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1.
Visualisation and Large Eddy Simulations (LES) of cavitation inside the apparatus previously developed by Franc (2011) for surface erosion acceleration tests and material response monitoring are presented. The experimental flow configuration is a steady-state closed loop flow circuit where pressurised water, flowing through a cylindrical feed nozzle, is forced to turn 90° and then, move radially between two flat plates towards the exit of the device. High speed images show that cavitation is forming at the round exit of the feed nozzle. The cavitation cloud then grows in the radial direction until it reaches a maximum distance where it collapses. Due to the complexity of the flow field, direct observation of the flow structures was not possible, however vortex shedding is inferred from relevant simulations performed for the same conditions. Despite the axisymmetric geometry utilized, instantaneous pictures of cavitation indicate variations in the circumferential direction. Image post-processing has been used to characterize in more detail the phenomenon. In particular, the mean cavitation appearance and the cavity length have been estimated, showing good correlation with the erosion zone. This also coincides with the locations of the maximum values of the standard deviation of cavitation presence. The dominant frequency of the ‘large-scale’ cavitation clouds has been estimated through FFT. Cloud collapse frequencies vary almost linearly between 200 and 2000 Hz as function of the cavitation number and the downstream pressure. It seems that the increase of the Reynolds number leads to a reduction of the collapse frequency; it is believed that this effect is due to the agglomeration of vortex cavities, which causes a decrease of the apparent frequency. The results presented here can be utilized for validation of relevant cavitation erosion models which are currently under development. 相似文献
2.
A level set method of non-uniform grids is used to simulate the whole evolution of a cavitation bubble, including its growth,
collapse and rebound near a rigid wall. Single-phase Navier–Stokes equation in the liquid region is solved by MAC projection
algorithm combined with second-order ENO scheme for the advection terms. The moving interface is captured by the level set
function, and the interface velocity is resolved by “one-side” velocity extension from the liquid region to the bubble region,
complementing the second-order weighted least squares method across the interface and projection inside bubble. The use of
non-uniform grid overcomes the difficulty caused by the large computational domain and very small bubble size. The computation
is very stable without suffering from large flow-field gradients, and the results are in good agreements with other studies.
The bubble interface kinematics, dynamics and its effect on the wall are highlighted, which shows that the code can effectively
capture the “shock wave”-like pressure and velocity at jet impact, toroidal bubble, and complicated pressure structure with
peak, plateau and valley in the later stage of bubble oscillating.
The project supported by the National Natural Science Foundation of China (10272032 and 10672043).
The English text was polished by Keren Wang. 相似文献
3.
Ajmal Shah Imran Rafiq Chughtai Mansoor Hameed Inayat 《International Journal of Multiphase Flow》2011
Steam jet pump is the best choice for pumping radioactive and hazardous liquids because it has no moving parts and so no maintenance. However, the physics involved is highly complicated because of the mass, momentum and energy transfer between the phases involved. In this study the characteristics of SJP are studied both experimentally and numerically to pump water using saturated steam. In the experimental study the static pressure, temperature along the length of the steam jet pump and the steam and water flow rates are recorded. The three dimensional numerical study is carried out using the Eulerian two-phase flow model of Fluent 6.3 software and the direct-contact condensation model developed previously. The experimental and CFD results, of axial static pressure and temperature, match closely with each other. The mass ratio and suction lift are calculated from experimental data and it is observed that the mass ratio varies from 10 to 62 and the maximum value of suction lift is 2.12 m under the conditions of the experiment. 相似文献
4.
Shu-Hao Chuang 《国际流体数值方法杂志》1989,9(11):1413-1426
Two-dimensional normal impinging jet flowfields, with or without an upper plate, were analysed by employing an implicit bidiagonal numerical method developed by Lavante and Thompkins Jr. The Jones–Launder K–? two-equation turbulent model was employed to study the turbulent effects of the impinging jet flowfield. The upper plate surface pressure, the ground plane pressure and other physical parameters of the momentum flowfield were calculated at various jet exit height and jet inlet Reynolds numbers. These results were compared with those of Beam and Warming's numerical method, Hsiao and Chuang, and others, along with experimental data. The potential core length of the impinging jet without an upper plate is longer than that of the free jet because of the effects of the ground plane, while the potential core length of the impinging jet with an upper plate is shorter than that of the free jet because of the effects of the upper plate. This phenomenon in the present analysis provides a fundamental numerical study of an impinging jet and a basis for further analysis of impinging jet flowfields on a variable angle plate. 相似文献
5.
