# Investigation of Boundary Effects on the Natural Cavitating Flow around a 2D Wedge in Shallow Water

Authors: Xin Chen; Ying Chen; Jia-Yi Cao; Jie Li
Journal: Modelling and Simulation in Engineering
 (2011)

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## Abstract

When a cavitated body moves in shallow water, both flexible free surface and rigid bottom wall will produce great influence on the cavity pattern and hydrodynamics to change the motion attitude and stability of the body. In this paper, a single-fluid multiphase flow method coupled with a natural cavitation model was employed to study the effects of two kinds of boundaries on the natural cavitating flow around a two-dimensional symmetry wedge in shallow water. Within the range of the cavitation number for computation (0.05 ~ 2.04), the cavity pattern would be divided into three types, namely, stable type, transition type and wake-vortex type. The shape of the free surface is fairly similar to that of the cavity's upper surface with well right-and-left symmetry. However, when the immersion depth and the cavitation number are decreasing, the symmetry of the cavity shape is destroyed due to the influence of bottom wall effects. When the cavitation number is less than about 0.1, with the immersion depth going down, free surface effects exerts a stronger influence on the drag coefficient of this 2D wedge, whereas wall effects bring a stronger influence on the lift coefficient.


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## Body

## 1. Introduction

Recently, high-speed underwater vehicles such as hydrofoil-assisted crafts, fast ferries gain much interest in marine transport industry. When fast vehicles covered with supercavity navigate in shallow water like littoral zones, both the flexible free surface and the rigid water bottom will produce significant influence on the cavity pattern and the hydrodynamics of the vehicle. In such case, the so-called “boundary effects” will make the flow blocked and affect the motion attitude and stability of the vehicle.Concerning the boundary effect problems caused by solid wall, many researches have been conducted so far in the world through the approaches of theoretical analysis, numerical simulation, and experimental investigation. Birkhoff et al. [1] theoretically studied the blocked cavitating flow around no-lift wedge and found that the defined drag coefficient in conventional experiments was very sensitive to the distance between the tunnel wall and the test model. Brennen [2] employed the Riabouchinsky closure model to examine the boundary effect on the axisymmetric cavity with limited length over a disk or sphere in water tunnel of circular cross-section. He obtained an analytic solution which indicates that the flow could be blocked under some particular condition. This expanded the insight about boundary effects into the area of axisymmetric cavitating flows. Chen et al. [3] utilized the multiphase model based on Reynolds averaged Navier-Stokes equation system to numerically analyze the boundary effect on ventilated cavitating flows around a given submerged vehicle with a disk cavitator in closed water tunnel.In addition, some other researches about the free surface effect on cavitating flows also have been done. Within the framework of the linearized theory, Franc and Michel [4] calculated the slope of the lift coefficient versus the angle of attack for cavitating hydrofoil with infinite cavities (cavitation number equals to 0) under a free surface and different immersion depths. For small or infinite value of the immersion depth, the slope tends towards the limited value.However, the boundary effect on cavitating flows when a rigid wall and a free surface coexist has not been widely investigated yet so far. Bal and Kinnas et al. [5] extended the capability of the boundary element method [6–8] to computate cavitating flows around a hydrofoil in numerical wave tank, with the wall effect and free surface effect simultaneously taken into account. Amromin [9] employed a corrected Riabouchinsky closure model on the basis of ideal fluid theory to numerically analyze the shallow-water effect on supercavitating flow. The computational results indicated that for the same cavity length was reached, the cavitation number under the combination of a solid wall and a free surface is greater than that of axisymmetric flows, and the cross-section of cavity had some three-dimensional deformation.Previous researches regarding boundary effects on cavitating flows were mostly limited in the area of potential flow theory, which has difficulty in describing the subtle structure inside the cavity and near the wake. Furthermore, viscous effects are impossible to be considered in the framework of potential flow. Thus, in the present work, numerical methods based on the viscous multiphase flow model [10–12] have been used to study boundary effects of the cavitating flow around two-dimensional wedge in shallow water.


