Jump to ContentJump to Main Navigation
Show Summary Details
More options …

Open Physics

formerly Central European Journal of Physics

Editor-in-Chief: Seidel, Sally

Managing Editor: Lesna-Szreter, Paulina


IMPACT FACTOR 2018: 1.005

CiteScore 2018: 1.01

SCImago Journal Rank (SJR) 2018: 0.237
Source Normalized Impact per Paper (SNIP) 2018: 0.541

ICV 2018: 147.55

Open Access
Online
ISSN
2391-5471
See all formats and pricing
More options …
Volume 17, Issue 1

Issues

Volume 13 (2015)

Dynamics and Wear Analysis of Hydraulic Turbines in Solid-liquid Two-phase Flow

Liying Wang / Bingyao Li
  • State Key Laboratory of Eco-hydraulics in Northwest Arid Region of China, Xi’an University of Technology, Shanxi, Xi’an, 710048 China
  • Email
  • Other articles by this author:
  • De Gruyter OnlineGoogle Scholar
/ Weiguo Zhao
  • Corresponding author
  • School of Water Conservancy and Hydropower, Hebei University of Engineering, Handan, Hebei, 056021, China
  • Email
  • Other articles by this author:
  • De Gruyter OnlineGoogle Scholar
Published Online: 2019-12-31 | DOI: https://doi.org/10.1515/phys-2019-0082

Abstract

To solve unstable operating and serious wearing of a hydraulic turbine in its overflow parts under solid-liquid two-phase flow, a particle model software and an inhomogeneous model in CFX are used to simulate the hydraulic turbine to understand the wearing of overflow parts and the external characteristics under the solid-liquid two-phase flow. Eleven different conditions at different densities and concentration have been calculated. The simulation results show that the volume distribution of solid particles is larger at the turn of the volute and nose end, resulting in the serious wear in this area. Due to uniform flow at the butterfly edge of volute under solid-liquid two-phase flow, the wear at the entrance of guide vane, the inlet of the blade and the outlet in the shroud is more serious than in other sections. Meanwhile, the collision between the solid phase particles and the overflow components is more intense under solid-liquid two-phase flow in the rotor which can lead to cavitation especially in the outlet and shroud of the blade. In addition, with the increase of density and concentration of solid particles the inlet and outlet pressure difference gradually rises, causing the efficiency loss of the hydraulic turbine.

Keywords: Solid-liquid two-phase flow; Francis turbine; Numerical simulation; Particle model; Inhomogeneous model; Wear

PACS: 88.60.kf; 47.11.-j; 88.60.K

1 Introduction

In recent years, with the rapid development of industry, hydropower, as a clean renewable energy, occupies an increasingly important position. As the core component of a hydropower station, the hydraulic turbine has been paid more attention by researchers and also has encountered many problems during its development. Most rivers in China have a large sediment content, especially in the Yellow River Basin where the annual sediment intake is as high as 1.6 billion tons. This can lead to serious sedimentwear for the hydraulic turbine under solid-liquid two-phase flow. Deep or shallow grooves on the surface will occur when the sediment particles flow through the overflow component, causing certain damage to the overflow parts, and the interruption of the blade will occur in serious cases. Meanwhile, due to the movement of sand particles in the hydraulic turbine, it will bring problems such as performance degradation, vibration, cavitation erosion, and so on, which will seriously affect the stability of turbine [1, 2]. Therefore, it is a critical to study the internal flow of the turbine in the sediment-laden flow and the wear of its overflow component.

