“…This set-up consists of a M ϭ1.37 supersonic jet surrounded by a subsonic entrained co-flow. Stagnation pressure and temperature for the main jet are respectively 3ϫ10 5 Pa and 260 K. The coflow velocity and stagnation temperature are 47 m/s and 290 K. The convective Mach number is M C ϭ0.55, and the convective velocity U C ϭ230 m/s. The supersonic jet has the same static pressure as the subsonic co flow.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…Lateral test section walls comprise large windows such that visualizations or laser Doppler measurements can be easily performed. A 200ϫ10 5 Pa dry air tank supplies the main jet.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…3 and 4. The CJ stagnation pressure is kept constant at 2.5ϫ10 5 Pa, which results in a velocity ratio U CJ /U 1 Ϸ0.89. The CJ nozzle is convergent, and its exit is sonic.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…Additional experiments were performed to test these hypotheses. Instantaneous visualizations were performed, increasing the stagnation pressure of the CJ up to 10 ϫ10 5 Pa. Two representative instantaneous images for a CJ stagnation pressure of 10ϫ10 5 Pa are shown in Fig. 14. Since the CJ nozzle is convergent, it is strongly underexpanded for this regime.…”
Section: B Two Point Correlationsmentioning
confidence: 99%
“…The former cathegory includes resonance based devices, such as cavities, 3 impingement obstacles, 4 and self-exciting wires. 5 The cavity size, obstacles geometry and position, the wire diameter and tension are adjusted such that the associated frequency matches that of the main flow instability. Such devices are technologically simple and can achieve significant mixing enhancement.…”
An experimental study is performed to analyze the interaction between a control jet ͑CJ͒ and a moderately supersonic main jet. Flow visualizations and laser Doppler velocimetry methods are used. A strong instability of the CJ has been identified. The dynamic of this instability corresponds to that of the local mixing layer. Two stability scenarios are proposed, one corresponding to the local Kelvin-Helmholtz instability of the main jet, the other linked to a local absolute instability of the interaction. The impact on the turbulent quantities is analyzed. It is shown that a strong modification of the Reynolds stress is manifest but that this extends only a small distance from the interaction.
“…This set-up consists of a M ϭ1.37 supersonic jet surrounded by a subsonic entrained co-flow. Stagnation pressure and temperature for the main jet are respectively 3ϫ10 5 Pa and 260 K. The coflow velocity and stagnation temperature are 47 m/s and 290 K. The convective Mach number is M C ϭ0.55, and the convective velocity U C ϭ230 m/s. The supersonic jet has the same static pressure as the subsonic co flow.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…Lateral test section walls comprise large windows such that visualizations or laser Doppler measurements can be easily performed. A 200ϫ10 5 Pa dry air tank supplies the main jet.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…3 and 4. The CJ stagnation pressure is kept constant at 2.5ϫ10 5 Pa, which results in a velocity ratio U CJ /U 1 Ϸ0.89. The CJ nozzle is convergent, and its exit is sonic.…”
Section: A Wind Tunnel and Control Jetmentioning
confidence: 99%
“…Additional experiments were performed to test these hypotheses. Instantaneous visualizations were performed, increasing the stagnation pressure of the CJ up to 10 ϫ10 5 Pa. Two representative instantaneous images for a CJ stagnation pressure of 10ϫ10 5 Pa are shown in Fig. 14. Since the CJ nozzle is convergent, it is strongly underexpanded for this regime.…”
Section: B Two Point Correlationsmentioning
confidence: 99%
“…The former cathegory includes resonance based devices, such as cavities, 3 impingement obstacles, 4 and self-exciting wires. 5 The cavity size, obstacles geometry and position, the wire diameter and tension are adjusted such that the associated frequency matches that of the main flow instability. Such devices are technologically simple and can achieve significant mixing enhancement.…”
An experimental study is performed to analyze the interaction between a control jet ͑CJ͒ and a moderately supersonic main jet. Flow visualizations and laser Doppler velocimetry methods are used. A strong instability of the CJ has been identified. The dynamic of this instability corresponds to that of the local mixing layer. Two stability scenarios are proposed, one corresponding to the local Kelvin-Helmholtz instability of the main jet, the other linked to a local absolute instability of the interaction. The impact on the turbulent quantities is analyzed. It is shown that a strong modification of the Reynolds stress is manifest but that this extends only a small distance from the interaction.
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