A jet and vortices have been observed when a plane shock wave reflects from a concave body in a shock tube. If the cavity
is deep enough then two reflected shocks appear near its edges. Air, carbon tetrafluoride (CF) and dichlorodifluoromethane (CClF) were chosen as test gases. The flow was visualized with the aid of a conventional shadow technique. Pressure measurements
at the body surface were also obtained. Numerical studies have been conducted using a two-dimensional inviscid model. There
is a good qualitative agreement between the experimental and numerical results.
Received 8 February 1996 / Accepted 30 June 1997 相似文献
6.
With an ever increasing demand for more effective heat sinks, liquid based electronic cooling has become a new prospect in the field. The present study introduces an electrohydrodynamic (EHD) pump with a simple design for dielectric liquids which have potential applications for electronic cooling. The pump consists of an eccentrically sandwiched wire electrode placed at the horizontal centerline between two parallel flat-plate electrodes. The EHD flow of dielectric liquid induced by the space charge generated due to the Onsager effect was obtained by the numerical solution of the Poisson–Nernst–Planck equations for ion transport and the Navier–Stokes equations for fluid flow. Good agreement obtained in the comparison of the numerical and the experimental results of velocity for the centrally sandwiched wire electrode case confirmed the validity of the numerical results. For a fixed voltage, the pump flow rate depends on the eccentricity of the wire electrode with respect to the plate electrodes and also with the electrode dimensions. By using the Taguchi method an optimum design for the EHD pump is obtained considering the wire electrode diameter, the flat plate electrode length and the eccentricity (the horizontal distance between the centers of wire and flat-plate electrodes) as the design parameters for fixed channel dimensions. 相似文献
7.
The numerical analysis of plane and axially symmetric jet flows of an incompressible inviscid fluid is treated. A new formulation of the variational inequality type is developed from the variational principle associated with jet problems. A successive approximation method is formulated by the combined use of variational inequality and the finite element method. Numerical examples based on the iterative method are presented. The results obtained agree well with those by other methods. 相似文献
8.
The objective of this work is to simulate and analyze the formations of three-dimensional tip leakage vortex (TLV) cavitation cloud and the periodic collapse of TLV-induced suction-side-perpendicular cavitating vortice (SSPCV). Firstly, the improved SST k–ω turbulence model and the homogeneous cavitation model were validated by comparing the simulation result with the experiment of unsteady cavitation shedding flow around the NACA66-mod hydrofoil, and then the unsteady TLV cloud cavitation and unstable SSPCV in an axial flow pump were predicted using the improved numerical method. The predicted three-dimensional cavitation structures of TLV and SSPCV as well as the collapsing features show a good qualitative agreement with the high speed photography results. Numerical results show that the TLV cavitation cloud in the axial flow pump mainly includes tip clearance cavitation, shear layer cavitation, and TLV cavitation. The unsteady TLV cavitation cloud occurs near the blade trailing edge (TE) where the shapes of sheet cavitation and TLV cavitation fluctuate. The inception of SSPCV is attributed to the tail of the shedding cavitation cloud originally attached on the suction side (SS) surface of blade, and the entrainment affect of the TLV and the influence of the tip leakage flow at the tailing edge contribute to the orientation and development of the SSPCV. The existence of SSPCV was evidently approved to be a universal phenomenon in axial flow pumps. At the part-load flow rate condition, the SSPCV may trigger cavitation instability and suppress the tip cavitation in the neighboring blade. The cavitation cloud on the SS surface of the neighboring blade grows massively, accompanying with a new SSPCV in the neighboring flow passage, and this SSPCV collapses in a relatively short time. 相似文献
9.
