Experiments on water vapour condensation within supersonic nozzle flow generated by an impulse tunnel
•Experiments on condensation shocks performed using a shock tunnel and Ludwieg tube.•A Nitrogen/Water vapour mixture with RH=25–100% and temperature 293–343 K was tested.•Fast pressure transducers allowed comparing experimental wave speeds with theory.•Condensation shock locations and angles were ac...
Gespeichert in:
Veröffentlicht in: | International journal of multiphase flow 2021-01, Vol.134, p.103473, Article 103473 |
---|---|
Hauptverfasser: | , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | •Experiments on condensation shocks performed using a shock tunnel and Ludwieg tube.•A Nitrogen/Water vapour mixture with RH=25–100% and temperature 293–343 K was tested.•Fast pressure transducers allowed comparing experimental wave speeds with theory.•Condensation shock locations and angles were acquired with Schlieren visualizations.•The impulse facility reduces operating costs relative to a continuous flow setup.
An impulse facility for analysis of water vapour nozzle flows using both shock tunnel and Ludwieg tube operating modes has been developed and tested at the University of Southern Queensland. Unique high-speed flow visualisation of the water vapour condensation shock has been acquired in the throat region of a nominally two-dimensional convergent-divergent nozzle with a 120 mm2 throat area. This paper presents the facility performance and the time-resolved visualisation results for the nozzle flow, and the results are analysed with the aid of image post-processing tools and quasi-one-dimensional (Q1D) thermodynamic calculations. The experiments have produced qualitative and quantitative data on the flow conditions at four different relative humidity values from 25% to 100%, and over a range of nozzle supply temperatures between 293 K and 343 K. The direct measurement of the pressures and wave speeds within the tunnel resulted in a good agreement with the ideal gas Q1D calculations, particularly for the first incident shocks and expansion waves. Differences progressively increased with the number of reflections, due to the effect of viscous dissipation and the non-ideal end-wall interaction caused by the presence of the nozzle inlet. Moreover, flow visualizations of the location and orientation of both the weak disturbance waves and the condensation shock enabled the investigation of the supersonic water vapour condensation within the nozzle of this impulse facility. Based on these measurements, the nozzle flow downstream of the condensation shock was demonstrated to have a lower Mach number relative to the dry nitrogen flow case. This phenomenon is due to the phase change heat release, which appeared to be more significant when the condensation shock intensity was higher. Although further development of the apparatus is possible, the impulse test-rig configuration that we have developed permits a relatively high flow rate of test gas for a short period of time, leading to significantly reduced operating expenses relative to a continuous flow fac |
---|---|
ISSN: | 0301-9322 1879-3533 |
DOI: | 10.1016/j.ijmultiphaseflow.2020.103473 |