Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method

Experimental & Computational and investigations of thrust vectoring by using counter flow method had been carried out in the present work. The experimental investigation included design and construction of test rig with rectangular duct with aspect ratio of (4.4) in order to investigate the eff...

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Main Authors: Ali Abdul Almuhsen Al-Asady, Omar Hussien Ali
Format: Article
Language:English
Published: Al-Nahrain Journal for Engineering Sciences 2017-01-01
Series:مجلة النهرين للعلوم الهندسية
Subjects:
Online Access:https://nahje.com/index.php/main/article/view/21
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spelling doaj-28b59a06e96943188f6d35974f005cb32021-02-02T18:01:03ZengAl-Nahrain Journal for Engineering Sciencesمجلة النهرين للعلوم الهندسية2521-91542521-91622017-01-0119221Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow MethodAli Abdul Almuhsen Al-Asady0Omar Hussien Ali1Dep. of Mechanical Engineering, Coll. of Engineering, Baghdad UniversityDep. of Mechanical Engineering, Coll. of Engineering, Baghdad University Experimental & Computational and investigations of thrust vectoring by using counter flow method had been carried out in the present work. The experimental investigation included design and construction of test rig with rectangular duct with aspect ratio of (4.4) in order to investigate the effect of various geometric variables on thrust vectoring angle. Set of experiment at tests was carried out over the mass flow ratio (Ṁs/Ṁp) range 0 ≤ (Ṁs/Ṁp) ≤ 0.31 with secondary slot gap height g/H= (0.0294, 0.0588, 0.088 and 0.1176) and coanda surface diameter R/H= (1.176, 2.353, 3.529and 4.705). Load measurements were obtained using four load cells. The computational investigation involved a 3D numerical solution by FLUENT Software for some of experimental cases. Experimental results show that the increase in secondary jet blowing rate lead to increasing in the jet vectoring angle, there are three zone can be observed, dead zone appears at low mass flow ratios, then followed by control region in which continuous thrust vector control can be achieved followed by a saturation region. The length of the dead zone‟ was also dependent on the size of the Coanda surface diameter which a small diameter resulted in a prolonged „dead zone‟ range, and the secondary gap height to the primary gap height had inverse relation with jet vectoring angle. The investigation shows that both the experimental and computational results obtained follow a similar trend line. Mach number is less than 0.5. https://nahje.com/index.php/main/article/view/21Thrust vectoring angleJet vectoringCoanda Effectcounter flowmass flow ratio
collection DOAJ
language English
format Article
sources DOAJ
author Ali Abdul Almuhsen Al-Asady
Omar Hussien Ali
spellingShingle Ali Abdul Almuhsen Al-Asady
Omar Hussien Ali
Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
مجلة النهرين للعلوم الهندسية
Thrust vectoring angle
Jet vectoring
Coanda Effect
counter flow
mass flow ratio
author_facet Ali Abdul Almuhsen Al-Asady
Omar Hussien Ali
author_sort Ali Abdul Almuhsen Al-Asady
title Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
title_short Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
title_full Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
title_fullStr Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
title_full_unstemmed Fluidic Jet Vectoring at Subsonic Flow ay Using Counter Flow Method
title_sort fluidic jet vectoring at subsonic flow ay using counter flow method
publisher Al-Nahrain Journal for Engineering Sciences
series مجلة النهرين للعلوم الهندسية
issn 2521-9154
2521-9162
publishDate 2017-01-01
description Experimental & Computational and investigations of thrust vectoring by using counter flow method had been carried out in the present work. The experimental investigation included design and construction of test rig with rectangular duct with aspect ratio of (4.4) in order to investigate the effect of various geometric variables on thrust vectoring angle. Set of experiment at tests was carried out over the mass flow ratio (Ṁs/Ṁp) range 0 ≤ (Ṁs/Ṁp) ≤ 0.31 with secondary slot gap height g/H= (0.0294, 0.0588, 0.088 and 0.1176) and coanda surface diameter R/H= (1.176, 2.353, 3.529and 4.705). Load measurements were obtained using four load cells. The computational investigation involved a 3D numerical solution by FLUENT Software for some of experimental cases. Experimental results show that the increase in secondary jet blowing rate lead to increasing in the jet vectoring angle, there are three zone can be observed, dead zone appears at low mass flow ratios, then followed by control region in which continuous thrust vector control can be achieved followed by a saturation region. The length of the dead zone‟ was also dependent on the size of the Coanda surface diameter which a small diameter resulted in a prolonged „dead zone‟ range, and the secondary gap height to the primary gap height had inverse relation with jet vectoring angle. The investigation shows that both the experimental and computational results obtained follow a similar trend line. Mach number is less than 0.5.
topic Thrust vectoring angle
Jet vectoring
Coanda Effect
counter flow
mass flow ratio
url https://nahje.com/index.php/main/article/view/21
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