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  • 8/10/2019 FAST Conference 2013 Paper ID 61 -The Wageningen C- And D-Series Propellers - Final Version

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    The Wageningen C- and D-Series Propellers

    J. Dang, MARIN, The Netherlands

    H. J. J. van den Boom, MARIN, The Netherlands

    J. Th. Ligtelijn, MARIN, The Netherlands

    SUMMARY

    The Maritime Research Institute Netherlands (MARIN) has recently started a Joint Industry Project (JIP) on developing

    two new propeller series for Controllable Pitch Propellers (CPPs). Following the well known Wageningen B-series and

    Ka-series, the new C-series comprise open CPPs whereas the newD-series concern ducted CPPs.The primary objective

    of developing the new CPP series is to help the shipbuilding and offshore industries in understanding the off-design per-

    formance of the CPPs, for which systematic information was lacking.

    CPP blades have been generated for 4- and 5-bladed open propellers and for 4-bladed ducted propellers in two ducts,

    representing the most contemporary propeller design practice. Systematic measurements of the propeller and duct

    thrusts, the torque and also the blade spindle torque have been carried out for the entire range of operational conditions

    and pitch-settings of each propeller. The results of the C4-40 series are presented in this paper as an example case.

    1. INTRODUCTION

    The Maritime Research Institute Netherlands (MARIN),

    former Netherlands Ship Model Basin (N.S.M.B.),

    started to develop the well-known Wageningen B-seriesPropellers right from the establishment of this institute in

    1932 [1]. The first series were published by van Lam-

    meren [2] and Troost [3,4], followed by further devel-

    opments and expansions of the series over more than 40

    years. A major review of the available data was given by

    van Lammerenet al[5,6]. The B-series had been furtherextended to 6 and 7 bladed propellers in the 1970s. To-

    tally, 20 series with more than 120 propellers were tested

    over that period.

    Systematic series have also been developed for ducted

    propellers since 1954 [7]. A major amount of data of theKa-series were published by Oosterveld [8]. In the mean-

    time, other systematic propeller series were also devel-

    oped worldwide, such as the Taylor- [9], Gawn- [10],

    (M)AU- [11] and SSPA- [12,13] series. However, in prac-

    tise the B-series data are among the most widely used in

    the industry.

    Besides that most of the propeller characteristics (the

    thrust and the torque) of the series in design operation

    condition have been made available by model tests be-

    tweenJ=0 andKT=0, four-quadrant open water character-istics of some of the propellers in the B-series and the

    ducted propellers in the Ka-series were also made avail-

    able in the 1980s [14] for off-design conditions. Table 1

    provides an overview of the propellers in theB-series, of

    which 4-quadrant open water characteristics are avail-

    able. For the Ka-series, only Ka 4-70 propellers in 19Aand 37 ducts have been published [1].

    Different from Fixed Pitch Propellers (FPPs), Controlla-

    ble Pitch Propellers (CPPs) are well-known for their ad-

    vantage for full power utilization at any circumstances:

    accelerating and stopping, rapid manoeuvring, dynamic

    positioning (DP), etc. For these reasons, CPPs are widely

    used for multi-purpose vessels where their propulsors are

    often used in off-design conditions.

    Table 1 Overview of B-series with four-quadrant open

    water characteristics (pitch ratioP/Dof the propellers are

    listed in the table).

    AE/A0 [%] 40 55 65 70 75 80 85 100

    Z=3 1.0

    Z=4 1.0 1.00.5, 0.6, 0.8

    1.0, 1.2, 1.41.0 1.0

    Z=5 1.0

    Z=6 1.0

    Z=7 1.0

    In order to predict the performance of a CPP in off-

    design conditions, people have to either carry out dedi-

    cated and expensive measurements for a specific propel-ler design, such as often done for navy vessels [15,16], or

    rely on the estimated values from the existing four-

    quadrant open water data from the B-series [17], which

    were primarily designed for merchant ships with FPP

    blade forms. Information for the complete two-quadrant

    open water characteristics of CPPs in the public domainis scarce, especially when the propeller blades are de-

    flected away from their design pitch [18,19]. In the

    Wageningen series book [1], off-design information is

    only available for two CPPs in ahead and astern condi-

    tions, one with a design pitch ratio of zero and the other

    of one.

