Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave

An unsteady numerical simulation method was used in order to explore more efficient atomization methods for liquid fuel in scramjet combustors and to study the influence of different shock wave incident positions on the atomization characteristics of kerosene in crossflow. The wedge compression surf...

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Main Authors: Yongsheng Zhao, Junfei Wu, Xiangyang Mu
Format: Article
Language:English
Published: MDPI AG 2022-12-01
Series:Aerospace
Subjects:
Online Access:https://www.mdpi.com/2226-4310/10/1/30
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author Yongsheng Zhao
Junfei Wu
Xiangyang Mu
author_facet Yongsheng Zhao
Junfei Wu
Xiangyang Mu
author_sort Yongsheng Zhao
collection DOAJ
description An unsteady numerical simulation method was used in order to explore more efficient atomization methods for liquid fuel in scramjet combustors and to study the influence of different shock wave incident positions on the atomization characteristics of kerosene in crossflow. The wedge compression surface was used to generate the incident shock wave, and the incident position of the shock wave on the fuel jet was controlled by changing the angle of the wedge surface. The inlet Mach number was 2.01; the total temperature was 300 K, and the momentum ratio was 12. The research results show that as the incident position of the shock wave moves upstream, the penetration depth of the jet is essentially unchanged, but the inner edge trajectory of the jet is closer to the wall. Because the shock wave affects the Kelvin–Helmholtz instability of the jet, the unsteadiness of the jet root is strengthened, and the unsteadiness downstream of the jet is weakened. The atomization of the jet and the stability of the particle-size distribution are, thus, realized more quickly. The incident shock wave reduces the Sauter mean diameter of the jet section and makes the droplet distribution more uniform. The incident shock wave makes the atomization angle of the jet along the flow direction increase first and then decrease. The changes in the jet characteristics are determined by the changes in the reflux region, momentum transport, and pressure distribution caused by the incident shock wave.
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spelling doaj.art-63367273bb0547c09961448a558428c92023-12-02T01:17:08ZengMDPI AGAerospace2226-43102022-12-011013010.3390/aerospace10010030Atomization Characteristics of Kerosene in Crossflow with an Incident Shock WaveYongsheng Zhao0Junfei Wu1Xiangyang Mu2China Academy of Aerospace Aerodynamics, Beijing 100074, ChinaChina Academy of Aerospace Aerodynamics, Beijing 100074, ChinaChina Academy of Aerospace Aerodynamics, Beijing 100074, ChinaAn unsteady numerical simulation method was used in order to explore more efficient atomization methods for liquid fuel in scramjet combustors and to study the influence of different shock wave incident positions on the atomization characteristics of kerosene in crossflow. The wedge compression surface was used to generate the incident shock wave, and the incident position of the shock wave on the fuel jet was controlled by changing the angle of the wedge surface. The inlet Mach number was 2.01; the total temperature was 300 K, and the momentum ratio was 12. The research results show that as the incident position of the shock wave moves upstream, the penetration depth of the jet is essentially unchanged, but the inner edge trajectory of the jet is closer to the wall. Because the shock wave affects the Kelvin–Helmholtz instability of the jet, the unsteadiness of the jet root is strengthened, and the unsteadiness downstream of the jet is weakened. The atomization of the jet and the stability of the particle-size distribution are, thus, realized more quickly. The incident shock wave reduces the Sauter mean diameter of the jet section and makes the droplet distribution more uniform. The incident shock wave makes the atomization angle of the jet along the flow direction increase first and then decrease. The changes in the jet characteristics are determined by the changes in the reflux region, momentum transport, and pressure distribution caused by the incident shock wave.https://www.mdpi.com/2226-4310/10/1/30shock wavecrossflowincident positionnumerical simulationatomization characteristics
spellingShingle Yongsheng Zhao
Junfei Wu
Xiangyang Mu
Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
Aerospace
shock wave
crossflow
incident position
numerical simulation
atomization characteristics
title Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
title_full Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
title_fullStr Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
title_full_unstemmed Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
title_short Atomization Characteristics of Kerosene in Crossflow with an Incident Shock Wave
title_sort atomization characteristics of kerosene in crossflow with an incident shock wave
topic shock wave
crossflow
incident position
numerical simulation
atomization characteristics
url https://www.mdpi.com/2226-4310/10/1/30
work_keys_str_mv AT yongshengzhao atomizationcharacteristicsofkeroseneincrossflowwithanincidentshockwave
AT junfeiwu atomizationcharacteristicsofkeroseneincrossflowwithanincidentshockwave
AT xiangyangmu atomizationcharacteristicsofkeroseneincrossflowwithanincidentshockwave