Numerical Predictions of the Propeller Cavitation behind Ship and Comparison with Experiment

,

(a.National Key Laboratory on Ship Vibration&Noise;b.Jiangsu Key Laboratory of Green Ship Technology, China Ship Scientific Research Center,Wuxi 214082,China)

Numerical Predictions of the Propeller Cavitation behind Ship and Comparison with Experiment

LIU Deng-chenga,b,ZHOU Wei-xina,b

(a.National Key Laboratory on Ship Vibration&Noise;b.Jiangsu Key Laboratory of Green Ship Technology, China Ship Scientific Research Center,Wuxi 214082,China)

The effects of turbulence model on propeller cavitation simulation results are presented.It shows that the common turbulence model can deal well with the propeller cavitaion shapes.And then the propeller cavitation performance behind ship was numerically simulated using a hextetrahedral mesh based on RANS solver,the Suaer’s cavitation model based on transport equation and a SSTk-ω turbulence model were coupled in the RANS solver.A symmetry boundary condition is applied on the top of computational domain instead of the free surface,which is similar to a tunnel’s wall. To observe the cavitation pattern during the revolution of propeller,the propeller is rotated with a constant rotation angle of 1.0 degree using a sliding mesh technique.Cavitation patterns of the simulations are compared with the experimental results carried out in Large Cavitation Channel of CSSRC (LCC).Although the predicted propeller tip vortex cavity is missing because of the mesh resolution,the predicted dynamic cavitation behaviors generally well agree with experimental observation.

cavitation;propeller;ship;numerical prediction

0 Introduction

The propeller cavitation can rise up the vibration,the noise and the erosion.Therefore, the predicted propeller dynamic cavitation behavior is of great interest for propeller designer.

Cavitation presents complex unsteady,turbulent and multi-phase flow phenomena with a large density difference and mass transfer.These features result in a unique challenge for the simulation of cavitating flows.

The simulations of cavitating flow using viscous CFD method were performed actively in the last decade because cavitation models and computation power have been rapidly developed.Many researchers did some simulations of foil and propeller cavitating flow.For example,Rhee and Kawamura[1]studied the cavitating flow around a marine propeller using an unstructured mesh.Liu[2-4]simulated the cavitation performance of marine propeller using a hybrid mesh based on RANS solver using singhal model.Coutier-Delgosha et al[5]computedcavitating flows around 2D foil by modifying turbulence model,and the sheet cavity length and the dynamic shedding behaviour were very similar to those observed in the experiment.Li[6-7]predicted unsteady cavitating flows of 2D NACA0015 foil and 3D twisted foil using the same idea.Shin et al[8]carried out cavitation simulation on conventional and high-skewed propellers in the Behind-Hull Condition.Paik et al[9]simulated the cavitation and hull pressure fluctuation for propeller with hull interaction,and so on.

In this paper,the effects of turbulence model on propeller cavitation simulation results are researched.And then the propeller cavitation performance behind ship was numerically simulated using a hextetrahedral mesh based on RANS solver,the Suaer’s cavitation model based on transport equation and a SST k-ω turbulence model were coupled in the RANS solver.

1 Numerical method

1.1 Governing equations

For the multi-phase flow solutions,the single-fluid mixture model is employed.The governing equations are written for the mass and momentum conservation of mixed fluid as follows:

where ρmis the mixed density,μ is the mixed viscosity,μtis the mixed eddy viscosity which is calculated by turbulence model.

Convection terms are discretized using a second order accurate upwind scheme,while diffusion terms are discretized using a second order accurate central differencing scheme.A segregated solver with SIMPLE as the velocity-pressure coupling algorithm was selected.The discrete equations are solved using Gauss-Seidel iterations,and algebraic multi-grid method accelerates the solution convergence.The effect of gravity is neglected.The double model is used for dealing with free-surface.

1.2 Sauer cavitation model

The mixed density is controlled by vapor fraction α:

The vapor transport equation is written as:

where ρvand ρlare the density of vapor and liquid,respectively.andare the rates of vapor generation and condensation,respectively.Sauer derived the expressions ofand

where ρvis saturated vapor pressure.

