Diagnostic Investigation of Aircraft Performance at Different Winglet Cant Angles

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      World Academy of Science, Engineering and Technology

    International Journal of Mechanical, Aerospace, Industrial, Mechatronic and Manufacturing Engineering Vol:8, No:12, 2014

    Diagnostic Investigation of Aircraft Performance atDifferent Winglet Cant Angles

    Dinesh M., Kenny Mark V., Dharni Vasudhevan Venkatesan, Santhosh Kumar B., Sree Radesh R., V. R. Sanal Kumar

     The induced drag is a different type of drag. It is caused by the

    AbstractÐComprehensive numerical studies have been carriedpressure imbalance at the tip of a finite wing between its upper

    out to examine the best aerodynamic performance of subsonic aircraft(pressure side) and lower (suction side) surfaces. That

    at different winglet cant angles using a validated 3D k-w SST model.imbalance is necessary in order to produce a positive lift force.

    In the parametric analytical studies NACA series of airfoils are  Ho 

    ever, near the tip the high pressure air from the lo 

    er sideselected. Basic design of the   inglet is selected from the lite

    rature4 and flo   features of the entire   ing including the   inglet tip effects

    tends to move up  ards,   here the pressure is lo   er, causing60 have been examined   ith different cant angles varying from 150 to the streamlines to curl (see Fig. 1). This three-dimensional00 0 00 60 at different angles of attack up to 14 . We have observed, among

    motion leads to the formation of a vortex,   hich alters the

    01 0/ the cases considered in this study that a case,   ith 15 cant angle the

    flo 

     field and induces a velocity component in the do 

    ardnoi aerodynamics performance of the subsonic aircraft during takeofft

    direction at the   ing, called do   n   ash [2]-[4]. The induceda 0c   as found better up to an angle of attack of 2.8 and further itsi

    lflo   pattern causes the relative velocity to cant do   n   ards at

    b performance got diminished at higher angles of attack. AnalysesuP 00 each airfoil section of the   ing, thus reducing the apparent/ further revealed that increasing the

     

    inglet cant angle from 15 to 60gr

    angle of attack. The lift vector is tilted back  ards and a force

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     o. at higher angles of attack could negate the performance deteriorationtes and additionally it could enhance the peak C /C on the orderof component in the direction of the drag appears, called induceda L D    3.5%. The investigated concept of variable-cant-angle   inglets drag. Reducing the size of this tip vortex and minimizing the41 appears to be a promising alternative for improving the aerodynamic0

    induced drag is of great importance for the modern aircraft2, efficiency of aircraft.2

    designers. For this purpose designers developed the 

    inglet1:o

    concept. Winglets are specially designed extensions adjustedN, Key

     

    ordsÐAerodynamic efficiency, Cant-angle, Drag8

    to the 

    ingtip that alter the velocity and pressure field and

    : reduction, Flexible Winglets.lo

    reduce the induced drag term, thus increasing aerodynamicV

    gefficiency.

    ni I. INTRODUCTIONree

    n HE main purpose of any   inglet is to improve the aircraftign Tperformance by reducing its drag [1]-[25]. The termE

    la   inglet   as previously used to describe an additional liftingcina surface on an aircraft. Wingtip devices are usually intended to

    hce improve the efficiency of fixed-

     

    ing aircraft [1]. There areM

    d several types of   ingtip devices, and although they function innae different manners, the intended effect is al  ays to reduce thec

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     a aircraft's drag by partial recovery of the tip vortex energy.psor Wingtip devices can also improve aircraft handling

    eA, characteristics and enhance safety. Such devices increase thexed effective aspect ratio of a

     

    ing 

    ithout materially increasing

    nIe the   ingspan. Note that an extension of span   ould reduce the

    Fig. 1 Demonstrating the tip vortex of a fixed 

    ing aircraftcne lift-induced drag, but   ould increase parasitic drag and   ould

    ic

    S require boosting the strength and 

    eight of the 

    ing.Bourdin et al. [5] reported that the investigated concept oflan It is   ell kno   n that any sort of body exposed in a viscous

    variable-cant-angle   inglets appears to be a promisingoita flo    experiences profile drag,   hether it produces lift or not.