## 2. Governing Equations and Numerical Method

In the present work, a single-fluid multiphase flow model based on the isotropic hypothesis for fluid and the Reynolds averaged Navier-Stokes equation will be employed. The mixture composed of air, vapor, and liquid is regarded as a kind of single fluid with variable density. Each component phase shares the same physical fields, namely, pressure, velocity, and so on. The gravity effect of liquid was considered, and the compressibility of gas was neglected. The volume fractions of air, vapor, and liquid phases, denoted asαa, αv, and αl, respectively, are introduced to obtain a set of governing equations describing the multiphase flow of air, vapor, and liquid phases.The continuity equation for the mixture is as follows:(1)∂ρm∂t+∂∂xi(ρmui)=0.The momentum theorem for the mixture holds as(2)∂∂t(ρmuj)+∂∂xi(ρmuiuj)=-∂p∂xj+ρmgi+∂∂xi[(μm+μt)(∂ui∂xj+∂uj∂xi)].The air phase should keep continuous as(3)∂∂t(ρaαa)+∂∂xi(ρaαaui)=0.The vapor phase should also satisfy continuity during phase-transition process:(4)∂∂t(ρvαv)+∂∂xi(ρvαvui)=ṁ--ṁ+,
where ρ refers to the density t is the flow time ui     denotes each velocity component p is the local pressure the subscripts m, a, v, and l, respectively, refer to the mixture, air, vapor and liquid phases i and j indicate the Cartesian coordinates which can be 1, 2, or 3.The volume fraction equation will not be solved for the primary phase, namely, the liquid phase. The volume fraction equation of liquid phase will be computed based on the following constraint:(5)αa+αv+αl=1.Additionally, two individual transport equations were employed to describe the mass-transfer process [13] as (4) between the vapor phase and the liquid phase:(6)p<pv,ṁ-=ρlρvρmαv(1-αv)3RB[23pv-pρl]1/2,p>pv,ṁ+=ρlρvρmαv(1-αv)3RB[23p-pvρl]1/2,
where  RB=((αv/(1-αv))(3/4πn))1/3is the radius of vapor bubble, n denotes the number of bubble nuclei per volume of liquid, and a value of 1012/m3 would be sufficient for modeling the phase transition.The volume-fraction-averaged density and viscosity of the mixture take on the following forms:(7)ρm=αaρa+αvρv+αlρl,μm=αaμa+αvμv+αlμl.Moreover, the Reliablek-ε  turbulence model [14] together with the wall function [15] was used to calculate the turbulence viscosity, μt, and make the governing equations closed.The finite volume method was utilized to discretize the integral governing equation set, and the high-resolution-interface-capturing high-order convection scheme [16] was employed to capture the free surface. In the equations, the temporal term was discretized with a first-order implicit scheme and second-order upwind scheme was employed for both the pressure term and the convection term. The convection term in turbulence model equation was approximated with first-order upwind scheme especially. The SIMPLE algorithm [17] was adopted to use a relationship between velocity and pressure corrections to enforce mass conservation and to obtain the pressure field. The ultimately linearized algebra equation system was solved with the Gauss-Seidel iteration method [18] and algebraic multigrid method. In computation, a time step of 10−4 s was specified to divide the totally physical time of 0.15~0.2 s. The maximum of inner iterations in each time step was set to be 50.


## 3. Computational Domain and Boundary Conditions

The 2D computational domain and boundary conditions are illustrated in Figure1, where the length and the bottom width of the symmetric wedge are c=60 mm and D=17 mm (R=0.5D). The origin of the coordinate system is located at the tip of the wedge. The positive directions of x and y axes point rightward and upward, respectively. The inlet boundary and the outlet boundary are 60c and 300c away from the origin. The wedge has an immersion depth of h=70, 140, 210 mm, respectively. The rest free surface is of H=280 mm high from the water bottom. The top boundary of the computational domain is 1.75H away from the bottom. The domain was divided into multiblock structured mesh that has 100800 cells.Figure 1
Computational domain and boundary specification.The physical boundaries are assigned with suitable conditions. The inlet boundary and the top boundary were disposed with constant velocity (u1=0m/s for y>h, or else u1=10 m/s; u2=0 m/s). The outlet boundary was specified with fixed static pressure (poutlet=P0 for y>h, or else poutlet=ρ0-ρlgy), which is used to adjust the cavitation number. The surface of the wedge and the bottom boundary were given no-slip conditions.