    With the deployment of more and more vessels with DP-

    capability, accurate prediction of the off-design perform-

    ance of a propulsor becomes more important than ever.

    Dedicated tests for each propeller design is unaffordable

    for most of the projects, while the existing limited infor-

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    mation is far from enough. For this reason there is a

    strong demand for systematic data on the performance ofCPPs in off-design conditions.

    In addition to these, a CPP blade has a completely differ-

    ent blade form than an FPP. This is because more practi-

    cal issues need to be considered for a CPP, such as: theblades must be able to pass each other from positivepitch to negative pitch, the blade has to be positioned

    properly between the bolt holes on the blade foot, the

    cavitation performance must be acceptable for a wide

    range of operational pitch settings, the blade overhang at

    the blade foot should preferably be avoided to prevent

    stress concentration; the blade tips must not touch the

    inner side of a duct at any deflected pitch angles for the

    ducted CPPs. Besides all these constraints, one of the

    important and unique issues is the blade spindle torque of

    CPPs [20], where very limited information can be found

    [19,21,22]. To the knowledge of the authors, there is also

    no CPP series with systematic information on the propel-ler blade spindle torque at all possible blade pitch set-

    tings (from full positive pitch to full negative pitch and

    over the complete two quadrants). Also no systematic

    information is available on blade feathering performance.

    In close co-operation with industry and universities

    MARIN started to explore the possibilities for develop-

    ing new systematic series for both open and ducted

    CPPs. In September 2011, a Jointed Industry Project

    (JIP) was officially launched, which is called the Wagen-

    ingen C- and D-series Propellers for CPPs and ductedCPPs, respectively. Here the C stands for controllable

    and theDstands for ducted.

    Conducting conventional open water tests for an exten-

    sive propeller series in two quadrants is not economically

    feasible as each propeller has to be tested at more than 10

    pitch settings between full positive and full negative

    pitch. New test technology had to be developed in order

    to reduce the test time significantly. This leads to the idea

    of a quasi-steady test technique for propeller open water

    characteristics which is enabled by the new sensor tech-nology that allows high frequent dynamic measurement

    with rapid response.

    Under support of the Wageningen C-series and D-seriesJIP, a pilot study has been successfully carried out to

    explore the possibility of using this technique. The study

    proved that the quasi-steady test results are as accurate as

    the conventional steady test results, while reducing the

    test time by a factor of 8 to 10 [23]. This technology de-velopment enabled the JIP to test large systematic series

    within reasonable budget.

    The propeller series, the blade design methodology, the

    parameterization of the propeller geometry, the test pro-

    cedures, the data analyses and the presentation of the

    results are discussed in the following sections. At the end

    of the paper, the complete test results of the C4-40 seriesare presented and discussed.

    2. DESIGN METHODOLOGY, THE PRO-

    PELLER SERIES AND THE TEST MATRIX

    In order to obtain systematic information on propeller

    open water characteristics, the WageningenB-series Pro-

    pellers were designed in such a way that the number of

    blades, the blade area ratio and the pitch-diameter ratiowere systematically varied, while the blade contour, theskew distribution, the pitch distribution (constant, except

    for the 4-bladed), the rake angle (15o), the hub-propeller

    diameter ratio (1/6, except for the 3-bladed propellers

    which has a ratio of 18%) and the section profiles are all

    kept the same for the whole series [1].

    While designing the Wageningen C- andD-series propel-

    lers, an extensive propeller database search has been car-ried out first. A large number of practical propeller de-

    signs, made with up-to-date hydrodynamic knowledge

    was gathered. Studies have been carried out to relate the

    propeller main dimensions to the typical applications, sothat each design of the blades reflects a certain scenario

    of a typical application. For instance, a 4-bladed CPPwith large blade area and high pitch ratios is often used

    for the fast ferries and cruise ships where the comfort is

    weighted more than the efficiency; a 4-bladed CPP with

    small blade area and low pitch ratios is typically used by

    transport ships with a large amount of harbour activities,

    such a shuttle tanker, where the propulsive efficiency isessentially important, rather than the comfort. The 5-

    bladed CPP designs are aimed at applications for the

    navies.

