Research Article  Open Access
Guoping Li, Eryun Chen, Ailing Yang, Zhibin Xie, Gaiping Zhao, "Effect of Guide Vanes on Flow and Vibroacoustic in an AxialFlow Pump", Mathematical Problems in Engineering, vol. 2018, Article ID 3095890, 11 pages, 2018. https://doi.org/10.1155/2018/3095890
Effect of Guide Vanes on Flow and Vibroacoustic in an AxialFlow Pump
Abstract
An effect of guidevane numbers on pressure fluctuations and structural vibroacoustics induced by unsteady flow is performed by a hybrid numerical method. A 3D flow field is simulated in axialflow pump with four impeller blades, in which three diffuser models with 5, 7, and 9 vanes are devised to match, respectively. A full scale structural vibroacoustics coupled model is solved using LMS acoustics software. The results show that the bladepassing frequency (BPF) is dominated frequency of the vibration acceleration of pump, which is consistent with frequency spectral characteristics of pressure pulsation. The unsteady pressure fluctuating becomes strong as the flow discharge decreases from 1.0Qv to 0.6Qv, the circumferential unsteady behavior of which is more severe due to flow nonuniformity induced by the suction elbow at partial operation. Generally, the pressure fluctuating increases slightly when the flow discharge increases from 1.0Qv to 1.3Qv. Moreover, pressure fluctuations amplitude on the pump with 9vane diffuser is small relative to other two models and the vibrating accelerating and radiation sound field at BPF are also slight relatively, which indicates that appropriate guidevane numbers contribute to suppress pressure fluctuations and vibroacoustics in axialflow pump. The conclusions in the present paper can provide theoretical guidance for low vibration pump design.
1. Introduction
Axialflow pumps are usually selected for pumping large flow rate against relatively low heads [1] and widely used in the military, marine, agricultural, and biomedical fields. It is thus expected that the fluid transportation is accompanied by little vibronoise. The guide vanes mounted in the downstream of the impeller can improve the hydrodynamic performance of the pump by transforming the kinetic energy into pressure energy. But the rotorstator mutual interaction can induce unsteady flow forces on the pump, causing vibration and noise [2], leading to structural fatigue failures. Therefore, the investigation of rotorstator interaction [3–5] effects on pressure fluctuation and vibration in the axialflow pump is of continuous interest.
The interaction between rotor and stator is always a hot issue because it has important influence on the flow structure, performance, and operation stability of the turbomachinery. Experiment study of the flow field structures between the rotors and stators was employed by Zhang [6]. Zierke [7, 8] studied the tip clearance flow field structures using flow visualization experiment technology, giving examples of measured physical phenomena such as endwall boundary layers, separation regions, wakes, and secondary vortical structures. With the rapid development of computers and computational method, the numerical simulation makes even more attractive technique to research the inner flow in pumps. Several numerical studies have been reported in the technical literature on rotor and stator interaction [9–11]. For example, Javadi [9] investigated the precessing helical vortex in a conical diffuser, with rotorstator interaction, which showed the rotorstator interaction is necessary to reproduce the physics of the helical vortex in the draft tube. Liu [10] presents an analytical investigation of stator lean on rotorstator interaction noise in the compressor, which indicated that statorleaned positive has better effect on noise reduction than leaned negative. Rodriguez [11] presents a theoretical analysis that allows us to describe the characteristics in the frequency domain of the vibration originated with the rotorstator interaction in centrifugal pump turbine.
Although these investigations have helped us to deeply understand the nature of such rotorstatorinteraction, the vibroacoustics induced by rotorstator interaction are seldom reported in the axialflow pump. In this paper, we focused on the effect of guide vanes on flow and vibroacoustics in axialflow pump. The NS equations were simulated in axialflow pump with four impeller blades, in which three diffuser models with 5, 7, and 9 vanes are devised to match respectively. A full scale structural vibroacoustics coupled model is solved using LMS acoustics software.
In what follows, the governing equations of the flow field will be explained in Section 2. Vibroacoustics induced by flow will then be described in Section 3. Conclusions close the paper in Section 4.
2. Numerical Simulation
The pump considered in this paper has four impeller blades, in which three diffuser models with 5, 7, and 9 vanes are devised to match, respectively, shown in Figure 1. The characteristic parameters of the pump are the rotor diameter , flow rate at nominal operation condition m^{3}/h, the corresponding pump head , and rotation speed .
