Wall-resolved Large Eddy Simulation of a flow through a square-edged orifice in a round pipe at Re = 25,000

Abstract The orifice plate is a pressure differential device frequently used for flow measurements in pipes across different industries. The present study demonstrates the accuracy obtainable using a wall-resolved Large Eddy Simulation (LES) approach to predict the velocity, the Reynolds stresses, the pressure loss and the discharge coefficient for a flow through a square-edged orifice in a round pipe at a Reynolds number of 25,000. The ratio of the orifice diameter to the pipe diameter is β  = 0.62, and the ratio of the orifice thickness to the pipe diameter is 0.11. The mesh is sized using refinement criteria at the wall and preliminary RANS results to ensure that the solution is resolved beyond an estimated Taylor micro-scale. The inlet condition is simulated using a recycling method, and the LES is run with a dynamic Smagorinsky sub-grid scale (SGS) model. The sensitivity to the SGS model and to the pressure–velocity coupling is shown to be small in the present study. The LES is compared with the available experimental data and ISO 5167-2. In general, the LES shows good agreement with the velocity from the experimental data. The profiles of the Reynolds stresses are similar, but an offset is observed in the diagonal stresses. The pressure loss and discharge coefficients are shown to be in very good agreement with the predictions of ISO 5167-2. Therefore, the wall-resolved LES is shown to be highly accurate in simulating the flow across a square-edged orifice.

[1]  Sandy Chang,et al.  Local mass transfer measurements for corals and other complex geometries using gypsum dissolution , 2013 .

[2]  D. Thomson,et al.  Spectrum estimation and harmonic analysis , 1982, Proceedings of the IEEE.

[3]  D. Lilly,et al.  A proposed modification of the Germano subgrid‐scale closure method , 1992 .

[4]  E. Lamballais Direct numerical simulation of a turbulent flow in a rotating channel with a sudden expansion , 2014, Journal of Fluid Mechanics.

[5]  P. Sagaut,et al.  Large eddy simulation of the flow around single and two side-by-side cylinders at subcritical Reynolds numbers , 2011 .

[6]  P. Moin,et al.  A dynamic subgrid‐scale eddy viscosity model , 1990 .

[7]  Helge I. Andersson,et al.  Numerical aspects of flow computation through orifices , 1997 .

[8]  S. Benhamadouche,et al.  A synthetic-eddy-method for generating inflow conditions for large-eddy simulations , 2006 .

[9]  Dominique Laurence,et al.  A LINEARISED TURBULENT PRODUCTION IN THE k-ε MODEL FOR ENGINEERING APPLICATIONS , 2002 .

[10]  P. R. Voke Subgrid-scale modelling at low mesh reynolds number , 1996 .

[11]  S. Shaaban,et al.  Optimization of orifice meter's energy consumption , 2014 .

[12]  Jyeshtharaj B. Joshi,et al.  Analysis of flow through an orifice meter: CFD simulation , 2012 .

[13]  Y. Tsuji,et al.  Particle image velocimetry measurements of flow field behind a circular square-edged orifice in a round pipe , 2013, Experiments in Fluids.

[14]  F. Menter Two-equation eddy-viscosity turbulence models for engineering applications , 1994 .

[15]  F. Archambeau,et al.  Code Saturne: A Finite Volume Code for the computation of turbulent incompressible flows - Industrial Applications , 2004 .

[16]  C. Meneveau,et al.  The dynamic Smagorinsky model and scale-dependent coefficients in the viscous range of turbulence , 1997 .

[17]  Pierre Sagaut,et al.  Flow over a flat plate with uniform inlet and incident coherent gusts , 2013, Journal of Fluid Mechanics.

[18]  C. Moulinec,et al.  Optimizing Code_Saturne computations on Petascale systems , 2011 .

[19]  Caskey,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS I . THE BASIC EXPERIMENT , 1962 .

[20]  O. G. Martynenko,et al.  Handbook of hydraulic resistance , 1986 .