ME 408 Fluid Mechanics II Chapter 9 Flow Over Immersed Bodies
Dec 19, 2015
ME 408 Fluid Mechanics II
Chapter 9
Flow Over Immersed Bodies
Content
• Classification of External Viscous Flow
• Fluid Dynamic Forces: Lift and Drag
• Reynolds Number Effect
• Boundary Layer: Laminar and Turbulent
• Flow Separation
• Experimental Drag Data
• Airfoil and Wing Characteristics
09_01
Flow Classification
2-Dimensional:
Axi-symmetric:
3-Dimenstional:
09_04
Reynolds Number Effect
The Reynolds number, Re = U l/, is the ratio between the inertial force and the viscous force.
Low Re: Mostly viscous flow
Moderate Re: Partial viscous flow around body
High Re: Viscous Boundary Layer near surface
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Flow Past Cylinder
Low Re: Mostly viscous flow
Moderate Re: Partial viscous flow around body with separation and re-circulation flow in wake
High Re: Viscous Boundary Layer near surface till separation and wake
09_03
Surface Forces
Pressure: Normal to surface
Shear Stress: Tangent to surface
09_02
Lift and Drag
The sum of forces due to pressure distribution and skin friction (shear stress) is the resultant force on a 2-D object.
This net force can be represented by its two components:
Lift: Component normal to the flow
Drag: Component in the flow direction
E_09_01
Example 9.1 (p. 329)
Flow parallel to flat plate
Skin Friction Drag only:D = 0.0992 lbf, L = 0
Flow normal to flat plate:
Pressure Drag onlyD = 55.6 lbf, L = 0
Flow at an angle with plate:
Both Lift and Drag are present.
Drag consists of both pressure drag and skin friction drag.
Boundary Layer Flow Along a Smooth Flat Plate
Experimental observation:At local Reynolds number (Rex = U x/) around 5x105, transition from Laminar to Turbulent Boundary Layer Flow occurs. This Rex of 5x105 is known as the critical or transitional Reynolds number.
Velocity Profiles
The gradient (du/dy) of the turbulent velocity profile at the wall (y=0) is higher than that of the laminar velocity profile.
Hence skin friction drag of turbulent boundary layer is higher than that of laminar one.
09_08
Boundary layer thickness (x): The location normal to surface at which the velocity reaches 0.99 of the velocity U in the inviscid free-stream. It increases in the x-direction along the plate.
Displacement thickness *(x): The distance normal to the surface that the streamline passing (x) is displaced from its original distance (h) at the leading edge of the plate. Hence,
*(x) = (x) – h
Laminar Boundary Layer on Flat Plate
• Blasius Solution
• Momentum Integral Method
Curve fit formula for turbulent boundary layer (Re > 500,000):
Experimental Skin Friction Drag Data
09_10
Drag Coefficientof Flat Plate
with Roughness
Curve fitting ofExperimental Data
Drag Coefficient of Flat Plate
Empirical Formulas
Boundary Layer Flow Separation
When flow separation occurs, there is also pressure drag.
100% Pressure Drag
Pressure (Form) Drag due to Flow Separation
Total Profile Drag= Skin Friction Drag
+ Form Drag
09_12
Development of velocity profile in
the boundary layer on curved surface:
Flow separation occurs when the gradient of the
velocity profile at the wall is zero,
forming a re-circulating wake
downstream.
Wind Tunnel Tests
Force transducer behind model senses lift, drag and pitching moment directly.Motor-controlled mechanism adjusts the model’s angle of attack.
Typical Experimental Data
Notice the sudden drop at the transition Re of 5x105 (Point E)
For Re > 5x105, the boundary is turbulent, which has a fuller velocity profile.
Flow separation is delayed, resulting in a smaller wake, and hence the pressure drag.
Adding surface roughness on circular and spherical shapes triggers turbulence at lower Re, and hence helps to reduce the drag coefficient
Benefit of Streamlining
Pressure drag is greatly reduced by preventing flow separation using a gradually tapering tail. Though skin friction increases with larger area, the total drag is much less. Hence streamlined bodies are made of smooth surfaces to reduce skin friction.
These objects have approximately the same drag:
Test Data of 2D Objects
Test Data ofAxi-Symmetric Objects
Test Data of 3D Objects
Recommended films:
http://web.mit.edu/hml/ncfmf.html
Fluid Dynamics of Drag Part I-IV
Airfoil Characteristics
09_25