Experimental Investigation of the Structure of Disturbances from Two Pulsed Sources in the Flat-Plate Supersonic Boundary Layer
- Authors: Afanasev L.V.1, Yermolaev Y.G.1, Kosinov A.D.1, Kocharin V.L.1, Semionov N.V.1, Yatskikh A.A.1
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Affiliations:
- Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
- Issue: No 4 (2023)
- Pages: 27-36
- Section: Articles
- URL: https://journals.rcsi.science/1024-7084/article/view/135086
- DOI: https://doi.org/10.31857/S1024708423600070
- EDN: https://elibrary.ru/WLFQGI
- ID: 135086
Cite item
Abstract
The work is devoted to the development of a new experimental method for entering controlled disturbances with a given frequency-wave structure into a supersonic boundary layer. Experimental data on the formation of disturbances from two pulsed sources (pulsed glow discharge) in the laminar flat-plate boundary layer at the Mach number equal to 2 are given. The experiments were carried out in the T-325 wind tunnel of ITAM SB RAS. The localized sources were spaced out at the same distance from the leading edge of the plate at 6 mm from each other spanwise. Flow pulsations were measured using a hot-wire probe of constant temperature anemometer, the signal was recorded synchronously with ignition of the discharges. This made it possible to distinguish the pulsations from the discharges against the background of random uncontrolled “natural” pulsations of the boundary layer. The spatial-temporal and frequency-wave structure of the generated disturbances from a single or two discharges, operating synchronously or with a time delay, are analyzed. It is found that the maximum difference in the structure of disturbances from one and two sources is observed in the central region, while at the side boundaries of the disturbances, the pulsations are close in all considered cases. In the wave spectra of disturbances from two discharges, nodes and antinodes are formed. Their position is determined by the distance between the sources and the time delay in their operation.
About the authors
L. V. Afanasev
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
Yu. G. Yermolaev
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
A. D. Kosinov
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
V. L. Kocharin
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
N. V. Semionov
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
A. A. Yatskikh
Khristianovich Institute of Theoretical and Applied Mechanics, Siberian Branch of the Russian Academy of Sciences
Author for correspondence.
Email: yatskikh@itam.nsc.ru
Novosibirsk, Russia
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