2.1. Governing Equations
In present paper, the flow of fluid through the pump is considered as an incompressible fluid. Large eddy simulation (LES) method is applied to solve the filtered NS equation to catch the detailed unsteady flow characteristics. LES focus on solving the large relevant turbulent scales, while small scales are removed from the simulated field with a low pass filter. The effect of the subgrid scales on the resolved scales is considered by an SGS model [12]. The governing equations are the spatially filtered continuity equation and the NavierStokes equations.where is the gridscale velocity component in the direction, the gridscale static pressure, the density, and the kinematic viscosity. Einstein’s summation convention for repeated indices is used. is the subgridscalestress tensor
In the present paper, the classical Smagorinsky model (Smagorinsky, 1963) is adopted, which assume the subgrid stress tensor to be proportional to the resolved rate of strain. Thuswhere is the filtered rate of strain tensor, given by
The eddy viscosity is expressed bywhere is Smagorinsky constant and is filter width.
Central finite difference method is used to discretize the convection terms involved. Momentum and turbulent kinetic energy equations are discretized using secondorder upwind scheme. The NS equations are solved with the commercial code AnsysFluent. Secondorder implicit format is used to discretize the time domain. SIMPLEC algorithm is adopted to calculate the pressurevelocity coupling. Before the unsteady flow solutions, steady flow is first computed and then used as initial condition to unsteady flow calculations. For the unsteady calculation, time step size is set to 1.13e4s, which is equivalent to the time for impeller rotating one degree.
2.2. Computational Domain and Boundary Conditions
Figure 2 describes the computational domain of pump model that is composed of inlet, rotor, stator outlet, and two identical right angle elbows. Moreover, the surface meshes of the rotor and stator are showed. Hexahedral elements are used and the blade zone is about 2.18 million cells, guide vanes zone about 1.37 million cells, the inlet and outlet zones about 537,000, and two elbows parts about 475,000 cells.
(a) 3D models of total domain including inlet, impeller blades, guide vanes, and outlet
(b) Surface mesh of the rotor and stator
The boundary conditions imposed are a constant massflow rate at the inlet, outflow boundary condition at the outlet, and the noslip conditions over wall. Before the unsteady flow solutions (LES), steady flow is first computed ( turbulence model), in which the turbulent intensity is according to the formula to different operating conditions and hydraulic diameter is 0.3m. Other turbulent model constants are , , , , and . Due to the rotation of impeller, two interfaces between the rotor and stator are formed, one of which is between the elbow and the impeller, and the other is between the impeller and guide vane.
2.3. Pressure Fluctuation
Figure 3 describes the monitoring points in the axialflow pump, which is located on different sections along the axial direction, namely, the impeller inlet, tip clearance, the interface between the impeller and guidevane, and guidevane outlet (respectively, located on z=0.033m, z=0.0m, z=0.075m, and z=0.21m), where the points marked P5, P6, P11, and P16 are located at the inner surface of the casing, others at the inside of axial pump. In our previous studied work [13], the frequency spectrum of pressure fluctuations of monitoring points located at the inner surface of the casing was investigated. In this paper, we further evaluated the variation of pressure coefficient fluctuations along the radial direction.
Figure 4 represents the frequency spectrum characteristics of pressure coefficient fluctuations, defined as , at different cross sections inside the axialflow pump with 7 vanes when operating at nominal flow rate, where and are instantaneous pressure and timeaveraged pressure of the monitor points; represents the circumference speed of the impeller outlet. It can be seen that the pressure coefficient fluctuations, caused by impeller rotation, of monitoring points at impeller inlet are dominated by BPF and its harmonic frequency. The amplitude of pressure coefficient fluctuations gradually increases at first from hub to rim along the radial direction and then declines at the point P5 located on the same cross section of the inner surface of the casing as shown in Figure 5. For the vane inlet section (z=0.075m), the amplitude of pressure coefficient fluctuations of monitoring points decreases significantly, which indicates that, after passing the impeller, pressure coefficient pulsation intensity becomes decreasing, and pressure coefficient fluctuations amplitude at low frequency becomes gradually visible. For the guide vanes outlet (z=0.21m), the amplitude of pressure coefficient pulsation of monitoring points continues to decrease. The pressure coefficient fluctuation of bladepassing frequency declines obviously and comparable to that of low frequency, which indicates that the effect of the rotating impeller on vane outlet pressure fluctuations becomes weak.
(a) z=0.033m
(b) z=0.075m
(c) z=0.21m
Figure 5 describes the frequency spectrum of pressure coefficient fluctuations of monitoring points located at the inner surface of the casing with 7 vanes when operating at nominal flow rate, from which it can be seen that the amplitude of pressure coefficient fluctuation is the largest on the point P6 located on the tip clearance, about 1.6 times of that at point P5 located on impeller inlet. The results indicate that nonuniform flow in the tip clearance may be a major contributor to large pressure fluctuation. After passing the impeller and the guidevane, pressure coefficient declines gradually, consistent with that reflected by Figure 4.
To verify the validity of computed results, pressure fluctuations in the axialflow pump casing were measured at the experimental test system as shown in Figure 6. The test system mainly consists of storage water tank, inlet and outlet pipe, control valve, motor, axialflow pump, high frequency sensor, and data acquisition system. Sample frequency is 25600 Hz, sampling number is 65536, and sampling time is 2.56s.
