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    Simulation for The Propeller Loading of Marine Electrical Propulsion Based on

    Matlab jiang pan

    School of Energy and PowerEngineering

    Wuhan University ofTechnology

    Wuhan, [email protected]

    Yao Yunan

    School of Energy and PowerEngineering

    Wuhan University ofTechnology

    Wuhan, [email protected]

    Fan Shidong

    School of Energy and PowerEngineering

    Wuhan University ofTechnology

    Wuhan, [email protected]

    Abstract With the requirement of energy-saving,

    environmental protection, control performance

    and military strategy.The improvement of ship

    electric propulsion technology has become an

    important direction for future development of

    ship.First according to the Chebyshev Polynomial

    to fitting Four-quadrant propeller characteristic

    chart,then establish the mathematical model of

    paddle.Last use matlab to create the simulation

    model,then run the model to simulate the real and

    dynamic working course in the no wind and head

    wind environment.

    Keywords -marine; electric; propulsion; simulation

    I. INTRODUCTION

    The accurate analysis of the propeller load

    characteristics is one of the most important part

    for the simulation of the electric propulsion. At

    design stage for the electric propulsion system, tomeet the indicator, simulate the propulsion

    system in all working condition. The existed

    simulation models omitted the influence of air

    resistance on the ship, and the simulation is run

    in an ideal conditions. On this basis, this article

    considering the air resistance and simulate the

    propeller loading in no wind and head wind

    situation. Therefore, the paragraph below will

    introduce the propeller load characteristics for

    complex conditions for further simulation.

    II. FOUR QUADRANT PROPELLER EXPRESSION

    The propeller thrust coefficient p K torque

    coefficien M K and ratio of velocity to

    revolution J are defined as follow [1]:24/ N D P K p = (1)

    25/ N D M K M = (2)

    DN V J p /= (3)

    In the expression: pV is the velocity of

    propeller; P and are thrust and torquegenerate from propeller; D is the diameter of

    propeller; is seawater density.

    According to different speeds and velocity,the propeller working conditions can be divided

    into four quadrants. And the

    coefficient p K , M K , and J are infinity. It is

    called non-bounded expression. In the dynamic

    expression of the propeller in full working

    condition, it is usually more convenient to take

    the form of bounded expression. When N and

    pV are not equal to zero at the same time, the

    978-1-4244-8039-5/11/$26.00 2011 IEEE

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    corresponding definition is [2]:

    )](/[' 2222 N DV D p K p p += (4)

    )](/[' 2223 N DV Dm K pm += (5)

    2/1222 )/(' N DV V J p p += (6)

    From the expression (6) it could deduce:

    2/1222 )/(1(/' N DV N DV J p p += (7)

    Then from the two expressions above it could

    deduce the relation between J and ' J :

    )1/(' 2 J J J += (N>0) (7a)

    )1/(' 2 J J J += (N

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    III . PROPELLER MATH MODEL

    Propeller torque:

    23

    2223

    '/'

    )('

    J V D K

    D N V D K M

    pm

    pm

    =+= (10)

    Propeller thrust:

    22

    2222

    '/'

    )('

    J V D K

    D N V D K P

    p p

    p p

    =+= (11)

    Due to thrust deduction coefficient:

    P P P

    t e

    =,

    the ffective thrust generated by propeller is :

    22 '/')1()1( J V D K t P t P p pe

    == (12)

    In the expression :e P is the effective thrust ,

    t is the thrust deduction coefficient .

    )1( = s p V V (13)

    In the expression: pV is the velocity of

    propeller, sV is the velocity of ship, is

    mixed flow coefficient.

    The motion equation for the propeller system

    is established:

    R P dt dvmm e =+ /)( (14)

    In the expression: m is the quality of ship ;m is the quality of water attached on the hull ;

    R is the toal resistance of ship.The total resistance of the ship include:

    hydrodynamic resistance 1 R and air

    resistance 2 R . Firstly the drag power of a ship in

    working state is calculated [3]:

    LC k DV

    N a s R+

    =)1(3

    (15)

    L B 10= (16)

    1003.07.0

    L+= (17)

    In the expression: L is length of ship; D isvessel displacement;

    is correction factor;

    a K is accessories influence coefficient; is

    coefficients of form ; B is breadth of ship ; is ship square coefficient.

    Hydrodynamic resistance calculating

    formula:

    s R V N R /751 = (18)

    Air resistance calculating formula:

    22 sb FV K R = (19)

    Among them the coefficient C and b K in

    the (15) and (19) are determined by the

    reference[3].

    In the simulation model, parameters t and are determined as follow [4]:

    =

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    readable. The simulation model and its sub-block

    are as follows [5] :

    The simulation model is built based on

    mathematical model In the matlab / simulink

    environment. In simulink tool box there are many

    packaged blocks, which can be copied to model

    window and then be connected together. As this

    model is complex. here choose a subsystem,

    making the model simple and easy to read. The

    simulation model and subsystem model are as

    follows:

    simulation model of the propeller

    Subsystem model

    DYNAMIC LOAD CHARACTERISTICS OF THE

    PROPELLER According to the parameters of electric

    propulsion ship, it applies the simulation model.

    The results are:

    (5)Velocity of ship

    (6) torque

    (7)Velocity of ship

    (8) torque

    CONCLUSION Sea breeze has great influence on a sailing

    ship, especially on maneuverability and the

    loading characteristic. Analysis of above result

    draws the following conclusions:

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