    alternative to conventional control surfaces such as ailerons,nr

    etelevators, and rudders as far as basic maneuvers are

     nI

    Dinesh   as an undergraduate student of Aeronautical Engineering, concerned. The concept consists of a pair of

     

    inglets 

    ithKumaraguru College of Technology, Coimbatore ± 641 049, Tamil Nadu,

      adjustable cant angle, independently actuated and mounted atIndia; (e-mail: [email protected]).

    Kenny Mark, Dharni Vasudhevan, Santhosh Kumar, and Sree Radesh arethe tips of a baseline flying   ing. A potential application for

    Undergraduate Students of Mechanical Engineering, Kumaraguru College ofthe adjustable   inglets   ould be for surveillance aircraft, forTechnology, Coimbatore ± 641 049, India (Phone: +91-9894467086, e-

      hich enhanced lo   -speed maneuverability is required. Notemail:[email protected],[email protected],[email protected], [email protected]).

    that deflecting a 

    inglet 

    hen the 

    ing is flying near its stallSanal Kumar is Professor and Aerospace Scientist and currently   ith th

    e angle is unlikely to cause the   ing to stall (in contrast to thedepartment of Aeronautical Engineering, Kumaraguru College of Technology,

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      effect of an aileron). Hence, variable cant-angle   inglets canCoimbatore ± 641 049, Tamil Nadu, India; (Corresponding Author, ph

    one: be used for effective lo  -speed roll control (instead of spoilers+91 ± 938 867 9565; + 91 ± 875 420 0501, e-mail:[email protected]).

    International Scholarly and Scientific Research & Innovation 8(12) 20142052 scholar.   aset.org/1999.8/10000064

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      World Academy of Science, Engineering and Technology

    International Journal of Mechanical, Aerospace, Industrial, Mechatronic and Manufacturing Engineering Vol:8, No:12, 2014

     

    hich are traditionally preferred to ailerons in that flightbe close to its optimal efficiency. Fig. 3 found in literature isregime).

    reproduced here 

    ith for a critical revie 

    . It sho 

    s that lo 

    est

    total drag is at a particular airspeed. Note that Pilots   ill use

    this speed to maximize the gliding range in case of an engine

    failure. Ho  ever, to maximize gliding endurance, aircraft's

    speed should be at the point of minimum power, which occurs

    at lower speeds than minimum drag.

    Fig. 2 Front view of a fixed wing aircraft with fixed winglet460 Fig. 2 shows the front view of a typical aircraft with winglet000 at fixed cant angle. Numerical and experimental studies01/n conducted by the earlier investigators on a flying wing

    oit configuration showed that adjustable winglets enable controlacil moments about multiple axes, forming a highly coupled flightbuP

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    Md patented the first functional winglets in 1910. Somerville

    vortex to an apparent thrust. This small contribution can benae installed the devices on his early biplane and monoplane

    worthwhile over the aircraft   s lifetime, provided the benefitcap designs. Wingtip devices increase the lift generated at the

    offsets the cost of installing and maintaining the winglets.so wingtip (by smoothing the airflow across the upper wing nearr

    Another potential benefit of winglets is that they reduce theeA, the tip) and reduce the lift-induced drag caused by wingtip

    strength of wingtip vortices, which trail behind the plane andxe vortices, improving lift-to-drag ratio. This increases fuel

    pose a hazard to other aircraft. Minimum spacing requirementsdn

    Ie efficiency in powered aircraft and increases cross-countrybetween aircraft operations at airports is largely dictated by

    cn speed in gliders, in both cases increasing range [1].

    these factors. Aircraft are generally classified by weighteic The literature review reveals that the United States AirS

    because the vortex strength grows with the aircraft lift

    l

    a Force studies could come up with the improvement in fuelncoefficient, and thus, the associated turbulence is greatest at

    oit efficiency, which correlates directly with the causal increase ina

    low speed and high weight.nre the aircraft  s lift-to-drag ratio. In flight, induced drag resultst