    The statistics from the database also showed that the CPPhub size changes noticeably with the blade area ratio and

    the blade design pitch ratio for open propellers. This is

    because these main parameters of a propeller are closelyrelated to the power density on the blade, which deter-

    mines how strong a hub should be and how large the

    pitch actuating system should be. However, this tendency

    is not found for the ducted CPPs. These findings are ap-

    plied to the present series designs where the C-series has

    different hub-propeller diameter ratios for each propellerdesign; while theD-series propellers have the same hub-

    propeller diameter ratio for all designs.

    Thereafter, each propeller in the series was designed in-dividually with the best present design practice with the

    compromise between efficiency, comfort and mechanical

    requirements, which comprise the blade strength re-

    quirements, minimum blade passing distance when going

    from positive to negative pitch, fitting the blade root be-

    tween the bolt holes, blade root over-hang, tip clearance

    in a duct while the pitch is actuated through the wholestroke, blade spindle torque at all operation conditions,

    etc. The compromise has given more weight on:

    - propulsive efficiency for low pitch and blade

    area ratios;

    -

    comfort (better cavitation performance) for highpitch and large blade area ratios.

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    The design methodology and philosophy discussed above

    for these C- and D-series propellers can be summarizedin one sentence: these series represent contemporary and

    practical CPP designs.

    The whole series consist of 20 open propellers and 15

    ducted propellers, as listed in Table 2, which were testedfor 604 complete two-quadrant open water characteristicsat various pitch settings and duct combinations (Table 3).

    Table 2 Overview of the C-series and D-series propeller

    models (design pitch ratio P0.7R/D of the propellers are

    listed in the table), in total 35 propeller models.AE/A0 [%] 40 55 60 70 75

    C4series0.8, 1.0,

    1.2, 1.4

    0.8, 1.0,

    1.2, 1.4

    0.8, 1.0,

    1.2, 1.4

    C5series1.0, 1.2,1.4, 1.6

    1.0, 1.2,1.4, 1.6

    D4series0.0, 0.8,

    1.0, 1.2,1.4

    0.0, 0.8,

    1.0, 1.2,1.4

    0.0, 0.8,

    1.0, 1.2,1.4

    Table 3 Overview of the test matrix, in total 604 com-

    plete two-quadrant propeller open water tests.

    tested

    pitch

    settingsP0.7

    R/D Propeller design pitch ratioP0.7R/D

    C4-40

    C4-55C4-70*

    C5-60

    C5-75

    D4-40D4-55

    D4-70

    in No.19A duct

    D4-40D4-55

    D4-70

    in No. 37 duct

    0.8 1.0 1.2 1.4 1.0 1.2 1.4 1.6 0.0 0.8 1.0 1.2 1.4 0.0 0.8 1.0 1.2 1.4

    -1.4

    -1.2 -1.0 -0.7 -0.4 -0.1 0.0 0.1 0.2 0.5 0.8 1.0 1.2 1.4

    1.6

    1.8

    *blade feathering tests, in both positive & negative advance directions.

    3. PROPELLER GEOMETRY

    After the initial design of each propeller of the series, themain parameters of every propeller were fitted with

    polynomials and the propeller models were manufactured

    according to the parametric descriptions. In order toreduce the influence of the blade weight on the

    measurements, all propeller blades and hubs were madeof aluminium with anodized final surface treatment.

    3.1 HUB-PROPELLER DIAMETER RATIO

    The hub-propeller diameter ratio is determined first,

    which varies with the design pitch ratio at 0.7R of the

    propeller, defined as:

    and represents the present best practice on hub design

    with smallest achievable hub size. The ratio isdetermined by the following quadratic polynomial:

    with a hub consisting of a basic spherical form contourconnected to two cylinders on the two sides (Figure 1).

