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      Flowfield Analysis and Reconstruction of Ethylene–Air Continuous Rotating Detonation Wave

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          Abstract

          The time difference calculation method, using the pressure peak rise time difference of high-frequency dynamic pressure signals to demonstrate the motion track of continuous rotating detonation wave (CRDW), is presented and verified. With the calculation method, the flowfield of CRDW has been reconstructed precisely. The angle of upstream oblique shock wave is defined for representing the influence of CRDW on the air inflow, which is impacted by the detonation combustion intensity and nozzle choking effect. The increase of combustor pressure makes the angle of upstream oblique shock wave decrease, indicating that the influence of detonation on air inflow strengthens. The angle of downstream oblique shock wave is mainly influenced by the contraction geometry of nozzle in the contraction ratio range of 2–10. The heights of CRDWs scatter around 60 ± 10  mm ( C 2 H 4 ), 40 ± 20  mm ( H 2 , single wave), and 20 ± 10  mm ( H 2 , two waves), respectively. The detonation wave height of single wave is higher than that of two waves in homo-rotating, and the height of ethylene–air CRDW is higher than that of hydrogen–air CRDW. This study will enrich the understanding and analysis method of CRDW flowfield structure.

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          Detonative propulsion

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            Rotating Detonation Wave Propulsion: Experimental Challenges, Modeling, and Engine Concepts

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              Continuous Spin Detonations

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                Author and article information

                Journal
                aiaaj
                AIAA Journal
                AIAA Journal
                American Institute of Aeronautics and Astronautics
                1533-385X
                17 February 2020
                December 2020
                : 58
                : 12
                : 5036-5045
                Affiliations
                National University of Defense Technology , 410073 Changsha, People’s Republic of China
                Author notes
                [*]

                Ph.D. Candidate, Science and Technology on Scramjet Laboratory, College of Aerospace Science and Technology, Hunan Province.

                [†]

                Professor, Science and Technology on Scramjet Laboratory, College of Aerospace Science and Technology, Hunan Province; wdliu@ 123456nudt.edu.cn (Corresponding Author).

                [‡]

                Associate Professor, Science and Technology on Scramjet Laboratory, College of Aerospace Science and Technology, Hunan Province.

                [§]

                Lecturer, Science and Technology on Scramjet Laboratory, College of Aerospace Science and Technology, Hunan Province.

                [¶]

                Assistant Engineer, Science and Technology on Scramjet Laboratory, College of Aerospace Science and Technology, Hunan Province.

                Article
                J058099 J058099
                10.2514/1.J058099
                7331cc5e-a279-4722-80ce-edf180732e84
                Copyright © 2019 by the American Institute of Aeronautics and Astronautics, Inc. All rights reserved. All requests for copying and permission to reprint should be submitted to CCC at www.copyright.com; employ the eISSN 1533-385X to initiate your request. See also AIAA Rights and Permissions www.aiaa.org/randp.
                History
                : 22 November 2018
                : 19 June 2019
                : 27 November 2019
                Page count
                Figures: 20, Tables: 1
                Funding
                Funded by: National Natural Science Foundation of Chinahttp://dx.doi.org/10.13039/501100001809
                Award ID: 51776220
                Award ID: 91541103
                Categories
                Continuous Detonation and its Applications

                Engineering,Physics,Mechanical engineering,Space Physics
                Engineering, Physics, Mechanical engineering, Space Physics

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