Twodimensional nonlinear parametric sloshing in the irregular tanks: numerical analysis and experimental investigation
LiShi Wang^{1} , Zhuang Wang^{2} , YuChun Li^{3}
^{1, 3}Department of Hydraulic Engineering, Tongji University, Shanghai 200092, China
^{2}Department of Civil Engineering, Jiangnan University, Wuxi 214122, China
^{3}Corresponding author
Journal of Vibroengineering, Vol. 19, Issue 3, 2017, p. 21532163.
https://doi.org/10.21595/jve.2016.17217
Received 30 May 2016; received in revised form 6 September 2016; accepted 19 September 2016; published 15 May 2017
JVE Conferences
The finite volume and volume of fluid (VOF) methods are used to simulate the twodimensional nonlinear parametric sloshes in the Ushaped and the circular tanks. An experiment is simultaneously conducted to observe and measure the responses of twodimensional nonlinear parametric sloshes. The natural frequencies and the nonlinear steadystate amplitudefrequency responses are respectively acquired and compared by numerical and experimental methods. The numerical results have a good agreement with the experimental values. Because the viscous damping is automatically considered in the numerical simulations, the steadystate wave amplitudes of parametric resonance (sloshing) are well predicted. The finite volume and VOF techniques aided by Fluent Code can be a practical tool for the engineers to analyze the longtime nonlinear parametric sloshing in arbitraryshape tanks.
Keywords: parametric sloshing, nonlinear steadstate responses, irregular tanks, finite volume method, volume of fluid (VOF), experiment.
1. Introduction
Liquid parametric sloshing, known also as Faraday waves, has been a long standing subject of interest [1, 2]. Parametric sloshing refers to the motion of the liquid free surface due to the periodic restoring force acting on free surface. The 1/2 subharmonic (or principle) parametric resonance will generate when the liquid container is vertically excited at a frequency close to twice the natural frequency of the free surface, leading to the exponential increase of the wave amplitude. This resonance phenomenon was first experimentally observed and studied by Faraday [3].
Parametric sloshing exists in many engineering fields. In aerospace engineering, parametric sloshing of liquid fuel has significant influences on the management and stability of a space vehicle because the additional sloshing forces and torques can interact with the control system through a feedback loop [4, 5]. In ocean engineering, the violent sloshing is often encountered in an oil tanker or Liquefied Natural Gas container under the actions of sea waves [6, 7]. The contained fluid in the ship might experience a parametric resonance (sloshing) due to the vertical excitation of see waves. In the watertransmission engineering, the parametric sloshing of water may occur in the longspan aqueduct bridges (such as the suspension aqueduct bridge) because of the wind vortexinduced vibration. The parametric sloshing of water may have a negative effect on structural safety of the aqueduct bridge. Theoretical prediction of the parametric sloshing response is very important to the related engineering designs.
The linear theory of parametric sloshing is capable of determining the stability boundaries of the free surface. The instabilities of (linear) parametric sloshing were fully studied by Benjamin and Ursell [8], Abramson [9], Dodge et al. [10], Woodward and Bauer [11], Kumar [12], as well as Li and Wang [13] etc.
When parametric resonance (sloshing) occurs, the wave amplitude on the free surface will not increase infinitely but turn into a steadystate oscillation or a limitcycle motion due to the nonlinear effect of free surface motion. The nonlinear theory of parametric sloshing can predict the steadystate response and uncover complex freesurface dynamic behaviors of fluid. Frandsen [14] used a fully nonlinear ﬁnite difference method for studying a twodimensional sloshing in the rectangular tank which was moved both horizontally and vertically. Horsley and Forbes [15] studied the timeperiodic solutions about the subharmonic resonance based on both the full and weakly nonlinear theories. Kolukula and Chellapandi [16] employed a fully nonlinear finite element method to analyze the response of the plane freesurface. Wang et al. [17] used the SPH method to simulate the nonlinear parametric sloshing. Faltinsen et al. [18] developed an analytical multidimensional modal method to calculate the longtime steadstate nonlinear sloshing in a rectangular tank. Faltinsen and Timokha [19, 20] further extended the multimodal approach to the liquid sloshes in the circular and spherical tanks.
