Computational study of the gas flow through a critical nozzle

Abstract The critical nozzle is defined as a device to measure the mass flow with only the nozzle supply conditions making use of the flow choking phenomenon at the nozzle throat. The discharge coefficient and critical pressure ratio of the gas flow through the critical nozzle are strongly dependent on the Reynolds number, based on the diameter of the nozzle throat and nozzle supply conditions. Recently a critical nozzle with a small diameter has been extensively used to measure mass flow in a variety of industrial fields. For low Reynolds numbers, prediction of the discharge coefficient and critical pressure is very important since the viscous effects near walls significantly affect the mass flow through the critical nozzle, which is associated with working gas consumption and operation conditions of the critical nozzle. In the present study, computational work using the axisymmetric, compressible, Navier-Stokes equations is carried out to predict the discharge coefficient and critical pressure ratio of gas flow through the critical nozzle. In order to investigate the effect of the working gas and turbulence model on the discharge coefficient, several kinds of gases and several turbulence models are employed. The Reynolds number effects are investigated with several nozzles with different throat diameters. The diffuser angle is varied in order to investigate the effects on the discharge coefficient and critical pressure ratio. The computational results are compared with the previous experimental ones. It is known that the standard k-ε turbulence model with the standard wall function gives the best prediction of the discharge coefficient. The discharge coefficient and critical pressure ratio are given by functions of the Reynolds number and boundary layer integral properties. It is also found that the diffuser angle affects the critical pressure ratio.

[1]  B. S. Stratford,et al.  The Calculation of the Discharge Coefficient of Profiled Choked Nozzles and the Optimum Profile for Absolute Air Flow Measurement , 1964, The Journal of the Royal Aeronautical Society.

[2]  Masaki Takamoto,et al.  Relations between the Discharge Coefficients of the Sonic Venturi Nozzle and a Kind of Gases. , 2000 .

[3]  J. Fenn,et al.  Experimental Determination of the Discharge Coefficients for Critical Flow through an Axisymmetric Nozzle , 1978 .

[4]  E. von Lavante,et al.  Unsteady effects in critical nozzles used for flow metering , 2001 .

[5]  Noel Bignell Comparison techniques for small sonic nozzles , 1996 .

[6]  M. Takamoto,et al.  Theoretical discharge coefficient of a critical circular-arc nozzle with laminar boundary layer and its verification by measurements using super-accurate nozzles , 2000 .

[7]  W. H. Heiser,et al.  Compound-Compressible Nozzle Flow , 1967 .

[8]  H. J. Hoge,et al.  Choked flow - A generalization of the concept and some experimental data. , 1965 .

[9]  Masaki Takamoto,et al.  Development of a calibration facility for small mass flow rates of gas and the uncertainty of a sonic venturi transfer standard , 1996 .

[10]  Yong Moon Choi,et al.  Interference effects of three sonic nozzles of different throat diameters in the same meter tube , 1999 .

[11]  Yoshiaki Miyazato,et al.  Shock train and pseudo-shock phenomena in internal gas flows , 1999 .

[12]  Hae-Man Choi,et al.  The evaluation of critical pressure ratios of sonic nozzles at low Reynolds numbers , 2001 .

[13]  Heuy Dong Kim,et al.  Post-Shock Expansion Phenomenon Caused by Normal Shock/Turbulent Boundary Layer Interaction. , 1993 .