    3.2 BLADE PARAMETRIC DESCRIPTIONS

    The radial distribution of the main parameters of the pro-

    pellers (blade chord length ratio C/D, pitch ratio P/D,

    skew ratio S/D, rake ratio X/D, maximum thickness ratio

    tmax/D and maximum camber ratio fmax/D of the blade

    sections) are all given in polynomials in the form of:

    wheresis the non-dimensional radius defined as:

    and ris the radius. At the blade tip when r=D/2,s=0. At

    the blade root when r=d/2, s=1. The coefficients a

    depend on the design pitch of the propeller p by

    quadratic polynomials defined as:

    By integrating the chord length of the propeller blades

    from the blade root to the tip, as given in Equation (3)

    and (4), the blade area can be easily derived and

    expressed also in parametric formula.

    3.3 BLADE SECTION PROFILES

    The NACA 66 (MOD) thickness distribution and the

    NACA a=0.8 meanline have been used for all of the pro-

    peller blades for the present propeller series. The thick-

    ness distribution is, however, applied perpendicular to

    the nose-tail line of the section profile.

    In order to prevent very thin blade trailing edges in

    model scale, the trailing edges of the propeller model

    blades are thickened to minimal 0.4 mm, starting gradu-

    ally from the maximum thickness of the profile to the

    trailing edges by a parabolic distribution.

    3.4 PITCH DEFINITION

    The design pitch is defined based on the nose-tail line of

    the blade section profile. At off-design condition, the

    pitch setting refers to the pitch of the blade at 0.7R which

    is based on the nose-tail line of the section profile at that

    pitch setting (R is the propeller radius at design pitch).

    3.5 TIP FORM, BLADE ROOT FILLETS AND

    ANTI-SINGING EDGE

    A non-ice-strengthened tip form and composite bladeroot fillets are applied to all of the model propellers. The

    composite blade root fillets consist of two fillet radii, the

    larger one has a radius of 3Tmaxand the small one has a

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    radius of Tmax/3, where Tmaxis the blade maximum thick-

    ness at the blade root. Due to the fact that the propellermodel blades are too thin to make anti-singing edges, no

    anti-singing edges are applied.

    4. TEST SET-UP AND PROCEDURES

    4.1 TEST SET-UP

    The test set-up is the same as used and discussed in Ref-

    erence [23] with a dummy test hub and force transducers

    as shown in Figure 1. The thrust and torque are measured

    on the shaft next to the propeller and the blade spindletorque is measured inside the test hub.

    Figure 1 Test set-up and propeller shaft thrust and torque

    sensors and blade spindle torque sensor.

    4.2 TEST PROCEDURES

    In a conventional propeller open water test from J=0 to

    KT=0, the propeller shaft rotational rate is often kept con-

    stant while the advance speed of the propeller varies.

    During propeller four-quadrant open water tests, likedone for FPPs, both the advance speed and the shaft

    rotational rate have to vary and change directions, be-

    cause only a finite towing speed of the carriage can be

    achieved. However, most controllable pitch propellerswill never rotate reversely. This practice has been also

    used here during the model tests, where only one rota-

    tional direction (positive rotational direction) has been

    tested. Therefore, only two-quadrant (the first and the

    fourth quadrant) open water characteristics have been

    measured.

    At propeller off-design conditions, the propeller hydro-

    dynamic pitch angle is often used, instead of the ad-vance ratio J, to define the operation condition of the

    blades,

    Under this definition, a complete set of two-quadrant

    open water characteristics of a controllable pitch propel-

    ler covers the range -90o +90

    o.

    A quasi-steady open water test is, in principle, an un-

    steady model test by continuously varying the advance

    speed and/or the rotational rate in such a way that the

    steady state performance of the propeller for the com-plete range of conditions can be derived. For the whole

    C- and D-series two-quadrant tests, the following four

    test runs have been used, as listed in Table 4.