This paper presents an extension of the local second gradient model to multiphasic materials (solids particles, air, water) and including the cavitation phenomenon. This new development was made in order to model the response of saturated dilatant materials under deviatoric stress and undrained conditions and possibly, in future, the behavior of unsaturated soils. Some experiments have showed the significance of cavitation for the hydromechanical response of materials. However, to date and as far as we are aware, no attempt was made to implement the cavitation as a phase change mechanism with a control of pore pressure. The first part of the results section explores the effects of permeability, dilation angle and loading rate on the stability of shear bands during a localization event. The reasons underlying the band instability are discussed in detail, which helps defining the conditions required to maintain stability and investigating the effects of cavitation without parasite effect of materials parameters or loading rate. The model showed that, if a uniform response is obtained, cavitation triggers localization. However, in case of a localized solution, cavitation follows the formation of the shear band, with the two events being quite distinct. 相似文献
10.
The compressible flows of plane free jets and jets of the intake-stroke of a rectangular piston-engine model are investigated by numerical simulations. The observed vortical structures appear to be the well-known coherent structures of turbulent shear layers. The simulated structures are compared to experimental data by means of density fields and turbulent statistics taken from different authors. The computed flow depends on physical as well as on numerical parameters. The good agreement with the experimental data is obtained by direct simulation without any turbulence model. 相似文献
11.
This paper reports on the simulation of the near-nozzle region of an isothermal Mach 0.6 jet at a Reynolds number of 100,000
exhausting from a round nozzle geometry. The flow inside the nozzle and the free jet outside the nozzle are computed simultaneously
by a high-order accurate, multi-block, large eddy simulation (LES) code with overset grid capability. The total number of
grid points at which the governing equations are solved is about 50 million. The main emphasis of the simulation is to capture
the high frequency noise generation that takes place in the shear layers of the jet within the first few diameters downstream
of the nozzle exit. Although we have attempted to generate fully turbulent boundary layers inside the nozzle by means of a
special turbulent inflow generation procedure, an analysis of the simulation results supports the fact that the state of the
nozzle exit boundary layer should be characterized as transitional rather than fully turbulent. This is believed to be most
likely due to imperfections in the inflow generation method. Details of the computational methodology are presented together
with an analysis of the simulation results. A comparison of the far field noise spectrum in the sideline direction with experimental
data at similar flow conditions is also carried out. Additional noise generation due to vortex pairing in the region immediately
downstream of the nozzle exit is also observed. In a second simulation, the effect of the nozzle exit boundary layer thickness
on the vortex pairing Strouhal frequency (based on nozzle diameter) and its harmonics is demonstrated. The limitations and
deficiencies of the present study are identified and discussed. We hope that the lessons learned in this study will help guide
future research activities towards resolving the pending issues identified in this work.
Presented as AIAA Paper 2006-2499 at 12th AIAA/CEAS Aeroacoustics Conference, 8–10 May 2006, Cambridge, MA, USA. 相似文献
Presented as AIAA Paper 2006-2499 at 12th AIAA/CEAS Aeroacoustics Conference, 8–10 May 2006, Cambridge, MA, USA. 相似文献
12.
Serrated jet nozzles are considered to be an efficient and practical passive control approach for jet noise. However, some fundamental mechanisms of serration effects on jet noise are not fully understood, especially in terms of the sound source. In this paper, a high-fidelity simulation framework using large-eddy simulation (LES) is demonstrated to predict near-field turbulence and far-field acoustics from an ultra-high-bypass-ratio engine with round and serrated nozzles. Far-field sound is predicted using Ffowcs Willams–Hawkings (FWH) integration. The results show that the serrated nozzle increases mixing near the nozzle and hence the turbulence decay rate, reducing the turbulence level downstream. The serrations shift the energy from the low frequencies to the high frequencies and decrease overall sound pressure levels by about 3 dB over the low-frequency range. Sound sources are analysed based on fourth-order space–time correlations. There are six major source components (, , , , , and ) inside the jet shear layers. The serrations are able to reduce the amplitude of these source terms, causing them to decay rapidly to a level below the round nozzle jet within 2D downstream of the nozzle. 相似文献
13.
E. Bollina 《International Journal of Heat and Fluid Flow》1984,5(2):93-100
A modified version of the standard axial piston pump, normally used with fuels, has been tested with organic fluids R11 and R113. Head-flow characteristics, volumetric and global efficiency, and npsh curves, have been determined at different speeds and fluid temperatures and the results compared with those obtained with kerosene. Pump efficiencies remain satisfactory with high density, very low viscosity and high vapour pressure fluids. In the absence of cavitation, pump performance seems to be a function of kinematic viscosity, while the npsh curves appear to be a complex function of density, viscosity and vapour pressure 相似文献
14.