## 4. Results and Discussion

In this section, influence of boundary effects on several aspects including cavity patterns, free surface’s shapes, and hydrodynamics of the wedge was discussed as follows.


### 4.1. Cavity Pattern

Figure2 presents the typical cavity patterns with a free surface at some specific values of cavitation number, which is defined as σv=(P∞-pv)/0.5ρlV∞2. The cavity outline is defined as the interface where the isosurface of αv=0.5 locates. Here, pv indicates the saturated vapor pressure of water at specific temperature and the P∞ and V∞ denote the upstream pressure and velocity at inlet boundary on y=0.Three cavity patterns: (a) steady type; (b) transition type; (c) wake-vortex type; the upper is the contour of the volume fraction of water; the lower is the contour of the magnitude of the vorticity.
(a)(b)(c)It seems obvious that the size of the cavity becomes smaller if the cavitation number increases. According to contours of the volume fraction of water and the magnitude of the vorticity, cavity patterns can be roughly divided into the three types as follows.(a)Steady Type: the cavitation number σv is approximately in the range of 0.05~0.3. The cavity presents the state of supercavity which is almost full of vapor. The cavity retains a stable shape except for some tiny oscillations near the tail of the cavity. The magnitude of the vorticity is much higher near the cavity surface, at the tailing part of the cavity, and behind the wedge.(b)Transition Type: the cavitation number σv is approximately in the range of 0.3~0.5. The cavity presents the state of cloudy mixture composed of vapor and liquid, which is produced by the strong reentrant jet generated from the tail of the cavity. The cavity can roughly keep relatively clear outline. The magnitude of the vorticity is much higher in the band-shaped zones originated from the ends of the wedge’s base.(c)Wake-Vortex Type: the cavitation number σv is approximately in the range of 0.5~2.04. The cavity presents the state of vortex cavitation, which occurs in shedding vortices of the wake flow and exhibits an evident periodicity.For the steady type of the cavity pattern, three relationships of cavity lengthLc      with the cavitation number σv is shown in Figure 3 where scattered symbols represent the numerical values and solid curves [4] were fitted from experimental data. Good agreement can be observed from the case of h/H=0.25, whereas the relative errors between the numerical and the experimental results get obvious for the other immersion depths. This fact could be due to the reason that the fitted curves of the experiments were obtained from the working condition of about σv>0.1 in the cases of h/H>0.25. These curves could not completely describe the present computational results in the range of σv<0.1 at the immersion depth of h/H>0.25.Figure 3
Relations betweenLc and σv.For a fixed cavitation number, the cavity length is increasing when the immersion depth goes upward. The boundary effect of the solid wall is much stronger than that of the free surface, which enables the flow blocked to make the local cavitation number decrease and the cavity size enlarge.


