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Co-Flowing Jet Control Using Lip Thickness Variation

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Abstract The control of co-flowing jets by varying lip thickness has been studied experimentally. Lip thickness is defined as the thickness of primary nozzle wall separating primary jet and secondary jet at the co-flowing nozzle exit. Co-flowing jets from a primary nozzle of diameter 10 mm (1.0 Dp) and a secondary duct with lip thickness (LT) 0.2 Dp, 1.0 Dp and 1.5 Dp at Mach numbers 0.6, 0.8 and 1.0 have been studied. Jet centreline total pressure decay, static pressure variation and jet mixing behaviour were analysed. The results show that the mixing of the co-flowing jet with substantial values of lip thickness is superior to the co-flowing jets with comparatively lower values of lip thickness. Co-flowing jets with lip thickness 1.0 Dp and 1.5 Dp experience a significantly higher mixing than the lip thickness 0.2 Dp jet, for all Mach numbers analyzed in the present study. Moreover, in the case of correctly expanded jets, the local static pressure is assumed to be equal to atmospheric pressure. This assumption becomes invalid for co-flowing jets with substantial lip thickness. The centerline static pressure varies sinusoidally above and below atmospheric pressure by a maximum of 11 %, which is due to wake dominance.
Title: Co-Flowing Jet Control Using Lip Thickness Variation
Description:
Abstract The control of co-flowing jets by varying lip thickness has been studied experimentally.
Lip thickness is defined as the thickness of primary nozzle wall separating primary jet and secondary jet at the co-flowing nozzle exit.
Co-flowing jets from a primary nozzle of diameter 10 mm (1.
0 Dp) and a secondary duct with lip thickness (LT) 0.
2 Dp, 1.
0 Dp and 1.
5 Dp at Mach numbers 0.
6, 0.
8 and 1.
0 have been studied.
Jet centreline total pressure decay, static pressure variation and jet mixing behaviour were analysed.
The results show that the mixing of the co-flowing jet with substantial values of lip thickness is superior to the co-flowing jets with comparatively lower values of lip thickness.
Co-flowing jets with lip thickness 1.
0 Dp and 1.
5 Dp experience a significantly higher mixing than the lip thickness 0.
2 Dp jet, for all Mach numbers analyzed in the present study.
Moreover, in the case of correctly expanded jets, the local static pressure is assumed to be equal to atmospheric pressure.
This assumption becomes invalid for co-flowing jets with substantial lip thickness.
The centerline static pressure varies sinusoidally above and below atmospheric pressure by a maximum of 11 %, which is due to wake dominance.

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