For quite a long time, the research on hydraulic machinery mainly concentrates on real experiments, modelling test and numerical calculations. The numerical method is a newly developed way with the development of the computer technology which has high reliability and visualization, and the Computational Fluid Dynamics (CFD) plays an important role in the study of hydraulic machinery internal flow and its dynamic characteristics. In recent years, the research on the operation of water turbines under clean water has been very specific and in-depth [3, 4, 5, 6]. For solid-liquid two-phase flow [7] and wear of hydraulic machinery, the researchers mostly focus on the dynamic characteristics of centrifugal pumps and a lot of experiments have been completed. Zhang Y. et al. [8, 9] studied the influence of the solid phase property on hydraulic transport performance and the distribution of solid particles in the pump channel, then analyzed the characteristics of internal flow field. Wang J. et al. [10, 11] used a CFX particle model to simulate the centrifugal pump in solid-liquid two-phase flow and the simulation results provided a basis for analyzing the wear of the overflowing parts, and then the reliability of particle model was also verified. Huang J. et al. [12] simulated a Francis turbine under a small opening condition by Fluent software and the wear of the turbine was obtained, moreover, the simulation results were consistent with the experimental results of the real turbine.

In the present research, researchers mainly take the mixture model as the main research method. The particle model is also used to study the solid-liquid two-phase flow, but its application to the turbine simulation has rarely been reported [13, 14, 15]. In this paper, the particle model and the inhomogeneous model are used to simulate and analyze the solid-liquid two-phase flow of the HL240 turbine using the ANSYS-CFX fluid analysis software. The wear of solid particles for the flow parts of hydraulic turbines under solid-liquid two-phase flow and the law of sediment flow inside the turbine are analyzed. Meanwhile, the external characteristics of the turbine under the state of solid-liquid two-phase flow are analyzed, which provides an important reference for the abrasion mechanism of the turbine in the solid-liquid two-phase flow.

2 Calculation Control Equations

2.1 Solid-liquid two-phase flow equations

In the calculation of solid-liquid two-phase flow, the governing equations of solid-phase and liquid phase are considered respectively, and the continuous equation for liquid-phase turbulence is

ρft+xjρfufj=Sf(1)

Where ρf is the density of liquid phase, ufj is the velocity component of liquid phase, and xj is Cartesian coordinate.

The continuous equation shows that the mass of the fluid flowing into any section should be the same as the mass of the fluid flowing out of any other section at the same time in a continuous medium with constant density.

The momentum equation is

ρfufjt+ρfufjufixi=pfxi+τfijxi+ρfgi+Ffdi+ufiSfρfufjufi¯xi(2)

The momentum equation indicates that the magnitude of the total external force acting on the object is equal to the change rate of the momentum of the object acting in the direction of the force.

The time-average equations of solid phase are

ρPt+ρPuPixj=SPρPuPj¯xj(3)ρPuPit+ρPuPjuPixj=ρPgi+FPdi+uPiSPxjρPuPjuPi¯+uPjρPuPi¯+uPiρPuPj¯+ρPuPjuPi¯(4)

2.2 Drag force equations

In the simulation, the particle model in the CFX fluid analysis software is used to simulate the flow law of the sediment containing medium in the hydraulic turbine. The Gidaspow model is used for the drag force between the solid and the liquid phases, and the equation is expressed as [16]

Dαβ=34CDdγβραUβUαUβUα(5)

When rc>0.8,

CD=rc1.65max24rcRe1+0.15rc0.687Re0.687,0.44(6)

When rc<0.8,

34CDdγβραUβUα=1501rc2μcrcdp2+741rcρcUcUddp(7)

Where D αβ is the drag force of solid particles in unit volume of continuous phase, CD is the drag coefficient, dP is the mean diameter of solid particles, γβ is the volume fraction of solid particles, Re is the Reynolds number, rC is the continuous phase volume fraction, ρf is the static pressure in the liquid phase, gi is the acceleration of gravity, ρα and ρc are the continuous phase densities, Uβ and Ud are particle velocities, Uα and Uc are the velocities of the continuous phase, and μc is the continuous phase viscosity.