    Table 4 Quasi-steady test runs for the complete 2-

    quadrant open water characteristics of a controllable

    pitch propeller.

    run shaft rotational rate advance speed range1 constant +900RPM 0 to +4m/s to 0 0oto ~+30oto 0o

    2 0 to +900RPM to 0 constant +4m/s +90oto ~+30oto +90o

    3 constant +900RPM 0 to4m/s to 0 0oto ~30oto 0o

    4 0 to +900RPM to 0 constant4m/s 90oto ~30oto90o

    This makes it possible to test the complete two-quadrant

    open water characteristics of a propeller in only 4 test

    runs, using 2 runs by varying the towing speed of thecarriage and 2 runs by varying the shaft rotational rate.

    From the first two runs - No. 1 and No. 2, the results in

    the first quadrant for from 0 to +90 degrees can be ob-

    tained. From the last two runs - No. 3 and No. 4, the re-

    sults in the fourth quadrant for from 0 to -90 degreescan be obtained.

    A sinusoidal variation as sketched in Figure 2 has been

    used for the variations of the carriage (advance) speed

    and the propeller rotational rate during the tests.

    Figure 2 Sketch of the sinusoidal variations for towing

    speed and propeller shaft rotational rate.

    For the first quadrant (test runs No. 1 and No. 2), the

    towing carriage is travelling in the normal towing direc-

    tion, which we call the positive direction as shown in

    the sketch in Figure 3.

    Figure 3 Sketch of test set-up for the first quadrant tests.

    For the fourth quadrant (test runs No. 3 and No. 4), the

    same set-up used for the first quadrant test but towed by

    the carriage in the reverse direction, see Figure 4. The

    advantage of this method is that the whole set-up remains

    the same as for the first quadrant, except for the towing

    direction of the carriage. The drawback is that the flowgoes first over the open water test POD housing and strut

    before it reaches the propeller. The influence of the wake

    from the strut was found to be very limited and has beencarefully corrected for.

    +Va

    +n

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    Figure 4 Sketch of test set-up for the fourth quadrant

    tests.

    More details of the quasi-steady propeller open water test

    procedures are given by Danget al[23].

    5. PRESENTATION OF RESULTS

    The measured propeller shaft thrust and torque, and the

    blade spindle torque, are non-dimensionalized by the

    relative velocity to the blade at 0.7R radius defined as,

    with the propeller thrust coefficient defined as,

    the propeller torque coefficient defined as,

    and the blade spindle torque coefficient defined as,

    where, the positive directions of the propeller shaft

    thrust, torque and the blade spindle torque are shown in

    Figure 5. The positive blade spindle torque is defined as

    the direction that tends to drive the propeller to a largerpitch.

    Figure 5 Definition of positive directions for the thrust,

    torque and the blade spindle torque.

    All coefficients provided above are hydrodynamic coef-

    ficients. The spindle torque induced by the centrifugal

    force of the model blade has been subtracted.

    Each set of data - the propeller thrust coefficients, the

    propeller torque coefficients and the blade spindle torque

    coefficients - was fitted with one of the following Fourier

    series respectively. The Fourier series coefficients were

    determined up to the order of 40, truncated from the 31stharmonic gradually (linearly) until completely at the 40thharmonic.

    (11)

    6. C4-40 SERIES

    As an example case, the test results of the C4-40 seriesare presented in this section.

    The C4-40 series propeller model are shown in Figure 6

    with MARINs propeller numbers and their design pitch

    noted in the figure. The propeller diameters vary between

    230.37mm to 242.81mm with hub diameter of 58.0mm.

    Model No. 7189 (P0.7R/D = 0.8) Model No. 7190 (P0.7R/D = 1.0)

    Model No. 7191 (P0.7R/D = 1.2) Model No. 7192 (P0.7R/D = 1.4)Figure 6 C4-40 series propeller models with aluminium

    blades on the dummy hubs at design pitch settings.

    During the test runs, the blade Reynolds number varieswith the variation of the propeller advance speed and the

    shaft rotational rate, which depends on the chord length

    of the propeller blades. Table 5 provides the range of the

    Reynolds numbers based on 0.7R chord length and local

    inflow velocity during the tests for the C4-40 series,

    where the Reynolds number is defined as,

    The open water characteristics of these series propellers

    in the first quadrant are plotted in Figure 7 inKT, 10KQ, ~Jdiagram. Their two-quadrant open water characteris-

    tics are plotted into diagrams on Figure 9 through Figure

    +n

    -Va

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    20. These values are all in model scale without any cor-

    rections for the Reynolds numbers, which varies duringthe quasi-steady open water tests.