There are still some problems that need to be solved in the theoretical simulations of nonlinear (parametric) sloshing. A general drawback of certain numerical methods is the limited ability to perform (longtime) steadstate simulations. The long time simulations are needed to obtain statistical estimates for the engineering designs. The linear damping ratio is usually introduced in the analytical methods (e.g. the multimodal method [1820]) for estimating the damping effect of nonlinear sloshing. It is known that the fluid damping plays an important role in steadstate resonance responses. So, it is difficult to accurately evaluate the nonlinear resonance responses by using the linear damping ratio, which is obtained under the condition of (linear) smallamplitude slosh. In fact, the sloshing damping, which almost always exceeds analytical predictions [21, 22], depends on the viscous dissipation at the rigid boundary of the tank, the viscous dissipation on the free surface and the viscous damping in the interior fluid. Most of the existing studies focus on the parametric sloshing in the rectangular tanks. The parametric sloshing in the irregular (nonrectangular) tank has been seldom studied due to mathematical difficulties.
The present work is the prophase study on the water parametric sloshing caused by vortexinduced vibration in the longspan aqueduct bridges. We use the finite volume and VOF methods (Fluent Code) to simulate the nonlinear parametric sloshing in the Ushape and circular tanks, since the Ushaped and circular section aqueducts are often adopted in the longspan water transmission bridges. The fluid domain is modeled by using a finite volume approximation, and the air–water (free) interface is tracked using a volume of fluid (VOF) technique. The nonlinear parametric sloshes in the two irregular tanks are simultaneously observed and measured in an experiment. The waveheight, natural frequencies and steadstate amplitudefrequency responses are respectively acquired and compared by numerical and experimental methods. The purpose of this paper is to establish a practical numerical approach for simulating nonlinear parametric sloshing. The advantages of this method are that it is applicable to the arbitrary shape tanks, and it can be used to simulate the longtime steadstate resonance responses and complex damping effect of the viscous fluid in largeamplitude sloshing.
2. Numerical analysis
2.1. Finite volume method for fluid motions
The continuity and momentum equations of a fluid are respectively presented as follows [23]:
where $U$ is the velocity vector of fluid; $p$ is the pressure of fluid; $\rho $ and $\mu $ are respectively the density and dynamic viscosity of the fluid; ${S}_{M}$ is the source term. A finite volume approach is used to discretize and integrate the governing equations of fluid flow over solution domain which was subdivided into a finite number of small control volumes. The finite volume approach can guarantee the conservation of a fluid property $\varphi $ in a finite control volume. For example, a general flow variable $\varphi $ may be a velocity component or enthalpy within a finite control volume. If a general variable $\varphi $ is introduced, the conservative form of Eqs. (12) can be written in the following form [23]:
where ${\mathrm{\Gamma}}_{\varphi}$ is the diffusion coefficient, ${S}_{\varphi}$ is the generalized source term. The Eq. (3) is the socalled transport equation for property $\varphi $. By setting $\varphi $ equal to different variable and selecting appropriate values for the diffusion coefficient and source term, we can obtain continuity and momentum equations. For the twodimensional parametric sloshing, the variables and parameters of the Eq. (3) are presented in Table 1.
Table 1. The variables and parameters of the Eq. (3)
Conservation equation