3 Numerical Simulation

3.1 Francis turbine model

The HL240 turbine is chosen as the research object under the 24 opening condition. The design head of this turbine is 45m, the runner diameter is 1m, the unit rotational speed is 72r/min, and the unit flow rate is 1.05m3/s. The full channel model of the turbine including spiral casing, guide vane, runner and draft tube is established using Solidworks. Then according to its different structure, the tetrahedral structure grid and hexahedral unstructured grid are used to divide the model. Theoretically, the result of numerical simulation will be gradually reduced with the increase of mesh number, until it disappears [17]. But considering the relationship between the computing performance and the computational time, the number of grids should be controlled in a certain range. Finally, based on the grid independence, the number of meshes is 4 295 627, the number of nodes is 1 457 503. The 3-D calculation model diagram of Francis turbine full flow path is depicted in Figure 1.

Full channel of flow field model of the Francis turbine
Figure 1

Full channel of flow field model of the Francis turbine

3.2 Numerical calculation

To study the flow and wear of the Francis turbine in solid-liquid two-phase flow, the Ansys flow field analysis software CFX module is adopted. Due to the complexity of the actual problem, it is not easy to realize in the simulation. In order to facilitate the analysis of the flow state of solid particles in the turbine, the following assumptions are made. (1) The liquid phase in the hydraulic turbine medium is an incompressible continuous fluid, the solid phase is discrete term, and the physical property of the two-phase is constant. (2) The particle diameter is homogeneous, the shape is spherical, and the effect of phase change is not considered. (3) The solid-liquid two-phase flow in the turbine is steady flow. (4) The collision loss of solid particles in turbine is not considered.

3.3 Experimental method

To explore the effect of solid phase properties on the dynamic characteristics and internal wear of hydro-turbine under solid-liquid two-phase flow, the following simulation test scheme is developed, and the influence of different solid states in the turbine is obtained through the analysis of different concentrations and densities. The different densities are: the particle concentration is 5% and the diameter is 0.1mm. Six kinds of working conditions including 1.5g/cm3, 2.0g/cm3, 2.3g/cm3, 2.5g/cm3, 2.8g/cm3, 3.0 g/cm3 are simulated. The different concentration: the particle density is 2.5g/cm3 and the diameter is 0.1mm.

4 Simulation results and analysis

In this paper, the particle model in the ANSYS-CFX software is adopted. Firstly, the conditions with 5% particle concentration, 2.5g/cm3 density and 0.1mm diameter is analyzed, emphasizing wear of the over-flow components such as volute, guide vane and blade. Secondly, the influence of particle properties such as concentration and density on the external characteristics of the Francis turbine is analyzed to reveal the complex flow mechanism inside the turbine under solid-liquid two-phase flow.

4.1 Wear analysis

4.1.1 Spiral casing

Figure 2 shows the volume fraction distribution of solid particles when the particle concentration is 5%, the density is 2.5g/cm3 and the diameter is 0.1mm. As can be seen from the diagram, at the entrance of the spiral case to the inlet section, the solid particles do not cause wear to the wall, and the worn parts mainly occur at the turn of the volute with the wear at the nose end of the volute being the most serious. When the water flows through the turning place in solid-liquid two-phase flow, the solid particles accumulate here due to the inertia, abrading the volute wall especially in the volute nose end and this is where the particles reach the highest concentration. Another reason is that the flow velocity and the solid particle velocity at the nose end are higher than other parts which may increase the silt abrasion in this area.

Volume fraction distribution of solid particles at the wall
Figure 2

Volume fraction distribution of solid particles at the wall

4.1.2 Guide vane

Figure 3 and Figure 4 show the distribution of the particle volume fraction of the guide vane and the velocity streamline distribution of solid particles at different blade span respectively. It can be seen from Figure 3 that the distribution of the volume fraction at the inlet of active guide vane is larger so the wear situation is more serious. The distribution shows the trend of increasing from middle to both sides and the volume fraction distribution is the largest in the hub and shroud. Meanwhile, it can be observed from Figure 4 that the flow state of solid particles is more uneven than that in the middle of the guide vanes near the hub and shroud, which leads to serious abrasion here. This is because when the water flows through the volute into the guide vanes, the flow state of the volute is uneven near the butterfly. The solid particles at the entrance of the guide vane have a serious impact and as the solid particles have a large volume fraction here this produces a lot of wear and tear to the guide vane at inlet. At the same time, due to the viscous flow, the liquid phase flows along the wall of the active guide vane, while the solid particles do not generate some wear for the active guide vane pressure surface and the suction surface. This result is also consistent with the one obtained in the literature [18, 19].