    Table 5 Blade chord Reynolds numbers during test runs.Blade chord Reynolds numberRe 10-5

    Runs Propeller Nos.7189R 7190R 7191R 7192R

    Run No. 1, 3min. 4.4003 4.2608 4.1291 4.0043

    max. 4.9185 4.7799 4.6490 4.5252

    Run No. 2, 4min. 2.1975 2.1663 2.1364 2.1078

    max. 5.0062 4.8645 4.7307 4.6041

    Figure 7 Open water characteristics of C4-40 series.

    To make an assessment on the C4-40 series propeller

    blade designs, a comparison has been made for the open

    water efficiency to the propeller ideal efficiency, together

    with the B-series for the same blade area ratio and the

    same pitch ratio. The comparison is based on the propel-

    ler thrust loading coefficient CT, as shown in Figure 8.

    It should be noted that the present series were carried out

    at a shaft rotational rate of 900 RPM with a chord Rey-

    nolds number Re at 0.7R radius between 0.4106 and

    0.5106 (Table 5) for C4-40 series, while the B-series

    were tested at much lower shaft rotational rate and the

    results were later corrected to a standard chord Reynolds

    number of 2.00106on 0.75R chord [5]. A direct, quanti-

    tative and fair comparison of these two series is therefore

    difficult.

    However, for a qualitative assessment on C4-40 series,

    Figure 8 can be used. The offsets between the ideal effi-ciency and the measured open water efficiency is often

    used to evaluate a propeller design, which contains all

    losses of a real propeller (such as the rotational losses,

    friction losses, non-uniform losses due to finite numberof blades, vortex losses, etc.). An offset of the efficiency

    of about 0.15 has been found for the C4-40 series, which

    is regarded as excellent designs. The same results are

    also found for the other C-Series Propellers.

    Figure 8 Comparison of open water efficiency with the

    ideal efficiency.

    7. CONCLUSIONS AND FUTURE WORK

    Two new propeller series The Wageningen C- and D-Series Propellers have been developed within a Joined

    Industry Project (JIP), with both industry and govern-

    ment funding. The series represent the most contempo-rary controllable pitch propeller design practice, both for

    open and ducted propellers, with balanced compromise

    between efficiency and comfort, while also observing

    practical and mechanical constraints. Compared to the

    ideal efficiency, the C-series propellers show good effi-

    ciency values.

    The complete two-quadrant open water characteristics of

    those propellers at all practically-used pitch settings have

    been tested, which provide a huge database with com-plete information on the off-design performance of con-

    trollable pitch propellers. They are the first and the onlyseries with blade spindle torque information for a com-

    plete range of operational conditions and pitch settings.

    All results are shared with the participating organisations

    in this JIP. Furthermore, the data will be implemented insoftware for practical use by all participants.

    In addition, it has been also planned to test the C4-70 and

    C5-75 series for blade spindle torque in cavitating condi-

    tions, the C4-70 and C5-75 series for cavitation inception

    characteristics at one pitch ratio, and the D4-70 series inNo. 37 duct for thrust breakdown due to excessive cavi-

    tation in bollard pull and free running conditions.

    0.0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1.0

    1.1

    1.2

    0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6

    THRUSTCOEFFICIENT

    KT,TORQUE

    COEFFICIENT

    10KQ,EFFICIENCY

    ADVANCE COEFFICIENT J

    P0.7R/D=0.8

    P0.7R/D=1.4

    P0.7R/D=1.0

    P0.7R/D=1.2

    0.30

    0.35

    0.40

    0.45

    0.50

    0.55

    0.60

    0.65

    0.70

    0.75

    0.80

    0.85

    0.90

    0.95

    1.00

    0.0 1.0 2.0 3.0 4.0 5.0

    PROPELLEROPENWATEREFFICIENCY

    PROPELLER THRUST LOADING COEFFICIENT C T=8/p KT/J2

    Ideal Efficiency

    B4-40 P/D=0.8

    B4-40 P/D=1.0

    B4-40 P/D=1.2

    B4-40 P/D=1.4

    C4-40 P/D=0.8

    C4-40 P/D=1.0

    C4-40 P/D=1.2

    C4-40 P/D=1.4

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    Figure 9 Thrust coefficient CT at various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=0.8.