$\varphi $

${\mathrm{\Gamma}}_{\varphi}$

${S}_{\varphi}$

Mass

1

0

0

$x$momentum

$u$

$\mu $

$(\partial p/\partial x)$

$y$momentum

$v$

$\mu $

$(\partial p/\partial y)\rho g\rho {a}_{y}$

Note: $u$ and $v$ are respectively the horizontal and vertical components of the velocity $U$; $g$ and ${a}_{y}$ are respectively the acceleration of gravity and the vertical exciting acceleration

The integration of Eq. (3) over a control volume $V$ yields:
Applying Gauss divergence theorem, we rewrite Eq. (4) as follows:
where $n$ is the unit vector normal to surface element $dA$; $A$ is the entire bounding surface. The flow variable $\varphi $ can be expressed as a balance between the various processes tending to increase or decrease it. So, we have:
$=\left[\begin{array}{l}\text{Rateofincreaseof}\\ \varphi \text{duetodiffusion}\end{array}\right]\text{+}\left[\begin{array}{l}\text{Rateofincreaseof}\\ \text{to}\varphi \text{duetosources}\end{array}\right].$
The Eq. (6) proves the conservation of a fluid property $\varphi $ for a finite control volume at specific times. Because a twodimensional sloshing model is only discussed in this study, the control volume is degenerated into the control area, and the area integral into the boundary line integral.
2.2. Volume of fluid (VOF) technique for tracking free surface
The free surface was tracked by using a volume of fluid (VOF) technique. The concept of VOF was first proposed by Hirt and Nichols [24]. This method is shown to be more flexible and efficient than other methods for treating the complicated free boundary deformations. A new variable, i.e. the volume fraction $F(x,y,z,t)$ which represents the fractional volume of the cell occupied by specified fluid, is introduced. A unit value of $F$ would correspond to a cell full of specified fluid, while a zero value would indicate that the cell contained no specified fluid [24, 25]. The air and water phases can be defined by the variable $F$. The interface between air and water is an averaged fractional volume of a mixture of the phases. $F(x,y,z,t)$ is defined as:
The time dependence of $F(x,y,z,t)$ is governed by the equation [24, 25]:
The key issue using the VOF method is the discretization of the Eq. (8). Several discrete methods have been proposed by many researchers such as Hirt and Nichols [24], Noh and Woodward [26], Ubbink [27] and Youngs [28].
The density and dynamic viscosity are the mixture values, which can be expressed as [29]:
where ${\rho}_{water}$ and ${\rho}_{air}$ are respectively the water density and air density; ${\mu}_{water}$ and ${\mu}_{air}$ are the water and air dynamic viscosity, respectively. It assumes that the velocities of the two phases are continuous across the interface. Substituting Eq. (9) into Eqs. (12), we can obtain the velocity and pressure by using the finite volume method.
2.3. Numerical test model
The two irregular tanks, as shown in Fig. 1, are used for present study. The tanks are filled with water. The bottom (inner) radius of Ushape tank is 100 mm with the water depth of $H=$115 mm. The inner radius of circular tank is 125 mm with the water depth of $H=$160 mm. The coordinates oxy is fixed to the tank. The $x$ axis is in the plane of free surface, and y axis points vertically upwards through the midpoint of the free surface.
Fig. 1. Two numerical test models (unit: mm)
The finite volume and explicit VOF techniques in the Fluent Code are employed to simulate nonlinear parametric sloshing in the tanks. The two tanks are both excited by a vertical acceleration ${a}_{y}={a}_{0}\mathrm{s}\mathrm{i}\mathrm{n}\left(2\pi ft\right)$, in which ${a}_{0}$ and $f$ are respectively the amplitude and frequency of the sinusoidal excitation. The top boundaries of the tanks are defined as the pressure outlets ($p=0$), as shown in Fig. 1. The rest boundaries of the tanks are defined as no slip walls. Quadrilateral structured meshing is done for the given control volume to reduce the accumulated error. The effect of the surface tension is not included in the numerical model. The model and parameter settings for the Fluent Code are presented in Table 2.
Table 2. Model and parameter settings for the fluent code
Model and parameter

Setting

Solver type model

PressureBased Multiphase, VOF

Spatial discretization pressure

PRESTO

Viscous model

RNG $k$$\epsilon $

Tracking free surface method

GeoReconstruct

Water Viscosity (kg/ms)

0.001

Water Density (kg/m^{3})
Air Viscosity (kg/ms)
Air Density (kg/m^{3})

998.2
1.789×10^{5}
1.225

YGravity (m/s^{2})
Time step size (s)