### 4.2. Shapes of Free Surface and Cavity Interface

Because shapes of the transition type and the wake-vortex type of cavity are too unstable to be analyzed quantitatively, only the steady type of cavity was selected to be discussed in this section.The height differenceshfs between the free surfaces at the conditions of deformation and of stillness are normalized as regard the maximal height difference hfsmax, to obtain the universal free surfaces for three different immersion depths in Figures 4, 5, and 6 where the free surfaces are defined as the contour of αa=0.5.Figure 4
Universal profiles of the free surface at differentσv, h/H=0.25.Figure 5
Universal profiles of the free surface at differentσv, h/H=0.50.Figure 6
Universal profiles of the free surface at differentσv, h/H=0.75.It can be observed from the figures that the free surface’s shapes of the cases are close to each other forσv<0.103(h/H=0.25), σv<0.109(h/H=0.50), and σv<0.116(h/H=0.75) respectively, approaching the curve of the Gauss function h¯fs=h¯fs0+Ae-0.5((x¯-xc)/w)2. Here,  h¯fs=(hfs2-(R2/4))/(hfsmax2-(R2/4)), x¯=x/Lc; the values of h¯fs0, A, xc, and w are listed in Table 1. In order to satisfy the requirement of the normalization, the value of  A+h¯fs0 must be one. The level of the free surface for the remained cases is relatively higher. In particular, the irregularity of the deformation of the free surface is more distinct when σv is greater than about 0.25.Table 1
Parameters for fitted curves of the free surface.
h/Hh¯fs0Axcw0.25010.480.3090.50010.500.3190.75010.520.325The influence of the free surface is quite different from that of the bottom wall on the shape of the cavity. Thus, the upper and the lower surface of the cavity must be discussed, respectively.Figures7, 8, and 9 present the profiles of the upper surface of the cavity when the cavity width Rup is normalized as to the maximal cavity width Rupmax, where the cavity width is defined as the vertical length from any specific point on cavity surface to the symmetry line of the 2D wedge.Figure 7
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.25.Figure 8
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.50.Figure 9
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.75.One can see that the upper surfaces of the cavity present pretty good unity in the cases forσv<0.103(h/H=0.25), σv<0.109(h/H=0.50), and σv<0.116(h/H=0.75), respectively. However, for other cases, the width of the back part of the cavity is much bigger, with a concave distortion in the vicinity of the cavity closure because of the reentrant jet. By direct translating the fitted curves in Figures 4–6 to be compared with the scattered cavity profiles in Figure 7–9, it was found that the shape of the free surface is similar to that of the upper surface of the cavity in the cavitation region. Such phenomenon owes to the flexibility of the free surface which deforms along with the development of cavity surface. All the parameters for the fitted curves in Figures 7–9 are given in Table 2. Strictly, the shape of the cavity’s upper surface is more appropriate to the curve of parabolic function. Here, the curves of Gauss function are adopted just for illustration of the similarity between profiles of the upper cavity surface and of the free surface.Table 2
Parameters for fitted curves of the upper surface of the cavity.
h/Hh¯fs0Axcw0.25−0.451.450.470.3090.50−0.421.420.500.3190.75−0.451.450.500.325Additionally, Figures10, 11, and 12 present the profiles of the lower surface of the cavity. The lower cavity width Rlow is normalized as to the maximal lower width Rlowmax.Figure 10
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.25.Figure 11
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.50.Figure 12
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.75.A close observation shows the irregular deformation in the tailing part of the cavity in the cases forσv>0.202(h/H=0.25), σv>0.206(h/H=0.50), and σv>0.212(h/H=0.75) respectively, which results from the shedding and concavity of the cavity caused by reentrant jet. As a whole, the lower surface of the cavity has relatively poorer similarity with the increasing immersion depth. In the major part of the cavitating zone, the lower surface looks much flatter than the upper one. This is actually due to the existence of the rigid bottom wall, which prevents the lower surface of the cavity from developing in the vertical direction. Because there is a big difference in shapes of the cavity’s lower surface, it is difficult that a normalized fitted curve can be given for each of the three immersion depths.Figures13, 14, and 15 present the relations between the cavitation number with positions located in the maximum of the level of free surface as well as the width of cavity surface.Figure 13
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.25.Figure 14
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.50.Figure 15
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.75.Forh/H=0.25, the position located in the maximal level of the free surface is very close to those in the maximal widths of the upper and lower surfaces of cavity. This indicates the shapes of the free surface and the cavity surfaces preserve symmetry. Along with the increase of the immersion depth, for σv>0.2 in the rough, the positions for the maximal widths of the upper and lower surface of cavity are close to each other, but the position for the maximal level of the free surface obviously moves backward. When the cavitation number σv is roughly less than 0.2, the position located in the maximal level of the free surface is still close to that in the maximal width of the cavity’s upper surfaces, which implies that the profiles of the free surface and the cavity’s upper surface maintain right-and-left symmetry. However, for h/H=0.50 and σv<0.1 or h/H=0.75 and σv<0.2, with the dropping σv, the position for the maximal width of the cavity’s lower surface moves forward, which reveals that the up-and-down symmetry shape of the cavity surface is destroyed. By these geometrical results, one can see that the influence of the rigid solid wall on the shape of the free surface and cavity interface is much stronger than that of the flexible free surface.