Volume fraction distribution of solid particles in guide
Figure 3

Volume fraction distribution of solid particles in guide

Flow velocity distribution of solid particles at different blade spans direction in guide vane
Figure 4

Flow velocity distribution of solid particles at different blade spans direction in guide vane

In the study on the wear condition of the runner blades, the analysis is carried out with a solid particle concentration of 5%, density of 2.5g/cm3 and a diameter of 0.1mm. Figure 5 shows the distribution of the solid particle volume fraction at different sections of the runner blades. It can be seen from the figure, whether close to the hub or the shroud, the blade inlet volume fraction is relatively large and the impact of solid particles is also serious here, thus causing more abrasion for the blade. However, in the suction surface of the blade, the volume fraction distribution of solid particles is low, therefore there is no wear on the suction surface of the blade. The solid particles in the pressure surface of the volume fraction distribution grow quickly from the hub to the shroud with the migration trend towards the downward ring of blade, especially close to the shroud. The effect of solid particles on the blade is largest, thus resulting in the most serious wear.

Volume fraction distribution of solid particles at different blade span directions
Figure 5

Volume fraction distribution of solid particles at different blade span directions

To further analyze the wear effect of different particle densities on the runner blades, Figure 6 shows the solid particle volume fraction distribution of different particle densities at the same section The analysis shows that with the increase of particle density the volume fraction of solid particles at the inlet and outlet of blade increases, especially at the outlet where the volume fraction increases to a maximum. This is because when the solid-liquid two-phase flow flows through the high-speed rotating runner, under the action of inertia and centrifugal force, the solid particles have a serious impact on the inlet and pressure surface of the blade, and as the high-speed water scours the blade near the shroud exit, the volume fraction of the solid particles is the largest. The results are consistent with the abrasion of the turbine blades in the actual hydropower station [20]. During the solid-liquid two-phase flow in the runner, the collision of solid-phase particles and over-flow components is more intense, which is very easy to cause cavitation, so the abrasion for the over current components is much more than the loss caused by them. Therefore, in the design of turbine runner, the abrasion resistance of the blade under the condition of solid-liquid two-phase flow should be considered such as rational designing the blade form and making the flow distribution of solid-liquid two-phase flow in the runner more reasonable. Only then can the service life of the turbine be increased and its operating efficiency be improved.

Volume fraction distribution of solid phase particles at the same blade span (span=0.5)
Figure 6

Volume fraction distribution of solid phase particles at the same blade span (span=0.5)

4.2 Analysis of external characteristics

Figure 7 shows the variation curves of the pressure difference of the mixed-flow turbine at different densities and concentrations. As shown in Figure 7(a), with the increase of density, the pressure difference of the import and export increases and the degree of change is also larger. Figure 7(b) shows that the change of pressure difference is less obvious than the increase of concentration but the overall shows increased tendency. According to the two-phase flow conveying mechanism under the same conditions, the higher the gravity of the solid phase property is, the greater the energy requiring to maintain its suspension is and the greater the efficiency loss is. Under the action of inertia and centrifugal force, the flow of particles in the flow of water will inevitably lead to the loss of local head and the increase of head loss along the path, thus reducing the efficiency of the turbine.

Variation of pressure difference of two phase flow at inlet and outlet in solid-liquid two-phase flow
Figure 7

Variation of pressure difference of two phase flow at inlet and outlet in solid-liquid two-phase flow

5 Conclusions

In this paper, the fluid analysis software CFX coupled with the two-order upwind scheme discrete difference equation based on the SIMPLEC method, the particle model and heterogeneous model are used to analyse the HL240 turbine in solid-liquid two-phase flow. The wear and external characteristics of the flow parts of the Francis turbine are investigated, and some flow laws of the mixed-flow turbine are obtained. It provides some reference value for the design of turbine and the improvement of service life. The main conclusions are summarized as follows:

  1. The particle model can be used to simulate the Francis turbine in solid-liquid two-phase flow, which can reveal its internal flow state and analyze the wear of overcurrent components, and the results are consistent with the experimental results. From the analysis of the external characteristic results, when the density and concentration of solid particles increase, the pressure difference at the inlet and outlet increases, which leads to the increase of the efficiency loss of the turbine.