    The drag reduction permitted by winglets can also reduce

    nI from the need to maintain lift. It is greater at lower speeds

    the required takeoff distance [8]. Winglets and wing fences

    where a high angle of attack is required. As speed increases,also increase efficiency by reducing vortex interference withthe induced drag decreases, but parasitic drag increases

    laminar airflow near the tips of the wing [7], by moving thebecause the fluid is striking the object with greater force, and

    confluence of low-pressure (over wing) and high-pressure

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      is moving across the object  s surfaces at higher speed. As(under wing) air away from the surface of the wing. Wingtip

    speed continues to increase into the transonic and supersonicvortices create turbulence, originating at the leading edge ofregimes, wave drag enters the picture. Each of these drag

    the wingtip and propagating backwards and inboard. Thiscomponents changes in proportion to the others based on the

    turbulence delaminates the airflow over a small triangularspeed. The combined overall drag curve therefore shows a

    section of the outboard wing, which destroys lift in that area.minimum at some airspeed; an aircraft flying at this speed will

    The fence/winglet drives the area where the vortex forms

    International Scholarly and Scientific Research & Innovation 8(12) 20142053 scholar.waset.org/1999.8/10000064

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      World Academy of Science, Engineering and Technology

    International Journal of Mechanical, Aerospace, Industria

    l, Mechatronic and Manufacturing Engineering Vol:8, No:12, 2014

    uppward away ffrom the wingg surface, sinnce the centerr of the  benefits for corrporate travell. In addition to factory-innstalled

    reesulting vortexx is now at tthe tip of thee winglet. Thheseare wiinglets on neew aircraft, aftermarket vendors devveloped

    suuccinctly reported in the opeen literature [ 1]-[25].rettrofit kits, forr popular jets and turboprops, to improvve both

    aerrodynamics annd appearancee. Winglets beecame so popuular on

    TTABLE ISPECIFICAATIONS OF WINGthiis class of airrcraft that thee Dassault Grroup, whose FFrenc

    h

    designers resistted applying them on theeir Falcon linee untilSl. No. Description Dimension

    reccently, were fforced to run aa contrarian mmarketing cammpaign.1 Airfoil Type NACA 0012

    Off late Cessna disclosed to ttest a new wingtip device called

    2 Wing Type Swept Back0

    Ellliptical Wingllets, which arre designed too increase rannge and3 Sweep Angle 32.434 Wing Span 22 cm

    inccrease payloaad on hot annd high depaartures. It hass been5 Taper Ratio 0.292553

    revvealed througgh this literatture review thhat winglet ddesigns 

    6 Aspect Ratio 3.62139

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      muust be optimizzed to be ablee to get maximmum benefits during

    27 Wing Area 133.65 cm

    cruuise and non-ccruise flight cconditions; and for that 3D design8. Maximum Chordd 9.4 cm

    opptimization is inevitable. TTherefore, 3DD numerical studies9. Minimum Chordd 2.75 cm

    4haave been carrried out for examining the possibilitties

    of600 TABLE II

    inccreasing the aaerodynamics efficiency off a typical winng with000 SPECIFICATTIONS OF WINGLEET

    vaariable-cant-anngle winglets.1/no Sl. No. Descripption Dimenssion

    ita 1 Winglet Type Blended WWingletcilb 2 Winglet Span 3 cmmuP/ 3 Winglet HHeight 3 cmmgr

    o 2

    t. 4 Winglet Area 9.255 cmce

    0 s 0

    Fig. 4 Physical model of a wwing with wingllet Cant-Angle 15a 5 Winglet Sweeep Angle 47.299w