(a) The experimental test system
(b) The rotor and guide vane
Figure 7 shows the comparisons between the computed results and experimental test, where Figures 7(a) and 7(c) represent pressure coefficient fluctuation characteristics in time domain corresponding to point P5 and P6 shown in Figure 3, respectively; Figures 7(b) and 7(d) represent frequency spectrum of pressure coefficient corresponding to point P5 and P6. t/T represents the ratio of computed time and rotor rotating period. These results indicated that pressure fluctuation is periodic and has four peaks and four valleys in one impeller rotation period, which is the same as blade number. The agreements between the numerical simulation and experimental values are relatively well, although small discrepancies do exist, which may be caused by different sampling frequency and sampling number.
(a) Pressure fluctuation characteristics in time domain
(b) Frequency spectrum of pressure coefficient fluctuations
(c) Pressure fluctuation characteristics in time domain
(d) Frequency spectrum of pressure coefficient fluctuations
Figure 8 describes the frequency spectrum of pressure coefficient fluctuations of monitoring point P4 with different vanes. It can be seen that the pressure coefficient fluctuations of the pump with 9vane diffuser are smaller than other two cases at all working points, which implies that the reasonable increasing of the vane numbers of the diffuser is beneficial to control the pressure fluctuation in the axialflow pumps. Moreover, the pressure coefficient fluctuating becomes strong as the flow discharge decreases rapidly from 1.0 to 0.6 in the pump matched three kinds of vane models, which indicates that the pump has strong exciting force as it is running at low discharge point. However, the pressure coefficient fluctuating also decreases slightly when the flow discharge increases from 1.0 to 1.3 , which is contradiction with our knowledge that the minimum pressure fluctuating is associated with the pump operation around to best efficiency point. So we examine the influence of the flow nonuniformity induced by the suction elbow on the pump circumferential unsteady behavior at operator point. Four monitoring points, P5, P51, P52, and P513, are located on the impeller inlet (z=0.033m) as shown in Figure 9(a). Figures 9(b)–9(g) describe the pressure fluctuations and frequency spectrum of four monitoring point with 7vanes at 0.8 , 1.0 , and 1.3 , respectively. It can be seen that the amplitude of pressure fluctuation exists in circumferential nonuniformity due to the flow nonuniformity induced by the suction elbow. Table 1 presents the coefficient of variance at BPF corresponding to four monitoring points, from which it can be seen that the maximum value of pressure fluctuations are 37.97kPa, 24.67kPa, and 25.35kPa to the axialflow pump with 7 vanes at different operation point, respectively, the mean values are 35.44kPa, 23.42kPa, and 24.63kPa, respectively, and the coefficient of variance is 4.9%, 3.6%, and 4.7%, respectively, which indicates that the circumferential unsteady behavior of pressure fluctuation is more severe due to flow nonuniformity induced by the suction elbow at partial operation. Generally, the pressure fluctuating increases slightly when the flow discharge increases from 1.0 to 1.3 .

(a) 5 vanes
(b) 7 vanes
(c) 9 vanes
(a) Location of monitor points
(b) Pressure fluctuation characteristics in time domain at 0.8Qv
(c) Frequency spectral of pressure fluctuation at 0.8Qv
(d) Pressure fluctuation characteristics in time domain at 1.0Qv
(e) Frequency spectral of pressure fluctuation at 1.0Qv
(f) Pressure fluctuation characteristics in time domain at 1.3Qv
(g) Frequency spectral of pressure fluctuation at 1.3Qv
3. Vibration and Noise Simulation
Unsteady flow exciting forces acting on the axialflow pump give rise to structural vibration and further radiate noise to the environment. In the present study, the interaction process among the fluidstructureacoustic is simulated by coupling way as follows: (1) LES method is used to solve the 3D unsteady flow, which supplies a time series for the pressure fluctuations at the interface between the fluid and wall, while the feedback effects of structural vibration on the fluid are neglected. (2) Finite element method is used to simulate structural vibration induced by the unsteady flow, and the noise field generated by the vibration is solved using boundary element method. The mutual coupling interaction between the vibration and noise field in the fluid is considered using the vibroacoustic coupling model, which supplies the vibration velocities on the outer surface of pump. (3) Noise field radiated to the environment is solved using boundary integral equation method.
3.1. Acoustic Model
The governing equation for acoustic fields generated by the vibration is Helmholtz equation:where is the sound pressure amplitude, the wavenumber, the angular frequency, and the sound speed.
In the present study, (6) is solved using boundary integral equation method, which has been widely used in acoustics. The boundary integral formulation equation for an interior acoustic problem corresponding to (6) iswhere and are the sound pressure and the particle normal velocity on the boundary surface , respectively, mean fluid density, and the Green kernel function,
The leading coefficient is equal to 1 for in the domain and 1/2 for on a smooth boundary, and it is equal to 0 for in the exterior domain.