  2. Under solid-liquid two-phase flow, the volume fraction of solid particles at the turn of the volute and the nose end is large and the wear of the wall is significant. This seriously affects the symmetrical distribution of the flow in the volute, and brings a certain influence to the safe and stable operation of the runner.

  3. In the high-speed rotating runner, due to the inertia and centrifugal force, solid particles mainly concentrate on the blade inlet and shroud exit and the wear here also increases. Meanwhile, due to the violent collision between the solid particles and the wall surface, it is easy to induce cavitation in the runner which increases the head loss in the runner, and the unsteady flow will then affect the flow in the draft tube.

In the future research, the optimization design of the guide vane based on metaheuristic methods [21, 22] and analysis of solid-liquid two-phase flow will be investigated. Moreover, the cavitation erosion of turbine in solid-liquid two-phase flow will be another study [23]. These studies will be of great importance to the normal and high-efficiency running of turbine.

Acknowledgement

This work is supported in part by the Natural Science Foundation of Hebei Province of China (Grant: E2018402092, F2017402142), National Natural Science Foundation of China (Grant: 11972144), and Scientific Research Key Project of University of Hebei Province of China (Grant: ZD2017017).

References

  • [1]

    Tang X., Yu X., Ren S., Solid liquid two phase fluid dynamics and its application in hydraulic machinery, The Yellow River water conservancy Publishing Press, Zhengzhou, 2006. Google Scholar

  • [2]

    Pyskunovs S.O., Maksimyk Yu.V., Valer V.V., Finite Element Analysis of Influence of Non-homogenous Temperature Field on Designed Lifetime of Spatial Structural Elements under Creep Conditions, Appl. Math. Nonlinear Sci., 2016, 1(1), 253-262. CrossrefGoogle Scholar

  • [3]

    Wang S., Dynamic characteristic analysis and synthetical optimization of Francis turbine’s runner, PhD thesis, Institute of Mechanical Science, Beijing, 2003. Google Scholar

  • [4]

    Trivedi C., Cervantes M.J., Gandhi K., Investigation of a High Head Francis Turbine at Runaway Operating Conditions, Energies, 2016, 149(9), 1-22. Web of ScienceGoogle Scholar

  • [5]

    Li H., Chen D., Zhang H., Wu C. Wang X., Hamiltonian analysis of a hydro-energy generation system in the transient of sudden load increasing, Appl. Energy, 2017, 185, 244-253. Web of ScienceCrossrefGoogle Scholar

  • [6]

    Binjuan Z., Shouqi Y. Houlin L., Zhongfu H., Mingao T., Simulation of solid-liquid two-phase turbulent flow in double channel pump based on Mixture model, Trans. CSAE, 2008, 24(1), 7-12. Google Scholar

  • [7]

    Vajravelu K., Sreenadh S., Saravana R., Influence of velocity slip and temperature jump conditions on the peristaltic flow of a Jeffrey fluid in contact with a Newtonian fluid, Appl. Math. Nonlinear Sci., 2017, 2(2), 429-442. CrossrefGoogle Scholar

  • [8]

    Zhang Y., Li Y., Cui B., Zhu Z. Dou H., Numerical simulation and analysis of solid liquid two-phase flow in centrifugal pump, Chin. J. Mech. Eng., 2013, 26(1), 53-60. CrossrefWeb of ScienceGoogle Scholar

  • [9]

    Zhang Y., Transient internal flow and external characteristics of the start-up process of a centrifugal pump, PhD thesis, Zhejiang University, Zhejiang, 2016. Google Scholar

