Turbulent boundary layers are complex fluid regions near solid surfaces, characterized by chaotic motion and rapid mixing. They play a crucial role in many engineering applications, affecting drag, heat transfer, and flow separation.
Understanding turbulent boundary layers is essential for optimizing fluid systems. This topic explores their structure, governing equations, and control methods, providing insights into how engineers can manipulate these layers to improve performance in various fields.
Turbulent vs laminar flow
Turbulent flow characterized by chaotic, irregular motion with rapid mixing and fluctuations in velocity, pressure, and temperature
Laminar flow characterized by smooth, parallel layers of fluid with no mixing between layers
Turbulent flow occurs at high Reynolds numbers while laminar flow occurs at low Reynolds numbers
Boundary layer theory
Describes the thin layer of fluid near a solid surface where viscous effects are significant
Boundary layer develops due to the no-slip condition at the surface, causing velocity to increase from zero to the freestream value
Boundary layer thickness
Top images from around the web for Boundary layer thickness WES - Experimental validation of a ducted wind turbine design strategy View original
Is this image relevant?
WES - Laminar-turbulent transition characteristics of a 3-D wind turbine rotor blade based on ... View original
Is this image relevant?
WES - Experimental validation of a ducted wind turbine design strategy View original
Is this image relevant?
1 of 3
Top images from around the web for Boundary layer thickness WES - Experimental validation of a ducted wind turbine design strategy View original
Is this image relevant?
WES - Laminar-turbulent transition characteristics of a 3-D wind turbine rotor blade based on ... View original
Is this image relevant?
WES - Experimental validation of a ducted wind turbine design strategy View original
Is this image relevant?
1 of 3
Defined as the distance from the surface where the velocity reaches 99% of the freestream value
Increases with distance from the leading edge of the surface
Affected by factors such as Reynolds number , pressure gradient, and surface roughness
Boundary layer separation
Occurs when the boundary layer detaches from the surface due to adverse pressure gradient
Leads to increased drag, reduced lift, and flow instability
Can be delayed or prevented by using flow control techniques such as suction or vortex generators
Turbulent boundary layer structure
Consists of distinct regions with different flow characteristics and scaling laws
Dominated by turbulent mixing and momentum transfer across the layer
Inner vs outer region
Inner region close to the wall where viscous effects are dominant and velocity scales with wall units
Outer region further from the wall where turbulent mixing dominates and velocity scales with boundary layer thickness
Overlap region in between where both scaling laws apply
Viscous sublayer
Thin layer closest to the wall where viscous stresses dominate and velocity profile is linear
Velocity scales with wall units u + = y + u^+ = y^+ u + = y +
Typically extends up to y + ≈ 5 y^+ \approx 5 y + ≈ 5
Buffer layer
Transition region between the viscous sublayer and the logarithmic layer
Velocity profile deviates from the linear and logarithmic laws
Extends from y + ≈ 5 y^+ \approx 5 y + ≈ 5 to y + ≈ 30 y^+ \approx 30 y + ≈ 30
Logarithmic layer
Region where the velocity profile follows a logarithmic law u + = 1 κ ln y + + B u^+ = \frac{1}{\kappa} \ln y^+ + B u + = κ 1 ln y + + B
κ \kappa κ is the von Karman constant ( ≈ 0.41 ) (\approx 0.41) ( ≈ 0.41 ) and B B B is a constant ( ≈ 5.2 ) (\approx 5.2) ( ≈ 5.2 )
Extends from y + ≈ 30 y^+ \approx 30 y + ≈ 30 to y / δ ≈ 0.2 y/\delta \approx 0.2 y / δ ≈ 0.2
Overlap region
Region where the inner and outer scaling laws overlap
Velocity profile follows a power law u / U ∞ = ( y / δ ) α u/U_\infty = (y/\delta)^\alpha u / U ∞ = ( y / δ ) α
α \alpha α is a constant that depends on the pressure gradient and Reynolds number
Turbulent boundary layer equations
Governing equations for turbulent boundary layers derived from the Navier-Stokes equations
Require modeling of the turbulent stresses to close the system of equations
Reynolds-averaged Navier-Stokes equations
Obtained by decomposing the velocity and pressure fields into mean and fluctuating components
Result in additional terms called Reynolds stresses that represent the effect of turbulent mixing
