Hostname: page-component-76fb5796d-9pm4c Total loading time: 0 Render date: 2024-04-30T05:47:25.338Z Has data issue: false hasContentIssue false

The Calculation of the Discharge Coefficient of Profiled Choked Nozzles and the Optimum Profile for Absolute Air Flow Measurement

Published online by Cambridge University Press:  04 July 2016

B. S. Stratford*
Affiliation:
Formerly National Gas Turbine Establishment, Pyestock, now Rolls-Royce Ltd.

Summary

A choked nozzle with an appropriate wall contour has adischarge coefficient, CD, so close to unity that a theoretical calculation of (I—CD) would allow the nozzle to be used as an absolute meter for air flow. The high discharge coefficient results basically from the fact that ∂(ρv)∂p=0 at M=1.

Simplified calculations yield formulae for the boundary layer displacement thickness and for the flow reduction resulting from the variation in static pressure across the throat. The optimum profile for the wall at the throat of an absolute meter is suggested to be a circular arc of radius of curvature equal to about twice the throat diameter. For such a meter the theoretical discharge coefficient is found to be within ¼ per cent of 0·995 over a wide range of Reynolds numbers.

The uncertainty in the discharge coefficient for a steady flow at Reynolds numbers of 106 and over appears to be less than ±0·15 per cent, both when the boundary layer is known to be entirely turbulent and when it is known to be entirely laminar. When the state of the boundary layer is not known the corresponding figure appears to be ±0·25 per cent. Experimental information might therefore be helpful on transition—under the appropriate conditions of flow unsteadiness and rig vibration. Available experimental results with known boundary layers tend to confirm the theoretical discharge coefficients down to a Reynolds number of 0·4x106.

A pressure ratio of about 1·1/1 or less would probably be sufficient to establish fully supersonic flow if the nozzle were followed by a suitable diffuser.

Type
Research Article
Copyright
Copyright © Royal Aeronautical Society 1964

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

1.Johnston, I. H. and Dransfield, D. C. The Test Performance of Highly Loaded Turbine Stages Designed for High Pressure Ratio. ARC R & M 3242, 1959.Google Scholar
2.Arnberg, B. T.Review of Critical Flow Meters for Gas Flow Measurements. Trans. ASME, Paper No. 61-WA-181, 1961; Journal of Basic Engineering, Vol. 84, Series D, No. 4, pp. 447460, 1962.Google Scholar
3.Stratford, B. S. and Ascough, J. C. A Recent Attempt at Accurate Airflow Measurement by Pitot-Static Traverse. Proceedings NEL Symposium on Flow Measurement in Closed Conduits, Paper A-6 1960; HMSO, 1962.Google Scholar
4.Ascough, J. C. The Development of a Nozzle for Absolute Airflow Measurement by Pitot-Static Traverse. ARC Tech Note No. 25 030, 1963. To be published as an R. & M.Google Scholar
5.Oswatitsch, KL. and Rothstein, W. Das Stromungsfeld in einer Laval-Diise Jb. dtsch, Lufo 1, pp. 91-102, 1942; Transl. as NACA TM 1215, 1949.Google Scholar
6.Rao, G. V. R.Evaluation of Conical Nozzle Thrust Coefficient. ARS Journal “Tech. comment”, pp. 606-7, Vol. 29, No. 8, 1959.Google Scholar
7.Sauer, R. General Characteristics of the Flow Through Nozzles at Near Critical Speeds. NACA TM No. 1147, translated from Deutsche Luftfahrtforschung, FB 1992, 1944.Google Scholar
8.Hall, I. M.Transonic Flow in Two-Dimensional and Axially-Symmetric Nozzles. Quart. Journ. Mech Applied Math., Vol. XV, Pt. 4, pp. 487508, 1962.Google Scholar
9.Stanton, T. E. Velocity in a Wind Channel Throat. ARC R & M No. 1388, 1930.Google Scholar
10.Sibulkin, M.Heat Transfer to an Incompressible Turbulent Boundary Layer and Estimation of Heat Transfer Coefficients at Supersonic Nozzle Throats. J. Aero. Sci., Vol. 23, No. 2, pp. 162172, 1956.Google Scholar
11.Sibulkin, M.Boundary-Layer Measurements at Supersonic nozzle Throats. J. Aero Sci., Vol. 24, No. 4, pp. 249252, 1957.Google Scholar
12.SmithRobert E., Jr. Robert E., Jr. and Matz, Roy J.A Theoretical Method of Determining Discharge Coefficients for Venturis Operating at Critical Flow Conditions. Trans ASME, Paper No. 61-WA-211, 1961; Journal Basic Engineering, Vol. 84, Series D, No. 4, pp. 434446, 1962.CrossRefGoogle Scholar
13.Stratford, B. S. and Beavers, G. S. The Calculation of the Compressible Turbulent Boundary Layer in an Arbitrary Pressure Gradient—a Correlation of Certain Previous Methods. ARC R & M 3207, 1959.Google Scholar
14.Mclafferty, George H. and Barber, Robert E. Turbulent Boundary Layer Characteristics in Supersonic Streams Having Adverse Pressure Gradients. UAC Research Department Report No. UAC-R-1285-11, 1959.Google Scholar
15.Young, A. D.Skin Friction in the Laminar Boundary Layer in Compressible Flow. Aero Quarterly, Vol. I, pp. 137164, 1949.Google Scholar
16.Thwaites, B.Approximate Calculation of the Laminar Boundary Layer. Aero Quarterly, Vol. I, pp. 245, 1949-50.CrossRefGoogle Scholar
17.Compressible Airflow: Graphs. Prepared on Behalf of the Aeronautical Research Council, London, Oxford University Press, 1954.Google Scholar
18.Ashwood, P. F., CROSSE, G. W. and Goddard, JEAN E. Measurement of the Thrust Produced by Convergent/Divergent Nozzles at Pressure Ratios Up to 20. ARC CP No. 326, 1956.Google Scholar
19.Herbert, M. V., Lewis, W. G. E., and Martlew, D. L. The Design Point Performance of Model Internal Expansion Propelling Nozzles With Area Ratios Up to 4. Unpublished Work at the MOA.Google Scholar
20.Hall, G. W.Application of Boundary Layer Theory to Explain Some Nozzle and Venturi Flow Peculiarities. Proc. Inst, of Mechanical Engineers, Vol. 173, No. 36, 1959.Google Scholar