Effectiveness of jet location on mixing characteristics inside a cavity in supersonic flow
Effectiveness of jet location on mixing characteristics inside a cavity in supersonic flow
The incorporation of cavities within supersonic combustion chambers is an effective means of slowing down the flow for fuel injection and consequent stable combustion. Understanding the flow physics associated with such flows, especially with the injection of a gas to replicate fuel injection, are essential for the optimum design of supersonic propulsion mechanisms. An experimental investigation was performed on a rectangular open cavity with upstream injection model in a Mach number of 1.9 using a trisonic indraft wind tunnel. A rectangular open cavity of dimensions L/D = 5, 100 mm in length (L) and 20 mm deep (D), was adopted, and it was embedded into the lower wall of the test section. An air jet with a jet-to-freestream momentum flux ratio of J = 1.2, 2.7 and 5.3 was injected upstream of the cavity. To evaluate the effect on mixing and flow stability the jet position, measured from the front edge of the cavity, was varied between 0.1L and 1L. The flow field was visualized using schlieren photography, particle image velocimetry, and oil flow measurements. It is found that the mixing characteristic within the cavity when the jet is positioned 0.1L is enhanced independent on the J value because the turbulence intensity of the flow velocity within the cavity is strongly influenced by the jet interaction which lifted the flow from the floor of the cavity compared to the other jet positions. However, the flow over the cavity is unstable at all jet positions. The separation shock formed at the front edge of the cavity oscillates significantly for the case where the jet is located at 0.1L because the separation shock location coincides with the compression shock behind the jet.
59-67
Ukai, Takahiro
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Zare-Behtash, Hossein
74be9b97-cb09-49c6-9f75-7ec58c0dd16c
Erdem, Erinc
6f4133a8-8084-4286-b93d-e303bc375d8d
Lo, Kin Hing
e2fcd08c-2efd-4cec-ad0a-92969e9d1139
Kontis, Konstantinos
e40ecdbc-e5e9-4522-abf9-e3c3f3c2d7fa
Obayashi, Shigeru
f5569406-1354-4642-82c3-82bf73c6594e
Ukai, Takahiro
b83787a3-b48e-4c83-8ad1-9d6c15ef8a7b
Zare-Behtash, Hossein
74be9b97-cb09-49c6-9f75-7ec58c0dd16c
Erdem, Erinc
6f4133a8-8084-4286-b93d-e303bc375d8d
Lo, Kin Hing
e2fcd08c-2efd-4cec-ad0a-92969e9d1139
Kontis, Konstantinos
e40ecdbc-e5e9-4522-abf9-e3c3f3c2d7fa
Obayashi, Shigeru
f5569406-1354-4642-82c3-82bf73c6594e
Ukai, Takahiro, Zare-Behtash, Hossein, Erdem, Erinc, Lo, Kin Hing, Kontis, Konstantinos and Obayashi, Shigeru
(2013)
Effectiveness of jet location on mixing characteristics inside a cavity in supersonic flow.
Experimental Thermal and Fluid Science, 52, .
(doi:10.1016/j.expthermflusci.2013.08.022).
Abstract
The incorporation of cavities within supersonic combustion chambers is an effective means of slowing down the flow for fuel injection and consequent stable combustion. Understanding the flow physics associated with such flows, especially with the injection of a gas to replicate fuel injection, are essential for the optimum design of supersonic propulsion mechanisms. An experimental investigation was performed on a rectangular open cavity with upstream injection model in a Mach number of 1.9 using a trisonic indraft wind tunnel. A rectangular open cavity of dimensions L/D = 5, 100 mm in length (L) and 20 mm deep (D), was adopted, and it was embedded into the lower wall of the test section. An air jet with a jet-to-freestream momentum flux ratio of J = 1.2, 2.7 and 5.3 was injected upstream of the cavity. To evaluate the effect on mixing and flow stability the jet position, measured from the front edge of the cavity, was varied between 0.1L and 1L. The flow field was visualized using schlieren photography, particle image velocimetry, and oil flow measurements. It is found that the mixing characteristic within the cavity when the jet is positioned 0.1L is enhanced independent on the J value because the turbulence intensity of the flow velocity within the cavity is strongly influenced by the jet interaction which lifted the flow from the floor of the cavity compared to the other jet positions. However, the flow over the cavity is unstable at all jet positions. The separation shock formed at the front edge of the cavity oscillates significantly for the case where the jet is located at 0.1L because the separation shock location coincides with the compression shock behind the jet.
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Accepted/In Press date: 28 August 2013
e-pub ahead of print date: 5 September 2013
Identifiers
Local EPrints ID: 491698
URI: http://eprints.soton.ac.uk/id/eprint/491698
ISSN: 0894-1777
PURE UUID: 14518726-8032-4462-b71c-6c7e4f444eef
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Date deposited: 03 Jul 2024 16:03
Last modified: 11 Jul 2024 02:18
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Author:
Takahiro Ukai
Author:
Hossein Zare-Behtash
Author:
Erinc Erdem
Author:
Kin Hing Lo
Author:
Konstantinos Kontis
Author:
Shigeru Obayashi
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