    4 6 Winglet Tapper Ratio 0.109

    10 7 Maximumm Chord 2.75 ccm2

    , 8 Minimumm Chord 0.3 cmm21:o

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    N

    , Aircraft suchh as the Airbuus A340 and the Boeing 7747-4008:l usse winglets. OOther designs such as soome versions of theoVg Boeing 777 andd the Boeing 7747-8 omit thhem in favor oof rakednir wwingtips. Largee winglets suuch as those seen on Boeiing 737eeni aiircraft equippeed with blendeed winglets arre most usefull duringgnE shhort-distance flights, wherre increased climb perfoormance

    lac offfsets increaseed drag. Notte that the raaked wingtipss are a

    ina feeature on somee Boeing airlinners, where thhe tip of the wwing hashce a higher degreee of sweep thaan the rest of the wing. Thee statedM

    d puurpose of this additional feaature is to impprove fuel effficiencyna

    e annd climb perfoformance, andd to shorten taakeoff field length. It

    ca

    p dooes this in much the saame way thaat winglets do,byso

    Fig. 5 3-D grid system iin the computattional domainr inncreasing thee effective aspect ratio of the winng andeA

    , innterrupting haarmful wingttip vortices. This decreasses the xe

    IIII. NUMERICAL METHODOOLOGYd ammount of lift--induced dragg experiencedd by the aircraft. InnIe testing by Boeeing and NAASA, raked wwingtips havve been

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      Numerical simmulations havve been carrieed out with thhe helpcne shhown to reduuce drag by aas much as 55.5%, as oppoosed to

    of f a steady 3DD, double precision, pressuure-based, SSST k-wicS immprovements of 3.5% to 44.5% from coonventional

     

    ingletsturrbulence moddel. This moddel uses a coontrol-volume based

    lan [99]. While an eequivalent incrrease in

     

    inggspan 

    ould bbe moretecchnique to coonvert the gooverning equuations to alggebraic

    oita efffective than aa   inglet of thhe same lengtth, the bendinng force

    eqquations. The viscosity is determined ffrom the Suthherlandnret beecomes a greaater factor. AA three-foot

     

    inglet has thhe same  forrmula. The   iing geometricc variables andd material proopertiesn

    I beending force as a one-foot increase in span, yet givves thearee kno  n a priori . Initiial   all temmperature andd

    inletsaame performannce gain as a t   o-foot   ingg span increasse [10].temmperature aree specified. AAt the exit, far field bouundary

    Foor this reason,, the short-rannge Boeing 7887-3 design caalled forcondition is preescribed. At tthe solid   allls no-slip bouundary

        inglets insteaad of the rakeed   ingtips ffeatured on alll othe

    r condition is impposed. The Coourant-Friedricchs-Le  y nummber is7887 variants.chhosen as 1.0 inn all of the computations. TThe turbulent kinetic

    Winglets aree also appliedd to several oother business jets to ennergy and the specific dissippation rate aree taken as 0.88. Idealreeduce take-offff distance, ennabling operaation out of smallergaas

     

    as selectedd as the 

    orkiing fluid. Inlett velocity is taaken asseecondary airports, and alloo   ing higher cruise altituudes for55.55 m/s,   ithh turbulence iintensity of 5 %. Tables I and I

    Iovverflying bad

     

    eather, bothh of 

    hich are valuable operrationalshoo    the geommetric detailss of the   inng and the   inglet

    considered in thhis study. Fig. 4 sho   s the pphysical modeel of an

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    l, Mechatronic and Manufacturing Engineering Vol:8, No:12, 2014

    0aircraft

     

    ing 

    ith 15 

    inglet cant angle. Fig. 5 sho 

    s the 3Dgrid system in the computational domain. Grid are selectedafter a detailed grid refinement history (Cells: 140144, Faces:929653, Nodes: 780461). The grids are clustered near the solid 

    alls using suitable stretching functions. Orthogonal Qualityranges from 0 to 1,   here values close to 0 correspond to lo    quality. Minimum orthogonal quality

     

    as 7.28711 E-01 andmaximum aspect ratio   as 2.60710 E+01.