2 The effect of turbulence model

For research the effect of different turbulence model,three different turbulence models are employed to research the effect of different turbulence model which include k-ε,SST k-ω and Reynolds stress turbulence model(RSM).The PPTC propeller cavitation in uniform flow is carried out.PPTC propeller is an international standard model which is proposed on the first workshop on cavitation and propeller performance.There are abundant experimental data.

Tab.1 presents the case of computational.The expressions of advance ratio and cavitation number are written as follows:

Tab.1 The case2-1 of cavitation computational

For tip vortex region grid refinement,a block was created according to the helix line,and the pitch is equal to the propeller pitch at the 1.0 time radius(see Fig.1).The textetrahedral mesh is used(see Fig.2).

Fig.1 The block for tip vortex region grid refinement

Fig.2 The grid types

Fig.3 The computational cavity shapes and compared with experimental

Fig.3 presents the comparison of the computed cavity shapes with the experimental results which come from Potsdam Model Basin at the first workshop on cavitation and propeller performance.The computed cavity shapes can be confirmed by the iso-surface of vapor volume fraction of 0.1.From the experimental results we clearly see that the cavitation is to occur in the tip,root and leading edge of suction side of propeller.Fig.4 shows that the all computational cases catch the cavity in the tip,root and leading edge,but the sheet cavitation at leading edge is a little unpredicted.The computational results indicated that the common turbulence model can deal well with cavitating flow,and the SST k-ω turbulence model is chosen for simulating the propeller cavitation behind ship because this turbulence model is often imposed in propeller performance simulation.

3 Propeller cavitations behind ship

3.1 Geometry and computational domain

An 82000DWT bulk carrier with five blades propeller was chosen for the cavitation simulation which has experimental data of cavitation observation come from LCC of CSSRC.Propeller model is a five bladed propeller with diameter D=0.237 m and area ratio of 0.52.

The computational domain was created:The inlet of the domain is at 1.5L upstream of the ship hull;exit at 2.5L downstream;outer boundary at 1.5L from the center of symmetrical plane; L is the length of ship.

3.2 Computation mesh and conditions

The entire domain is filled with hextetrahedral mesh.The minimum size of grid is 1.8 mm in the ship stern region and 0.5 mm in the propeller tip region(see Fig.4),there are only about 2～4 grids in the propeller tip vortex region because of the size of propeller model tip vortex cavitation is about 1～2 mm,so the propeller tip vortex cavitation will be missing.The grid cells number was about 3.2 million in static region and 0.8 million in rotating region.

Boundary conditions were set to simulate the flow around ship with propeller:on the inlet boundary and the outer boundary,velocity components of uniform stream with the given inflow speeds were imposed;on wall surface,the no slip condition was imposed;and on thesymmetrical plane boundaries of free-surface,symmetry was ensured;on the exit boundary, the static pressure was set to a constant value according to the cavitation index.The unsteady wetted computation results are used as the initial value of unsteady cavitation simulation.The propeller is rotated with a constant rotation angle of 1.0°using a sliding mesh technique.The conditions are described in Tab.2.The expression of cavitation index is written as follows:

Fig.4 The mesh of ship stern surface

Tab.2 The computational conditions

3.2 Results and comparison with experiment

The simulations of propeller cavitating flow with ship are calculated at two conditions. The computed results of thrust coefficient are summarized in Tab.3.The results of model test are also presented at wetted condition.For the wetted simulation,the comparison shows quite good agreement,and the thrust coefficients are over predicted 4.34%and 1.73%at design and ballast condition,respectively.The simulated results show that the thrust coefficient will be slightly increased less than 1%when propeller comes into cavitation at design and ballast condition.

Cavitation patterns at some propeller blade angle at the design and ballast draught conditions are compared with the experimental results in Figs.5 and 6,respectively.The iso-surface of vapor volume fraction at value 0.1 shows the interface of cavity.The tip vortex cavitation in simulation results is missing which is consistent with expected,but the cavity patterns generally well agree with the experiments.At the design and ballast draught condition,the leading edge cavitation from 0.7R to 0.95R of the propeller blade at propeller blade angle of 350° is appeared in the numerical simulation,while the patch cavitation is observed in model test.