### 4.3. Hydrodynamic Coefficients

The instability of the cavity could also induce the oscillation of the hydrodynamic coefficients, taking curves, for example, as illustrated in Figures16 and 17. So, we will still analyze the cases of steady type cavity in this section.Figure 16
Variation ofCd and Cl along with σv, h/H=0.50, σv=0.507, transition type cavity.Figure 17
Variation ofCd and Cl along with σv,h/H=0.75, σv=1.808, wake-vortex type cavity.Figures18 and 19 present the relations between the cavitation number σv and the predicted drag and lift coefficients defined as  Cd=Fx/0.5ρlV∞2c and Cl=Fy/0.5ρlV∞2c, where Fx and Fy, respectively, stand for the component of the resultant force acting on the wedge in x direction and y direction.Figure 18
Relations betweenCd and σv.Figure 19
Relations betweenCl and σv.It is clearly revealed from the curves that the drag coefficient becomes large gradually with an increase in cavitation number, whereas the lift coefficient curves describe a negative slope in the present computational range of the cavitation number. Furthermore, especially when the cavitation number is less than about 0.1, the boundary effect of the free surface has an stronger influence on the drag coefficient for smaller immersion depth, whereas the boundary effect of the solid wall exerts an stronger influence on the lift coefficient for larger immersion depth. Such complicated influence on hydrodynamic coefficients mainly results from the different range of the cavitating zone and the displacement of the stagnation point near the tip of the wedge which is correlated to a change in circulation around the wedge [4].


## 4.1. Cavity Pattern

Figure2 presents the typical cavity patterns with a free surface at some specific values of cavitation number, which is defined as σv=(P∞-pv)/0.5ρlV∞2. The cavity outline is defined as the interface where the isosurface of αv=0.5 locates. Here, pv indicates the saturated vapor pressure of water at specific temperature and the P∞ and V∞ denote the upstream pressure and velocity at inlet boundary on y=0.Three cavity patterns: (a) steady type; (b) transition type; (c) wake-vortex type; the upper is the contour of the volume fraction of water; the lower is the contour of the magnitude of the vorticity.
(a)(b)(c)It seems obvious that the size of the cavity becomes smaller if the cavitation number increases. According to contours of the volume fraction of water and the magnitude of the vorticity, cavity patterns can be roughly divided into the three types as follows.(a)Steady Type: the cavitation number σv is approximately in the range of 0.05~0.3. The cavity presents the state of supercavity which is almost full of vapor. The cavity retains a stable shape except for some tiny oscillations near the tail of the cavity. The magnitude of the vorticity is much higher near the cavity surface, at the tailing part of the cavity, and behind the wedge.(b)Transition Type: the cavitation number σv is approximately in the range of 0.3~0.5. The cavity presents the state of cloudy mixture composed of vapor and liquid, which is produced by the strong reentrant jet generated from the tail of the cavity. The cavity can roughly keep relatively clear outline. The magnitude of the vorticity is much higher in the band-shaped zones originated from the ends of the wedge’s base.(c)Wake-Vortex Type: the cavitation number σv is approximately in the range of 0.5~2.04. The cavity presents the state of vortex cavitation, which occurs in shedding vortices of the wake flow and exhibits an evident periodicity.For the steady type of the cavity pattern, three relationships of cavity lengthLc      with the cavitation number σv is shown in Figure 3 where scattered symbols represent the numerical values and solid curves [4] were fitted from experimental data. Good agreement can be observed from the case of h/H=0.25, whereas the relative errors between the numerical and the experimental results get obvious for the other immersion depths. This fact could be due to the reason that the fitted curves of the experiments were obtained from the working condition of about σv>0.1 in the cases of h/H>0.25. These curves could not completely describe the present computational results in the range of σv<0.1 at the immersion depth of h/H>0.25.Figure 3
Relations betweenLc and σv.For a fixed cavitation number, the cavity length is increasing when the immersion depth goes upward. The boundary effect of the solid wall is much stronger than that of the free surface, which enables the flow blocked to make the local cavitation number decrease and the cavity size enlarge.