–9.81
0.005

3. Experimental investigation
In our previous study [13], a twodimensional parametric sloshing experiment was conducted for a fluid in the rectangular, circular and Ushaped tanks. The previous experiment was only for the stability analyses of parametric sloshing, which belongs to the scope of linear parametric sloshing. In present experimental study, we focus on the steadstate responses of liquid, which fall into the scope of the nonlinear parametric sloshing.
The present test devices, being same as the preceding experiment [13], are illustrated in Fig. 2. The experimental devices consist of three systems, i.e. an excitation system, an acceleration acquisition system and a waveheight measurement system. A sinusoidal signal is respectively produced and amplified by the signal generator and the power amplifier, and then transmitted to the vibration exciter. The vibration exciter exerts a vertical sinusoidal acceleration on the tank. The vertical acceleration signal of the tank is respectively collected, analyzed and recorded by the accelerometer, the dynamic signal analyzer, and computerA. A laser displacement sensor is fixed on the rigid tank to measure the wave height on the liquid free surface. The light signal is captured by the laser displacement sensor and the data acquisition instrument, and then analyzed and recorded by the signal analyzer and computerB, respectively.
Fig. 2. Experimental diagram
The test tanks, made of Plexiglas, are constructed as the flatshape containers so as to simulate the twodimensional sloshing. The height and width of the filled water are same as the numerical models shown in Fig. 1. The water is dyed white so that the liquid free surface can reflect the light that the laser sensor emits. The principal parametric sloshes (resonances) in the Ushaped and circular tanks can be respectively aroused by the vibration exciter in the unstable domains, which were discussed in details in [13].
4. Comparison between numerical and experimental results
4.1. The natural frequency
When the forcing frequency of the vertical acceleration is about twice the $j$th natural frequency of fluid, the principal (subharmonic) parametric slosh of mode $j$ can be excited by the vertical acceleration. After the excitation is stopped, the freeattenuation responses of waveheight in mode j can be numerically and experimentally obtained, respectively, and the natural frequencies can be calculated by using FFT. The measured locations of wave height for the two tanks are shown in Tables 3 and 4 (see Fig. 1). The numerical solutions and experimental values of the first four natural frequencies for the two tanks are respectively presented in Tables 3 and 4, in which the measured frequencies were obtained in the previous study [13]. The maximum relative errors of the frequencies between numerical and measured values are within 1.6 % accuracy. The numerical solutions agree well with the experimental results. It is shown that the Fluent Code (finite volume and VOF techniques) can accurately calculate the natural frequencies of sloshing fluid in the irregular tanks.
Table 3. The IIV natural frequencies (Ushape tank)
Numbers of mode

Fluent code (Hz)

Measured (Hz) [13]

Measured location of wave height (mm)

Error values (%)

I

1.85

1.85

$x=$ –85

0.00

II

2.70

2.74

$x=$0.0

1.48

III

3.40

3.38

$x=$ –33.0

0.73

IV

3.90

3.90

$x=$0.0

0.05

Table 4. The IIIV natural frequencies (Circular tank)
Numbers of mode

Fluent code (Hz)

Measured (Hz) [13]

Measured location of wave height (mm)

Error values (%)