  • [10]

    Wang J., Jiang W., Kong F., Qu X., Su X., Numerical simulation of solid-liquid two-phase turbulent flow in centrifugal pump based on Particle model, J. Drain. Irrig. Mech. Eng., 2013, 31(10), 846-850. Google Scholar

  • [11]

    Wang J., Jiang W., Kong F., Su X. Chen H., Numerical simulation of Solid-liquid two-phase turbulent flow and wear characteristics of centrifugal pump, Trans. Chin. Soc. Agric. Mach., 2013, 44(11), 53-60. Google Scholar

  • [12]

    Huang J., Zhang L., Yao J. Long L., Numerical simulation of two-phase turbulent flow in Francis turbine passage on sediment erosion, J. Drain. Irrig. Mech. Eng., 2016, 34(2), 145-150. Google Scholar

  • [13]

    Hall N., Elenany M., Zhu D.Z., Rajaratnam N., Experimental study of sand and slurry jets in water, J. Hydraul. Eng., 2010, 136(10), 727-738. Web of ScienceCrossrefGoogle Scholar

  • [14]

    Azimi A.H., Zhu D.Z. Nallamuthu R., Computational investigation of vertical slurry jets in water, Int. J. Multiphase Flow, 2012, 47, 94-114. Web of ScienceCrossrefGoogle Scholar

  • [15]

    Azimi A.H., Zhu D.Z., Nallamuthu R., Experimental study of sand jet front in water, Int. J. Multiphase Flow, 2012, 40, 19-37. Web of ScienceCrossrefGoogle Scholar

  • [16]

    Ansys, ANSYS CFX-Solver Modeling Guide Release 13.0. New York: Ansys Inc, 2010. Google Scholar

  • [17]

    Zhou L., Shi W., Lu W., Li H., Pei B.,. Analysis on pressure fluctuation of unsteady flow in deep-well centrifugal pump, Trans. Chin. Soc. Agric. Mach., 2011, 27(10), 44-49. Google Scholar

  • [18]

    Guangjie P., Zhengwei W., Yexiang X. Yongyao L., Abrasion predictions for Francis turbines based on liquid-solid two phase fluid simulations, Eng. Failure Anal., 2013, 33, 327- 335. CrossrefWeb of ScienceGoogle Scholar

  • [19]

    Noon A.A., Kim M.H., Erosion wear on Francis turbine components due to sediment flow, Wear, 2017, 378-379, 126-135. Web of ScienceGoogle Scholar

  • [20]

    Thapa B.S., Thapa B., Dahlhaug O.G., Empirical modelling of sediment erosion in Francis turbines, Energy, 2012, 41, 386-391. CrossrefWeb of ScienceGoogle Scholar

  • [21]

    Zhao W.,Wang L., Zhang Z., A novel atom search optimization for dispersion coefficient estimation in groundwater, Future Gener. Comput. Syst., 2019, 91, 601-610. CrossrefGoogle Scholar

  • [22]

    Zhao W., Wang L., An Effective Bacterial Foraging Optimizer for Global Optimization, Inf. Sci., 2016, 329, 719-735. CrossrefWeb of ScienceGoogle Scholar

  • [23]

    Celebioglu K., Altintas B., Aradag S., Tascioglu Y., Numerical research of cavitation on Francis turbine runners, Int. J. Hydrogen Energy, 2017, 42(28), 17771-17781. CrossrefWeb of ScienceGoogle Scholar

About the article

Received: 2019-06-12

Accepted: 2019-07-26

Published Online: 2019-12-31


Citation Information: Open Physics, Volume 17, Issue 1, Pages 790–796, ISSN (Online) 2391-5471, DOI: https://doi.org/10.1515/phys-2019-0082.

Export Citation

© 2019 L. Wang et al., published by De Gruyter. This work is licensed under the Creative Commons Attribution 4.0 Public License. BY 4.0

Comments (0)

Please log in or register to comment.
Log in