Tab.3 The thrust coefficient at two conditions

Fig.5 The comparison of cavitation patterns at design draught condition

Fig.6 The comparison of cavitation patterns at ballast draught condition

Fig.7 and Fig.8 show the cavitation photos at design and ballast draught condition.At the two draught conditions,the cavitation presents unstable behavior at some propeller blade angle of 20°and 30°,especially at the ballast draught condition,but the simulation results are stable at all blade angles.The simulations results can present the cavitation dynamic behavior withblade angles,not present the cavitation dynamic behavior with time at the same blade angle.

Fig.7 Cavtation photos at design draught condition

Fig.8 Cavtation photos at ballast draught condition

4 Conclusions

Firstly,the effects of turbulence model on propeller cavitation simulation results are pre-sented.It shows that the common turbulence model can deal well with the propeller cavitaion shapes.And then the propeller cavitation performance behind ship was numerically simulated using a hextetrahedral mesh based on RANS solver,the Suaer’s cavitation model based on transport equation and a SST k-ω turbulence model were coupled in the RANS solver.And the simulation results were compared with the experimental results performed in the large cavitation channel.

The simulated results show that the thrust coefficient will be slightly increased less than 1%when propeller comes into cavitation at design and ballast condition.The cavitation patterns of simulations results can present the cavitation dynamic behavior with blade angles,not present the cavitation dynamic behavior with time at the same blade angle.Although the predicted propeller tip vortex cavity is missing because of the mesh resolution,the predicted dynamic cavitation behaviors generally well agree with experimental observation.We believe that numerical assessment cavitation pressure fluctuation is tangible in the near future.

For the further work,simulations of hull pressure fluctuation for a marine propeller operating behind a hull will be simulated.

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[3]Liu Dengcheng,Hong Fangwen.The Numerical Predicted of SMP11 propeller performance with and without cavitation[C]// Second International Symposium on Marine Propulsors,SMP’11,June,2011.Hamburg,Germany,2011.

[4]Liu Dengcheng.The numerical predicted of VP1304 propeller cavitation performance in oblique flow[C]//Fourth International Symposium on Marine Propulsors.smp’15,May 31-June 4,2015.Workshop:Propeller performance.Austin,USA, 2015.

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船后螺旋槳空泡數(shù)值預報及試驗對比

劉登成a，b，周偉新a，b

（中國船舶科學研究中心 a.船舶振動噪聲重點實驗室；b.江蘇省綠色船舶技術(shù)重點實驗室，江蘇 無錫 21408）

文章研究了湍流模型對螺旋槳空泡計算結(jié)果的影響，結(jié)果表明常用的湍流模型均可較好地預報螺旋槳空泡形態(tài)。采用RANS求解器，結(jié)合SST k-ω湍流模型和Sauer空化模型，數(shù)值模擬了船后螺旋槳空泡。用對稱面邊界條件處理自由表面，滑移網(wǎng)格技術(shù)處理螺旋槳旋轉(zhuǎn)，時間步長為1°。螺旋槳空泡模擬結(jié)果與大型循環(huán)水槽試驗結(jié)果進行了對比，雖然由于計算網(wǎng)格稀疏的原因沒能捕捉到螺旋槳梢渦空泡，但螺旋槳空泡隨空間角度的動態(tài)行為與試驗觀察結(jié)果吻合較好。

空泡；螺旋槳；船體；數(shù)值預報

U661.73

:A

劉登成（1982-），男，中國船舶科學研究中心高級工程師；

U661.73

:A

10.3969/j.issn.1007-7294.2016.03.001

1007-7294（2016）03-0233-10

周偉新（1970-），男，中國船舶科學研究中心研究員。

Received date：2015-12-03

Foundation item:Supported by the National Natural Science Foundation of China(Grant No.11332009)

Biography：Liu Deng-cheng(1982-),male,senior engineer,E-mail:edon_001@163.com;

ZHOU Wei-xin(1970-),male,researcher.