    IV. RESULTS AND DISCUSSION

    It is 

    ell kno 

    n that 

    inglets application is one of the mostFig. 8 Comparison of aerodynamic performance (C /C ) at different

    L D

    noticeable fuel economic technologies on aircraft. The angles of attack 

    ithout and 

    ith 

    inglet at different cant anglesdiagnostic investigation reveals that the   inglet designs must

    Fig. 6 sho   s the comparison of lift coefficient (C ) atbe optimized to be able to get maximum benefits during cruise

    L4

    different angles of attack   ithout and   ith   inglet orienting at6 and non-cruise flight conditions. In this paper comprehensive0

    0 0 0 0

    0 four different cant angles viz., 15 , 30 , 45 and 60 . It is0 numerical studies have been carried out to examine the best0

    00

    evident from Fig. 6 that a case 

    ith cant angle 60 is giving the1 aerodynamic performance of subsonic aircraft at different/n

    highest coefficient of lift at various angles of attack (0-14).

    inglet cant angles using a validated 3D k-w SST model. Inita

    Nevertheless, as evident in Fig. 7, this trend is not seen   hileci the parametric analytical studies NACA series of airfoils arelb

    comparing the drag coefficient (C ) at different angles of

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     u selected. Basic design of the   inglet is selected from theD

    P0

    /g literature and flo

     

     features of the entire 

    ing including the tipattack. One can discern from Fig. 7 that a case   ith 60 c

    antro.

    0 0t effects have been examined

     

    ith different cant angles varyingangle CD is relatively high up to 2.8 than a case   ith 15 c

    antes

    0a 0 0 0

    angle and further it diminishes up to 12 angle of attack and 

      from 15 to 60 at different angles of attack up to 14 .4

    again it increases due to change in flo 

      features. These10

    2

    variations are corroborated   ith C /C curves,   hich are,

    L D21

    sho  n in Fig. 8. It is evident from Fig. 8 that aerodynamic:oN

    0

    , performance of an aircraft   ith   inglet at a cant angle of 158

    0

    :l

    is giving better performance up to an angle of attack 2.8andoV

    0g

    further a case 

    ith 

    inglet cant angle of 60 is giving betterni

    performance due to the change in overall flo    features and thereen

    corresponding drag coefficient variation as discussed in the

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    ign

    previous session. Fig. 9 sho   s the reference plane taken forE

    la

    generating numerical results for comparison. Figs. 10-17 sho   cin

    the pressure and velocity contours corresponding to theahce

    reference plane sho 

    n in Fig. 9 at t 

    o different cant anglesMd

    and various angles of attack.nae Fig. 6 Comparison of lift coefficient (CL) at different angles of attack

    In the parametric analytical studies NACA series of airfoilsca   ithout and   ith   inglet at four different cant angles

    are selected. Basic design of the   inglet is selected from thepsor

    literature and flo   features of the entire   ing including the tipeA,

    effects have been examined   ith different cant angles varying

    x 0 0 0e

    from 15 to 60 at different angles of attack up to 14 . We havednIe

    observed, among the cases considered in this study that a casec

    0n

      ith 15 cant angle the aerodynamics performance of the

    eic

    0S

    subsonic aircraft during takeoff 

    as found better up to 2.8lan

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      angles of attack and further its performance got diminished atoita

    higher angles of attack. Analyses further revealed thatnr

    0 0e

    increasing the 

    inglet cant angle from 15 to 60 at highertnI

    angles of attack could negate the performance deterioration

    and additionally it could enhance the peak value of C /C on

    L D 

    the order of 3.5 %. A 

    inglet's main purpose is to improve

    performance by reducing drag. To understand how this is

    done, it is first necessary to understand the distinction betweenFig. 7 Comparison of drag coefficient (CD) at different angles of

    attack without and with winglet at four different cant anglesprofile drag and induced drag. Profile drags is a consequence

    of the viscosity, or stickiness, of the air moving along the

    surface of the airfoil, as well as due to pressure drag (pressure

    forces acting over the front of a body not being balanced by

    those acting over its rear). As a wing moves through viscous

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      aiir, it pulls somme of the air along with it,, and leaves ssome ofthhis air in motioon. Clearly, it takes energy to set air in mmotion.

