach 6 SW-BL Interaction

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Hypersonic Educational Initiative

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