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    Flat Plate Drag

    Drag on flat plate is solely due to friction createdby laminar, transitional, and turbulent boundarylayers.

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    Flat Plate Drag

    Local friction coefficient

    Laminar:

    Turbulent:

    Average friction coefficient

    Laminar:

    Turbulent:

    For some cases, plate is long enough for turbulent flow,but not long enough to neglect laminar portion

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    Effect of Roughness

    Similar to MoodyChart for pipe flow

    Laminar flow

    unaffected byroughness

    Turbulent flowsignificantly affected:Cf can increase by 7xfor a given Re

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    Cylinder and Sphere Drag

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    Cylinder and Sphere Drag

    Flow is strong function ofRe.

    Wake narrows forturbulent flow since TBL(turbulent boundary layer)is more resistant toseparation due toadverse pressure

    gradient. sep,lam 80

    sep,lam 140

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    Effect of Surface Roughness

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    Lift

    Lift is the net force(due to pressure andviscous forces)perpendicular to flowdirection.

    Lift coefficient

    A=bc is the planformarea

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    Computing Lift

    Potential-flow approximation givesaccurate CL for angles of attack belowstall: boundary layer can be neglected.

    Thin-foil theory: superposition of uniform

    stream and vortices on mean camber line. Java-applet panel codes available online:

    http://www.aa.nps.navy.mil/~jones/online_tools/panel2/

    Kutta conditionrequired at trailing edge:

    fixes stagnation pt at TE.

    http://www.aa.nps.navy.mil/~jones/online_tools/panel2/http://www.aa.nps.navy.mil/~jones/online_tools/panel2/http://www.aa.nps.navy.mil/~jones/online_tools/panel2/http://www.aa.nps.navy.mil/~jones/online_tools/panel2/
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    Effect of Angle of Attack

    Thin-foil theory shows thatCL2 for < stall

    Therefore, lift increases

    linearly with

    Objective for most

    applications is to achievemaximum CL/CD ratio.

    CDdetermined from wind-tunnel or CFD (BLE or NSE).

    CL/CD increases (up to order100) until stall.

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    Effect of Foil Shape

    Thickness andcamber influencespressure distribution(and load distribution)and location of flowseparation.

    Foil databasecompiled by Selig(UIUC)http://www.aae.uiuc.edu/m-selig/ads.html

    http://www.aae.uiuc.edu/m-selig/ads.htmlhttp://www.aae.uiuc.edu/m-selig/ads.htmlhttp://www.aae.uiuc.edu/m-selig/ads.htmlhttp://www.aae.uiuc.edu/m-selig/ads.htmlhttp://www.aae.uiuc.edu/m-selig/ads.htmlhttp://www.aae.uiuc.edu/m-selig/ads.html
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    Effect of Foil Shape

    Figures from NPS airfoil javaapplet.

    Color contours ofpressure field

    Streamlines throughvelocity field

    Plot of surface pressure Camber and thickness shown

    to have large impact on flowfield.

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    End Effects of Wing Tips

    Tip vortex created byleakage of flow from high-pressure side to low-pressure side of wing.

    Tip vortices from heavyaircraft persist fardownstream and posedanger to light aircraft.

    Also sets takeoff andlanding separation atbusy airports.

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    End Effects of Wing Tips

    Tip effects can bereduced by attachingendplatesor winglets.

    Trade-off betweenreducing induceddrag and increasingfriction drag.

    Wing-tip feathers onsome birds serve thesame function.

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    Lift Generated by Spinning

    Superposition of Uniform stream + Doublet + Vortex

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    Lift Generated by Spinning

    CL strongly depends on rateof rotation.

    The effect of rate of rotation

    on CD is small. Baseball, golf, soccer,

    tennis players utilize spin.

    Lift generated by rotation iscalled The Magnus Effect.