## 4.2. Shapes of Free Surface and Cavity Interface

Because shapes of the transition type and the wake-vortex type of cavity are too unstable to be analyzed quantitatively, only the steady type of cavity was selected to be discussed in this section.The height differenceshfs between the free surfaces at the conditions of deformation and of stillness are normalized as regard the maximal height difference hfsmax, to obtain the universal free surfaces for three different immersion depths in Figures 4, 5, and 6 where the free surfaces are defined as the contour of αa=0.5.Figure 4
Universal profiles of the free surface at differentσv, h/H=0.25.Figure 5
Universal profiles of the free surface at differentσv, h/H=0.50.Figure 6
Universal profiles of the free surface at differentσv, h/H=0.75.It can be observed from the figures that the free surface’s shapes of the cases are close to each other forσv<0.103(h/H=0.25), σv<0.109(h/H=0.50), and σv<0.116(h/H=0.75) respectively, approaching the curve of the Gauss function h¯fs=h¯fs0+Ae-0.5((x¯-xc)/w)2. Here,  h¯fs=(hfs2-(R2/4))/(hfsmax2-(R2/4)), x¯=x/Lc; the values of h¯fs0, A, xc, and w are listed in Table 1. In order to satisfy the requirement of the normalization, the value of  A+h¯fs0 must be one. The level of the free surface for the remained cases is relatively higher. In particular, the irregularity of the deformation of the free surface is more distinct when σv is greater than about 0.25.Table 1
Parameters for fitted curves of the free surface.
h/Hh¯fs0Axcw0.25010.480.3090.50010.500.3190.75010.520.325The influence of the free surface is quite different from that of the bottom wall on the shape of the cavity. Thus, the upper and the lower surface of the cavity must be discussed, respectively.Figures7, 8, and 9 present the profiles of the upper surface of the cavity when the cavity width Rup is normalized as to the maximal cavity width Rupmax, where the cavity width is defined as the vertical length from any specific point on cavity surface to the symmetry line of the 2D wedge.Figure 7
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.25.Figure 8
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.50.Figure 9
Universal profiles of the upper surface of the cavity at differentσv, h/H=0.75.One can see that the upper surfaces of the cavity present pretty good unity in the cases forσv<0.103(h/H=0.25), σv<0.109(h/H=0.50), and σv<0.116(h/H=0.75), respectively. However, for other cases, the width of the back part of the cavity is much bigger, with a concave distortion in the vicinity of the cavity closure because of the reentrant jet. By direct translating the fitted curves in Figures 4–6 to be compared with the scattered cavity profiles in Figure 7–9, it was found that the shape of the free surface is similar to that of the upper surface of the cavity in the cavitation region. Such phenomenon owes to the flexibility of the free surface which deforms along with the development of cavity surface. All the parameters for the fitted curves in Figures 7–9 are given in Table 2. Strictly, the shape of the cavity’s upper surface is more appropriate to the curve of parabolic function. Here, the curves of Gauss function are adopted just for illustration of the similarity between profiles of the upper cavity surface and of the free surface.Table 2
Parameters for fitted curves of the upper surface of the cavity.
h/Hh¯fs0Axcw0.25−0.451.450.470.3090.50−0.421.420.500.3190.75−0.451.450.500.325Additionally, Figures10, 11, and 12 present the profiles of the lower surface of the cavity. The lower cavity width Rlow is normalized as to the maximal lower width Rlowmax.Figure 10
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.25.Figure 11
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.50.Figure 12
Universal profiles of the lower surface of the cavity at differentσv, h/H=0.75.A close observation shows the irregular deformation in the tailing part of the cavity in the cases forσv>0.202(h/H=0.25), σv>0.206(h/H=0.50), and σv>0.212(h/H=0.75) respectively, which results from the shedding and concavity of the cavity caused by reentrant jet. As a whole, the lower surface of the cavity has relatively poorer similarity with the increasing immersion depth. In the major part of the cavitating zone, the lower surface looks much flatter than the upper one. This is actually due to the existence of the rigid bottom wall, which prevents the lower surface of the cavity from developing in the vertical direction. Because there is a big difference in shapes of the cavity’s lower surface, it is difficult that a normalized fitted curve can be given for each of the three immersion depths.Figures13, 14, and 15 present the relations between the cavitation number with positions located in the maximum of the level of free surface as well as the width of cavity surface.Figure 13
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.25.Figure 14
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.50.Figure 15
Positions located in the maximal level of the free surface and the maximal width of the cavity surface at differentσv, h/H=0.75.Forh/H=0.25, the position located in the maximal level of the free surface is very close to those in the maximal widths of the upper and lower surfaces of cavity. This indicates the shapes of the free surface and the cavity surfaces preserve symmetry. Along with the increase of the immersion depth, for σv>0.2 in the rough, the positions for the maximal widths of the upper and lower surface of cavity are close to each other, but the position for the maximal level of the free surface obviously moves backward. When the cavitation number σv is roughly less than 0.2, the position located in the maximal level of the free surface is still close to that in the maximal width of the cavity’s upper surfaces, which implies that the profiles of the free surface and the cavity’s upper surface maintain right-and-left symmetry. However, for h/H=0.50 and σv<0.1 or h/H=0.75 and σv<0.2, with the dropping σv, the position for the maximal width of the cavity’s lower surface moves forward, which reveals that the up-and-down symmetry shape of the cavity surface is destroyed. By these geometrical results, one can see that the influence of the rigid solid wall on the shape of the free surface and cavity interface is much stronger than that of the flexible free surface.


