3.3Aircraft Drag

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    Aircraft Drag IIDEN/305

    G. Dorrington Oct. 2001

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    Drag Coefficient

    D = 1/2r U2 S CD

    = q S CD

    where D = Drag

    q = dynamic pressure = 1/2r U2

    U = velocity

    r = density

    S = wing planform area

    G. Dorrington Oct. 2001

    2s = b

    c

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    Drag Coefficient of an Aircraft

    The total drag coefficient of an aircraft (with lift)

    can also be written as:

    CD = CD0 + kPCL2 + CL2/(e p A)

    or

    CD = CD0 + k CL2/(p A) where k is typically about1.2

    G. Dorrington Oct. 2001

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    Drag of Aircraft

    The Drag of an aircraft in cruise where

    L=W can hence be written as:

    D = q S {CDo + k CL2/(p A)}

    = q S CDo + q S k (L/qS)2 /(p A)

    = q S CDo + k W2/(qS p A)= q S CDo + k W

    2/(q b2p)

    G. Dorrington Oct. 2001

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    Drag Polar

    G. Dorrington Oct. 2001

    `

    U

    D

    D = (rU2/2) S CDo + 2kW2/(rU2b2p) = AU2 + B/U2

    induced

    profile

    total

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    Zero-lift (or Profile)

    Drag of Aircraft

    CD0 = KMIS CD0i Si /S ref

    mutual interference = 1.3

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    Zero-lift (or Profile)

    Drag of Aircraft

    Dprofile = qSCD0 = KMFS qCD0i Si

    S = Sref= planform area of wing

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    Zero-lift (or Profile)

    Drag of Aircraft

    Dprofile/(qS) = CD0 = KMFS CD0i Si/S

    S = Sref= planform area of wing

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    Need for wind tunnel tests:

    empirical resultsComputational methods cannot yet predict profile drag of

    any body above Re=500,000

    Need to do wind tunnel testing: Re scaling

    Drag estimation is still a black art

    Following are some general empirical results

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    Fuselage: Bodies of Revolution

    Which body has the

    lowest drag based on

    frontal area pd2/4

    (same for all) ?

    d

    L

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    Fuselage: Bodies of Revolution

    L/d around 3-4 is best

    d

    L

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    Fuselage: Bodies of Revolution

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    Fuselage: Bodies of Revolution

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    Fuselage: Bodies of Revolution

    Based on wetted area, empirical equation:

    CD0 = Cf(1 + 1.5 (d/L)1. 5 + 7 (d/L)3 )

    where wetted area is approximately 0.85 p d l

    L

    d

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    Fuselage: Bodies of Revolution

    Based on wetted area, empirical equation:

    CD0 = Cf(1 + 1.5 (d/L)1. 5 + 7 (d/L)3 ) = Cf x form factor

    where wetted area is approximately 0.85 p d l

    L

    d

    L/d form factor

    2 2.41

    3 1.55

    4 1.30

    5 1.19

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    Fuselage: Bodies of Revolution

    For turbulent flow

    Cf= 0.455 (log 10 ReL )-2.58

    ReL = r U L/ m

    For example, at ReL = 8000,000 , Cf= 0.0031

    Re. No. Cf turbulent

    1000000 0.0045

    2000000 0.0039

    4000000 0.0035

    8000000 0.0031

    16000000 0.0028

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    Fuselage: Bodies of Revolution

    Hence if L/d = 3 :

    CD0 = 0.0031 x 1.55 = 0.0048

    based on S = 0.85 p d l

    L

    d

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    Fuselage: Bodies of Revolution

    Hence if L/d = 3 :

    CD0 = 0.0031 x 1.55 = 0.0048 based on S = 0.85 p d l

    3m

    1m

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    Fuselage: Bodies of Revolution

    Hence if L= 3m, d =1m:

    CD0 = 0.0031 x 1.55 = 0.0048 based on S = 8 m2

    Dprofile /q = 0.0048 x 8 m2 = 0.038 m2 (about 20 cm x 20 cm)

    3m

    1m

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    Fuselage: Bodies of Revolution

    Hence if L= 3m, d =1m:

    CD0 = 0.0031 x 1.55 = 0.0048 based on S = 8 m2

    Dprofile /q = 0.0048 x 8 m2 = 0.038 m2 (about 20 cm x 20 cm)

    3m

    1m

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    Fuselage: Bodies of Revolution

    Hence if U = 39 m/s , at sea level:

    Dprofile = 36 N , Pprofile = Dprofile U = 1.4 kW

    3m

    1m

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    Wing Profile Drag

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    Wing Profile Drag

    t

    c

    CD0 = Cf(1+ 2 t/c + 60 (t/c)4)

    based on wetted area = 2.2 S

    hence if t/c =0.15, CD0 = 1.33 Cf

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    Wing Profile Drag

    if t/c =0.15, CD0 = 1.33 Cf

    and if the flow is fully turbulent

    Cf = 0.455 (log10 Rec)-2.58

    where Rec = r U c / m

    t

    c

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    Wing Profile Drag

    if t/c =0.15, CD0 = 1.33 Cf

    and Reynolds number = 1000,000

    CD0 = 0.0045 x1.33 = 0.006

    based on wetted area Si = Swet = 2.1 S

    so based on S = Splanform

    CD0 = 0.006 x 2.1 = 0.0125

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    Wing Profile Drag

    if t/c =0.15, CD0 = 1.33 Cf

    But flow is fully laminar

    Cf = 1.328 Rec-1/2

    where Rec = r U c / m < 300,000

    t

    c

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    Wing Profile Drag

    if t/c =0.15, CD0 = 1.33 Cf

    and Rec=300,000fully laminar

    Cf = 1.328 Rec-1/2 = 0.0024

    CD0 = 0.0032 based on wetted area

    = 0.0068 based on planform area

    t

    c

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    Wing Profile Drag

    if t/c =0.15, CD0 = 1.33 Cf

    but flow is mixed laminar and turbulent

    Laminar BLTurbulent BL

    Transition

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    Wing Profile Drag

    Laminar BLTurbulent BL

    Transition

    Cf S = 0.455 (log10 Rec)-2.58 S

    - 0.455 (log10 Rex)-2.58 S x/c

    + 1.328 Rex -1/2 S x/c

    x Rex = Recrit = 300000

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    Wing Profile Drag

    At Rec= 600,000

    Cf S = 0.0049 S

    - 0.0057S x/c

    + 0.0024 S x/c

    x Rex = Recrit = 300000

    x = Recritm/rU

    c = Recm/rU

    x/c= Recrit /Rec

    = 0.5

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    Wing Profile Drag

    At Rec = 600,000

    Cf S = 0.0031 S

    - 0.0057S /2

    + 0.0024 S /2

    x Rex = Recrit = 300000

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    Wing Profile Drag

    At Rec = 600,000

    Cf S = (0.0031 - 0.00165) S = 0.00145 S

    x Rex = Recrit = 300000

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    Total Profile Drag

    D = q S CD0 = KMI {q S C D0 wing+ q S tail C D0 tail

    + q S fuselage C D0 fuselage ..}

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    Design ImplicationsIf significant natural laminar flow is feasible, then

    note advantage to keep chord c low to maximise

    laminar chord fraction x/c

    Implies high Aspect Ratio A = b2

    /S

    To reduce profile drag:

    reduce wing area S

    reduce wetted area of fuselage and control surfacesetc., keep streamline - reduce parasitic drag (rivets

    etc.), keep surfaces smooth

    keep aircraft small

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    End

    See exercises in gstutor

    G Dorrington Oct 2001