    Figure 10 Thrust coefficient CTat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.0.

    Figure 11 Thrust coefficient CT at various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.2.

    Figure 12 Thrust coefficient CTat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.4.

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER THRUST COEFFICIENT CT

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER THRUST COEFFICIENT CT

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER THRUST COEFFICIENT CT

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER THRUST COEFFICIENT CT

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    P/D = 1.6

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    Figure 13 Torque coefficient CQat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=0.8.

    Figure 14 Torque coefficient CQat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.0.

    Figure 15 Torque coefficient CQat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.2.

    Figure 16 Torque coefficient CQat various pitch settings

    for propeller C4-40 with design pitch ratioP0.7R/D=1.4.

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    1.2

    1.4

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER TORQUE COEFFICIENT 10CQ

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    1.2

    1.4

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER TORQUE COEFFICIENT 10CQ

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    1.2

    1.4

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER TORQUE COEFFICIENT 10CQ

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    1.2

    1.4

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER TORQUE COEFFICIENT 10CQ

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    P/D = 1.6

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    Figure 17 Blade spindle torque coefficient CQbladeat vari-

    ous pitch settings for propeller C4-40 with design pitch

    ratioP0.7R/D=0.8.

    Figure 18 Blade spindle torque coefficient CQbladeat vari-

    ous pitch settings for propeller C4-40 with design pitchratioP0.7R/D=1.0.

    Figure 19 Blade spindle torque coefficient CQbladeat vari-

    ous pitch settings for propeller C4-40 with design pitch

    ratioP0.7R/D=1.2.

    Figure 20 Blade spindle torque coefficient CQbladeat vari-

    ous pitch settings for propeller C4-40 with design pitchratioP0.7R/D=1.4.

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -1.0

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER BLADE SPINDLE TORQUE COEFFICIENT 100CQblade

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -1.0

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER BLADE SPINDLE TORQUE COEFFICIENT 100CQblade

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -1.0

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYNAMICPITCHANGLE[degrees]

    PROPELLER BLADE SPINDLE TORQUE COEFFICIENT 100CQblade

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    -90

    -75

    -60

    -45

    -30

    -15

    0

    15

    30

    45

    60

    75

    90

    -1.0

    -0.8

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0.8

    HYDRODYN

    AMICPITCHANGLE[degrees]

    PROPELLER BLADE SPINDLE TORQUE COEFFICIENT 100CQblade

    P/D = -1.2

    P/D = -1.0

    P/D = -0.7

    P/D = -0.4

    P/D = -0.1

    P/D = 0.0

    P/D = 0.1

    P/D = 0.2

    P/D = 0.5

    P/D = 0.8

    P/D = 1.0

    P/D = 1.2

    P/D = 1.4

    P/D = 1.6

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    8. ACKNOWLEDGEMENTS

    The authors thank all participants in The Wageningen C-

    and D-Series Propellers JIP: Advance Gearbox, Andritz

    (Escher Wyss), Bluewater, Bruntons Propellers (Stone

    Marine), Brunvoll, Caterpillar (Berg Propulsion),

    CSDDC, CSSRC, Damen, DNV, DSME, GL-Group (Fu-tureShip), Hundested, Hyundai, Kamome, Kawasaki,

    MAN, MARIN, Nakashima, NGC, Niigata, Rolls-Royce,

    Royal Netherlands Navy, Scana Volda, SMERI, SMMC,

    TU Delft, Wrtsil and ZF Marine. In addition, this JIP is

    also supported by UDP-JIP, SPA-JIP and STA-JIP.

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