## 4.3. Hydrodynamic Coefficients

The instability of the cavity could also induce the oscillation of the hydrodynamic coefficients, taking curves, for example, as illustrated in Figures16 and 17. So, we will still analyze the cases of steady type cavity in this section.Figure 16
Variation ofCd and Cl along with σv, h/H=0.50, σv=0.507, transition type cavity.Figure 17
Variation ofCd and Cl along with σv,h/H=0.75, σv=1.808, wake-vortex type cavity.Figures18 and 19 present the relations between the cavitation number σv and the predicted drag and lift coefficients defined as  Cd=Fx/0.5ρlV∞2c and Cl=Fy/0.5ρlV∞2c, where Fx and Fy, respectively, stand for the component of the resultant force acting on the wedge in x direction and y direction.Figure 18
Relations betweenCd and σv.Figure 19
Relations betweenCl and σv.It is clearly revealed from the curves that the drag coefficient becomes large gradually with an increase in cavitation number, whereas the lift coefficient curves describe a negative slope in the present computational range of the cavitation number. Furthermore, especially when the cavitation number is less than about 0.1, the boundary effect of the free surface has an stronger influence on the drag coefficient for smaller immersion depth, whereas the boundary effect of the solid wall exerts an stronger influence on the lift coefficient for larger immersion depth. Such complicated influence on hydrodynamic coefficients mainly results from the different range of the cavitating zone and the displacement of the stagnation point near the tip of the wedge which is correlated to a change in circulation around the wedge [4].


## 5. Conclusions

In the present work, the natural cavitating flows around a two-dimensional wedge in shallow water were numerically investigated, by using the single-fluid multiphase flow model based on RANS equation coupled with a cavitation model. The influence of two types of boundaries on the cavity pattern, the shape of the free surface and hydrodynamic characteristics was studied. The following conclusions can be drawn by analysis and comparisons.Firstly, in the range of the calculated cavitation number (0.05~2.04), cavity patterns can be divided into three types as steady type, transition type, and wake-vortex type. The successful simulation of the cavity of wake-vortex type demonstrates that the viscous multiphase model has an evident advantage over the numerical methods in traditional framework of potential flow.In fact, the classes of cavity patterns here are still rough. Much more computation in a wider and finer range of cavitation number should be carried on to precisely determine the threshold value of cavitation number between two types of cavity pattern.Secondly, for the cavity of steady type, the numerical results can be found to be quite in accordance with the experimental ones in the case of relative small immersion depth. But the deviation of the numerical values from the experimental data gets obvious for larger depths, especially at the cavitation numbers less than 0.1. Along with the reduction of the cavitation number, the cavity size increases as well as the deformation zone of the free surface. The free surface generally keeps consistent with the upper surface of the cavity in their shapes. However, the lower surface of the cavity looks much flatter due to the restriction of its growth in vertical direction by the effect of the rigid bottom wall. The position located in the maximal width of the cavity’s lower surface moves forward gradually with the dropping cavitation number, which destroys the symmetry of the cavity shape.Finally, the drag coefficient becomes large gradually with an increase in the cavitation number, while the lift coefficient curves describe a negative slope in the present computational range of cavitation number. Furthermore, when the cavitation number is smaller than about 0.1, the boundary effect of the free surface has a stronger influence on the drag coefficient for smaller immersion depth, whereas the boundary effect of the solid wall exerts a stronger influence on the lift coefficient for larger immersion depth.



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*Source: 257539-2011-11-28.xml*