Require modeling to close the system of equations
Closure problem
Arises because there are more unknowns than equations in the Reynolds-averaged Navier-Stokes equations
Requires modeling of the Reynolds stresses using turbulence models such as eddy viscosity models or Reynolds stress models
Choice of turbulence model depends on the flow configuration and desired accuracy
Turbulent boundary layer parameters
Various dimensionless parameters that affect the structure and behavior of turbulent boundary layers
Used to characterize the flow and compare results from different experiments and simulations
Reynolds number effects
Turbulent boundary layers become thicker and more energetic as the Reynolds number increases
Viscous sublayer and buffer layer become thinner relative to the boundary layer thickness
Turbulent mixing and momentum transfer increase with Reynolds number
Pressure gradient effects
Favorable pressure gradient (decreasing pressure in the flow direction) leads to a thinner boundary layer and delayed separation
Adverse pressure gradient (increasing pressure in the flow direction) leads to a thicker boundary layer and earlier separation
Zero pressure gradient corresponds to a boundary layer with constant thickness
Surface roughness effects
Roughness elements on the surface can trigger transition to turbulence and increase turbulent mixing
Roughness increases the skin friction drag and heat transfer at the surface
Effect of roughness depends on the size and shape of the roughness elements relative to the boundary layer thickness
Turbulent boundary layer measurements
Experimental techniques used to measure velocity, pressure, and temperature in turbulent boundary layers
Provide data for validating turbulence models and studying the physics of turbulent flows
Hot-wire anemometry
Measures velocity by sensing the change in resistance of a thin wire exposed to the flow
Provides high temporal resolution but limited spatial resolution
Requires careful calibration and correction for temperature effects
Particle image velocimetry
Measures velocity by tracking the displacement of tracer particles in the flow
Provides high spatial resolution but limited temporal resolution
Requires optical access to the flow and careful seeding of tracer particles
Turbulent boundary layer control
Techniques used to manipulate the structure and behavior of turbulent boundary layers
Aim to reduce drag, enhance heat transfer, or delay separation
Passive vs active control
Passive control uses fixed geometric modifications such as riblets or vortex generators
Active control uses dynamic actuation such as suction, blowing, or wall motion
Active control can adapt to changing flow conditions but requires energy input
Riblets
Streamwise grooves on the surface that reduce turbulent mixing and skin friction drag
Work by restricting the spanwise motion of near-wall vortices
Optimal riblet size and spacing depend on the boundary layer thickness and Reynolds number
Polymer additives
Long-chain polymer molecules added to the fluid that reduce turbulent drag
Work by suppressing near-wall turbulence and increasing the viscous sublayer thickness
Effective at low concentrations but can degrade over time and cause environmental issues
Suction
Removal of fluid from the boundary layer through porous walls or slots
Reduces the boundary layer thickness and delays separation
Requires careful design of the suction system to avoid flow disturbances
Turbulent boundary layer applications
Practical applications where understanding and controlling turbulent boundary layers is important
Span a wide range of fields including aerospace, automotive, and energy systems
Aerodynamic drag reduction
Reducing turbulent skin friction drag on aircraft, cars, and ships
Achieved through techniques such as riblets, polymer additives , and suction
Can lead to significant fuel savings and emission reductions
Heat transfer enhancement
Increasing turbulent heat transfer in heat exchangers, cooling systems, and combustion chambers
Achieved through techniques such as surface roughness, vortex generators, and jet impingement
Can lead to more compact and efficient heat transfer devices
Flow-induced noise reduction
Reducing turbulent noise generated by flow over surfaces such as aircraft wings, wind turbine blades, and submarine hulls
Achieved through techniques such as porous surfaces, serrations, and active flow control
Can lead to quieter and more environmentally friendly transportation systems