To solve the Helmholtz integral equation numerically, (7) is first discretized and evaluated for each node on the boundary. This produceswhere and denote global coefficient matrix. For the each node , this produceswhere represents the Kronecker delta function and the shape function.
3.2. Vibration Model
The finite element model of structure vibrations yieldswhere denotes a displacement vector, stiffness matrices, damping matrices, and mass matrices. is the force loading of the acoustic pressure on the structure surface. The symbol denotes fluidstructural coupling matrix, which is given bywhere denotes the couplingsurface element numbers. and represent the structure element shape function and acoustic element shape function, respectively. represents the unit normal vector. represents the flow excitation force, yielding
In the present paper, the mutual interaction of fluidstructure is simulated by oneway weak coupling, in which the wall vibration is negligible.
For coupled vibroacoustic problems, an acoustic and a structural problem must be solved simultaneously to include the mutual coupling interaction between the fluid pressure and the structural deformation. The normal fluid velocity, , must equal the normal structural velocity along the fluidstructure coupling interface, where is the transformation matrix.
The nonreflecting condition is carried out at the inlet and outlet. According to linear timeharmonic acoustic simulation rule, six linear elements per wavelength are required.
3.3. Numerical Results
Full scale axial pump structural vibroacoustics are simulated by LMS Virtual Lab software. Figure 10 shows a full scale structure mesh, which has 0.58 million 4noded tetrahedral elements. The coefficients used are Elasticity modulus E=210GPa, density , and Poisson ratio . Moreover, for validating computed modal, the comparisons between the computed results and experimental results are performed, a detailed description of which can be seen in [13].
Figure 11 shows the vibration acceleration frequency spectrum characteristics for sampled points M1, M2, and M3, shown in Figure 10, when the axialflow pump works at nominal flow rate. These sampled points are located on the inlet and outlet flange and the pump seat, respectively. It can be seen that the structural vibration is dominated by the BPF component, which is in accordance with frequency spectral characteristics of pressure pulsation. The amplitude of vibration acceleration with 7vane diffuser is bigger than other pumps and with 9vane diffuser is small relatively. This trend coincides with the law of exciting force as mentioned.
(a) M1
(b) M2
(c) M3
Figure 12 shows acoustics field directivity distribution of thirtysixth monitoring points, located at 1.15 meter away from the center of the rotor, induced by the vibration of axialflow pump with different vanes corresponding to BPF, from which it can be seen that the noise field directivity distributions are typical dipoles. This is conforming to the fact that only the dynamic surface pressure (dipole source) is loaded and the monopole and quadrupole contributions of fluidacoustic sources are neglected in the coupled simulation.
The sound pressure level () of radiation noise field excited by the pump vibration reaches the maximum value at the pump outlet direction either to the 5vanes or to 7vanes and 9vanes, that is, about 18.3dB, 36.1dB, and 15.6dB, respectively, from which it can be seen that radiation noise field excited by the pump vibration with 9vane diffuser is small relative to other two models for BPF components, which indicated that appropriate guidevane numbers contribute to suppressing pressure fluctuations and vibroacoustics in axialflow pump.
4. Conclusions
This study presented an effect of guidevane numbers on pressure fluctuations and structural vibroacoustics induced by unsteady flow. The vibroacoustic field of the axialflow pump is simulated using coupled vibroacoustic model. Some conclusions as follows:
(1) The dominant frequency of pressure fluctuations is the bladepassing frequency and its harmonic frequency, and the amplitude at the tip clearance is prevailing. The unsteady pressure fluctuating becomes strong as the flow discharge decreases from 1.0 to 0.6 , the circumferential unsteady behavior of which is more severe due to flow nonuniformity induced by the suction elbow at partial operation. Generally, the pressure fluctuating increases slightly when the flow discharge increases from 1.0 to 1.3 . Pressure fluctuations amplitude on the pump with 9vane diffuser is small relative to other two models
(2) The dominant frequency of the vibration acceleration of axialflow pump is also bladepassing frequency, which is consistent with pressure fluctuation frequency spectral characteristics. The vibrating accelerating and radiation sound field on the pump with 9vane diffuser are also slight relatively at BPF, which indicated that appropriate guidevane numbers contribute to suppress pressure fluctuations and vibration in axialflow pump.
Data Availability
The data used to support the findings of this study are available from the corresponding author upon request.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
This work was supported by the National Natural Science Foundation of China (51106099 and 11502146), the Natural Science Foundation of Shanghai (15ZR1429600), and Research Fund of Science and Technology Commission of Shanghai Municipality (13DZ2260900).
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Copyright © 2018 Guoping Li et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.