II

2.49

2.53

$x=$0.0

1.6

III

3.10

3.09

$x=$ –40.0

0.10

IV

3.60

3.58

$x=$0.0

0.33

4.2. Steadstate amplitudefrequency responses
The principal parametric sloshes (resonances) of the first four modes in the Ushaped and circular tanks can be respectively aroused in the unstable domains. The full timehistory responses of the wave height of the first four resonances are respectively simulated and measured by the numerical and experimental methods. The measured locations of wave height for the two tanks are same as those in Section 4.1, as shown in Tables 3 and 4. Fig. 3 and 4 respectively show the free surface shapes of principal parametric resonances of modes IIV for the Ushaped and circular tanks.
The two typical timehistory response curves of the 2ndmode principal parametric sloshes in the Ushaped and circular tanks are respectively presented in Figs. 5 and 6, from which it can be seen that each free surface elevation (at $x=$0.0) experiences an unstable process, and then turns into a steadystate oscillation or a limitcycle motion. In the steadystate phase, the wave amplitudes exceed the range of linear motion, and the upward amplitudes are greater than the downward amplitudes. It should be pointed out that the full timehistory response curve of waveheight depends on the initial conditions of the free liquid surface. Because the initial disturbances (conditions) in the test are random and cannot be measured accurately, it is difficult to compare the numerical and experimental timehistory curves in one figure. However, the steadstate wave amplitudes of parametric sloshing do not rely on the initial conditions. It can be found from Figs. 5 and 6 that the numerical and experimental wave amplitudes agree well.
Fig. 3. Free surface shapes of principal parametric resonances of modes IIV (Ushape tank)
a) Numerical simulation
b) Experimental simulation
Fig. 4. Free surface shapes of principal parametric resonances of modes IIV (Circular tank)
a) Numerical simulation
b) Experimental simulation
According to the stabilityboundary charts of subharmonic response (principal parametric resonance) in [13], if the exciting amplitude is fixed, then there is an unstable frequency domain for each sloshing mode. In each unstable domain, the steadystate wave amplitude varies with the driving frequency.
Figs. 7 and 8 respectively show the steadstate (upward) amplitudefrequency responses in unstable regions for the principal parametric resonances in the Ushaped and circular tanks (modes IIIV). The calculated locations on liquid surface of wave height are same as the measured locations (see Tables 3 and 4). It can be seen from Figs. 7 and 8 that the numerical solutions agree well with the experimental results.
It can be found that the wave magnitude suddenly reaches to zero at the two endpoints of the unstable regions. These “jump” behaviors are similar to the other experimental observations (e.g. Dodge et al. [10]). From Figs. 7 and 8, it can also be found that the lefttoright amplitude gradually decreases with the increase of forcing frequency. This behavior of parametric sloshing is similar to that in the cylindrical tank [10].
It is noted that when the resonance of mode 1 occurs in the circular tank, the surface wave will overturn at the wall so that the waveheight near the wall is difficult to measure. As a result, the steadstate amplitudefrequency response of mode 1 in the circular tank is not extracted here.
The numerical method (Fluent Code) can do a reasonably good job of modeling the nonlinear parametric sloshing, and give a good prediction of the wave (upward) amplitudes.
Fig. 5. Numerical and experimental waveheight responses (at $x=$0.0) of principal parametric resonance of mode II under the same excitation (Ushape tank)
a) Numerical result
b) Experimental result
Fig. 6. Numerical and experimental waveheight responses (at $x=$0.0) of principal parametric resonance of mode II under the same excitation (Circular tank)
a) Numerical result
b) Experimental result
Fig. 7. Steadstate amplitudefrequency responses of the IIV mode principal parametric resonances in the unstable domains (Ushape tank)
Fig. 8. Steadstate amplitudefrequency responses of the IIIV mode principal parametric resonances in the unstable domains (circular tank)
5. Conclusions
The finite volume and VOF techniques (Fluent Code) were successfully applied for predicting the twodimensional nonlinear parametric sloshing. A twodimensional parametric sloshing experiment was conducted for a fluid in the Ushape and circular tanks. The natural sloshing frequencies and the long timehistory steadstate responses of free surface elevations were respectively obtained by numerical and experimental methods. The numerical and experimental results agree well. The finite volume and VOF techniques (Fluent Code) are the efficient tools for solving the longtime nonlinear parametric sloshes in the general irregular tanks, and can give a good prediction of the steadstate wave amplitude. The finite volume and VOF techniques aided by Fluent Code can be a practical tool for the engineers to analyze the nonlinear parametric sloshing. The mechanism of nonlinear steadstate parametric sloshing needs a further study.
Acknowledgements
This study is supported by the National Science Foundation of China (Grant No. 51279133). The authors gratefully acknowledge this financial support.
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