Ezddin Ali Farag Hutli Milos S. Nedeljkovic Nenad A. Radovic 《Archive of Applied Mechanics (Ingenieur Archiv)》2008,78(5):329-341
Experimental setup with a submerged cavitating jet has been used for the study of influences of material, exposure time and
working fluid temperature on the erosion process. Each of the parameters has been varied separately, and the results of erosion
are analyzed in detail. Additionally, comparison of experiments with nitrated and non-nitrated material has been made in order
to study the enhancement (mostly reflected as the prolonged incubation time) of erosion resistance achieved by nitrating the
specimen surface. 相似文献
15.
16.
《应用数学和力学(英文版)》2017,(12)
The turbulent properties of the fiber suspension in a turbulent round jet are numerically simulated and visualized, and some of the results are compared with the experimental data. The effects of the Reynolds number, fiber volume fraction, and aspect ratio are analyzed. The results show that the fiber injection in the flow has a delay effect on the streamwise velocity decay along the jet axis, and such an effect becomes more obvious with the increases in the fiber volume fraction and aspect ratio and the decrease in the Reynolds number. The flow with fibers shows an increase in the streamwise velocity along the radial direction, and the increase magnitude is directly proportional to the fiber volume fraction and aspect ratio and inversely proportional to the Reynolds number. The presence of fibers makes the turbulent kinetic energy and Reynolds stress increase, and the extent increases with the fiber volume fraction, Reynolds number, and fiber aspect ratio. 相似文献
17.
18.
Unsteady CFD simulations of a pump in part load conditions using scale-adaptive simulation 总被引:4,自引:0,他引:4
The scope of this work is to demonstrate the applicability of an eddy resolving turbulence model in a turbomachinery configuration. The model combines the Large Eddy Simulation (LES) and the Reynolds Averaged Navier Stokes (RANS) approach. The point of interest of the present investigation is the unsteady rotating stall phenomenon occurring at low part load conditions. Since RANS turbulence models often fail to predict separation correctly, a LES like model is expected to give superior results. In this investigation the scale-adaptive simulation (SAS) model is used. This model avoids the grid dependence appearing in the Detached Eddy Simulation (DES) modelling strategy. The simulations are validated with transient measurement data. The present results demonstrate, that both models are able to predict the major stall frequency at part load. Results are similar for URANS and SAS, with advantages in predicting minor stall frequencies for the turbulence resolving model. 相似文献
19.
A. S. Bansode Siddharth Patel T. Rajesh Kumar B. Muralidhar T. Sundararajan Sarit Kumar Das 《Heat and Mass Transfer》2007,43(10):1037-1047
A 3D numerical study was carried out to analyze flow, heat and mass transfer first in a single half-cell cathode channel of
proton exchange membrane (PEM) fuel cell. From practical point of view, it is necessary to put the appropriate number of cells
in a stack. Hence, the above study on a single half-cell is extended to a stack of channels. Due to stacking, the assumption
of uniform flow distribution would no longer hold true. Therefore, the channel flow-maldistribution is considered. The water
formed at the active surface due to the electrochemical reaction diffuses through the porous layer and eventually enters the
gas flow duct. The higher gas velocities in the duct result in faster water vapour removal which leads to a lower value of
water vapour into the duct and hence a lower Nusselt number. 相似文献
20.
液压泵噪声是液压系统的主要噪声源,针对轴向柱塞泵的流致振动噪声,提出一种改善泵配流特性的设计方案。首先,根据柱塞泵的工作原理对柱塞腔压力特性和泵出口流量特性准确建模并求解。通过分析压力冲击和流量脉动对错配角(φ0)的响应,得φ0=4°为佳。利用一种多目标遗传算法(NSGA-Ⅱ),以减小压力超调量和流量脉动率为目标,对三角槽结构进行了优化;并获得该多目标优化问题的Pareto最优解集,通过对最优解集的分析知,深度角θ1=16°且宽度角θ2=85°时较为理想。最后,为了验证模型的正确性,建立流体域计算流体动力学(CFD)模型,对比两种模型计算结果发现吻合较好,能够相互验证。利用CFD分析结果可视化的特点,从柱塞泵流场的角度,进一步分析了泵压力冲击以及流量脉动产生的原因。 相似文献