    0

    (d) Anglee of attack = 6

    Fig. 9 The selected refereence plane for reesults generatioon

    46000001

    /noitacilbuP/

    gro.tesaw

    4

    102

    ,21

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     :o

    0N

    (e) Anglee of attack = 8, 0

    8 (a) Anglee of attack = 0:

    00l

    Fig. 10 (a)-(ee) Pressure conttours (Pascal) aat cant angle 15 atoVg

    symmmetry plane withh different anglees of attacknir

    een

    ignE

    lacinahc

    eM

    dna

    ecapso

    re

    A

    ,x

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     ed

    n

    I00

    e (b) Anglee of attack = 20

    c(a) Anglee of attack = 0

    neic

    S

    lanoi

    tanretnI

    0(c) Anglee of attack = 4

    0

    (b) Anglee of attack = 2

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    00

    (c) Anglee of attack = 4(b) Anglee of attack = 2

    4600

    0001/noitacil

    buP/gro.tesaw

    410

    2

    ,

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     21 00: (d) Anglee of attack = 6

    oN

    0

    ,(c) Anglee of attack = 4

    8:lo

    V

    gniree

    nignE

    lacinah

    ceM

    dna

    ecaps

    ore

    Ax, (e) Anglee of attack = 80

    0e

    (d) Anglee of attack = 6d

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     n 0I Fig. 11 (a)-(e) Pressure conntours (Pascal) aat cant angle 155 at

    ec refereence plane withh different anglees of attackneicS

    lanoitanretnI

    0

    (e) Anglee of attack = 8

    00

    Fig. 12 (a)-(ee) Pressure conttours (Pascal) aat cant angle 60at

    (a) Anglee of attack = 00symmmetry plane withh different anglees of attack

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    (a) Anglee of attack = 000

    (e) Anglee of attack = 8

    004

    Fig. 13 (a)-(ee) Pressure conttours (Pascal) aat cant angle 60 at60

    refereence plane with different anglees of attack

    000

    01/noitac

    ilbuP/gro.tes

    aw

    4102

    ,2

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     1

    :oN, (b) Anglee of attack = 2008:loV

    g0

    n(a) Anglee of attack = 0

    ire

    enig

    nE

    lacinahceM

    dna

    ecapsore

    A

    ,

    x

    ed (c) Anglee of attack = 40

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     nI

    e

    cn

    0e

    (b) Anglee of attack = 2icS

    lanoitan

    retnI

    (d) Anglee of attack = 600

    0

    (c) Anglee of attack = 4

    International Scholarly and Scientific Research & Innovation 8(12) 2014

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    (d) Angle of attack = 600

    (c) Angle of attack = 4

    460000

    01/noitacilbu

    P/gro.tesaw

    4

    1

    0

    2

    , 021 (e) Angle of attack = 8

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     nI

    eFig. 15 (a)-(e) Velocity contours (meters per second) at cant angl

    ec (a) Angle of attack = 00

    0n

    15 at reference plane with different angles of attackeicS

    lanoitan

    retnI

    0(b) Angle of attack = 20

    (a) Angle of attack = 0

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    00(b) Anglee of attack = 2

    0

    (a) Anglee of attack = 0

    460000

    01/noitacilbu

    P/gro.tesaw

    4

    102

    ,2 01 (c) Anglee of attack = 4

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    :oN

    0,

    (b) Anglee of attack = 28:lo

    V

    gnireenig

    nE

    lacinahceM

    dna

    ecap

    so

    re

    A

    , 00x (d) Anglee of attack = 6

    0e

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      (c) Anglee of attack = 4dnI

    ecneicS

    lanoitanre

    tnI

    0(e) Anglee of attack = 8

    0Fig. 16 (a)-(e) VVelocity contouurs (meters per second) at cantt angle

    (d) Anglee of attack = 6

    060 at syymmetry plane wwith different aangles of attack

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    International Scholarly and Scientific Research & Innovation 8(12) 20142061 scholar.waset.org/1999.8/10000064