Spelling suggestions: "subject:"iiquid jet inn crossflow"" "subject:"iiquid jet iin crossflow""
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Primary Breakup and Droplet Evaporation of Liquid Jets in Subsonic CrossflowsShaw, Vincent 24 May 2022 (has links)
No description available.
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Atomization of a Liquid Water Jet in Crossflow at Varying Hot Temperatures for High-Speed Engine and Stratospheric Aerosol Injection ApplicationsCaetano, Luke 01 January 2022 (has links)
This paper aims to study how varying crossflow burning temperatures from 1100 C to 1800 C affect the liquid droplet breakup, size distribution, and atomization of a liquid water jet injected into a vitiated crossflow. The LJIC injection mechanism was implemented using the high-pressure axially staged combustion facility at the University of Central Florida. The measurement devices used to gather particle data from the exhaust plume were the TSI Aerodynamic Particle Sizer (APS), which measures particles between 0.523 µm and 20 µm, and the Sensirion SPS30 (SPS30), which measures particles between 0.3 µm and 10 µm. Both measurement devices were placed 3 ft away from the choked exit. Table 3 shows that the 1800 C crossflow temperature behaved as predicted by having the largest particle distribution of 67.97% and the largest particle count of 19,301 at 0.523 µm. The 1100 C crossflow produced the second-largest normalized particle count of 66.69% and raw particle count of 20,209 at 0.523 µm. This result is contrary to the original hypothesis because it shows that the relationship between temperature and particle count is non-linear and that many other factors must be at play in the atomization process, such as the droplet distribution at the nano level. The SPS30 was used to compare the particle size distributions between a 1500 C and 1800 C crossflow. Acquiring number concentration data for particles up to 10 µm in size, the 1800 C crossflow had a distribution peak at 802.76416 N/cm3, and the 1500 C crossflow had a peak of 867.28272 N/cm3. For the 0.5 µm peak, The 1800 C had a 10 µm particle size distribution peak at 674.27.76416 N/cm3, and the 1500C crossflow had a peak of 730.501 N/cm3. The decreased number concentration from 1500 C to 1800 C case grants the water particles in the 1800 C crossflow increased surface area, which allows for increased heat exposure from the vitiated crossflow [7]. Despite some nonlinear particle count results, the highest crossflow temperature of 1800 C produces the best atomization results by reducing the total particle count and having the largest collection of particles at the lowest detectable particle size of 0.523 µm.
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Liquid Jets Injected into Non-Uniform CrossflowTambe, Samir B. 06 August 2010 (has links)
No description available.
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Simulation multi-échelle de l’atomisation d’un jet liquide sous l’effet d’un écoulement gazeux transverse en présence d’une perturbation acoustique / Multiscale simulation of the atomization of a liquid jet in oscillating gaseous crossflowThuillet, Swann 05 December 2018 (has links)
La réduction des émissions polluantes est actuellement un enjeu majeur au sein du secteur aéronautique. Parmi les solutions développées par les motoristes, la combustion en régime pauvre apparaît comme une technologie efficace pour réduire l’impact de la combustion sur l’environnement.Or, ce type de technologie favorise l’apparition d’instabilités de combustion issues d’un couplage thermo-acoustique. Des études expérimentales précédemment menées à l’ONERA ont mis en évidence l’importance de l’atomisation au sein d’un injecteur multipoint sur le phénomène d’instabilités de combustion. L’objectif de cette thèse est de mettre en place la méthodologie multi-échelle pour reproduire les phénomènes de couplage entre l’atomisation du jet liquide en présence d’un écoulement gazeux transverse (configuration simplifiée d’un point d’injection d’un injecteur multipoint) et d’une perturbation acoustique imposée, représentative de l’effet d’une instabilité de combustion. Ce type d’approche pourra, à terme, être utilisé pour la simulation instationnaire LES d’un système de combustion, et permettra de déterminer les temps caractéristiques de convection du carburant liquide pouvant affecter les phénomènes d’évaporation et de combustion, et donc l’apparition des instabilités de combustions. Afin de valider cette approche,les résultats issus des simulations sont systématiquement comparés aux observations expérimentales obtenues dans le cadre du projet SIGMA. Dans un premier temps, une simulation du jet liquide en présence d’un écoulement gazeux transverse est réalisée. Cette simulation a permis de valider l’approche multi-échelle : pour cela, les grandes échelles du jet, ainsi que les mécanismes d’atomisation reproduits par les simulations, sont analysés. Ensuite, l’influence d’une perturbation acoustique sur l’atomisation du jet liquide est étudiée. Les comportements instationnaires du jet et du spray issu de l’atomisation sont comparés aux résultats expérimentaux à l’aide des moyennes temporelles et des moyennes de phase. / The reduction of polluting emissions is currently a major issue in the aeronautics industry.Among the solutions developed by the engine manufacturers, lean combustion appears as an effectivetechnology to reduce the impact of combustion on the environment. However, this type oftechnology enhances the onset of combustion instabilities, resulting from a thermo-acoustic coupling.Experimental studies previously conducted at ONERA have highlighted the importanceof atomization in a multipoint injector to the combustion instabilities. The aim of this thesis isto implement the multi-scale methodology to reproduce the coupling phenomena between theatomization of the liquid jet in the presence of a crossflow (which is a simplified configuration ofan injection point of a multipoint injector) and an imposed acoustic perturbation, representativeof the effect of combustion instabilities. This type of approach can ultimately be used for the unsteadysimulation of a combustion system, and will determine the characteristic convection timesof the liquid fuel that can affect the phenomena of evaporation and combustion, and therefore theappearance of combustion instabilities. In order to validate this approach, the results obtainedfrom the simulations are systematically compared with the experimental observations obtainedwithin the framework of the SIGMA project. First, a simulation of the liquid jet in gaseous crossflowis performed. This simulation enabled us to validate the multi-scale approach : to this end,the large scales of the jet, as well as the atomization mechanisms reproduced by the simulations,are analyzed. Then, the influence of an acoustic perturbation on the atomization of the liquidjet is studied. The unsteady behavior of the jet and the spray resulting from the atomization arecompared with the experimental results using time averages and phase averages.
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Analysis of Variations in Flow-Independent Liquid Jet-in-Crossflow InjectionsScott, Michael 01 January 2024 (has links) (PDF)
Liquid fuel injection is a critical mechanism for the deliverance of liquid fuel in contemporary aircraft propulsion combustion systems due to its outsized influence in providing optimal combustion conditions and improving overall aircraft efficiency and performance. Despite this, these liquid jet in crossflow (LJIC) systems are highly variable due to conditions in the jet and the surrounding airflow, leading to variability in performance behavior and inconsistency in fuel mixing and combustion efficiency. This has prompted the introduction of solid pintile obstructions of novel designs to provide a more flow-independent fuel injection scheme and decrease variability of the jet properties against a range of crossflow conditions.
This thesis will examine the effects of a solid pintile obstruction on the behavior of an LJIC injection in a typical ramjet combustion configuration, with a focus on the face angle variations of these pintiles. Two pintiles, with face angles of 60° and 120°, will be tested against a no-pintile control configuration under a range of relevant operating conditions and observed under a novel method of 3D-imaging in the x-z plane view. The investigation is designed to understand the effects of these pintiles in the context of broad shifts in the momentum flux ratio and Weber number across a broad range of vitiated and non-vitiated environments.
Results demonstrate the significance of the pintiles on the trajectory and performance of an LJIC injection. Building upon previous investigations on the influence of various pintile dimensions, the face angle was found to play a similarly critical role in the influence of the LJIC injection. Overall, the 120° wider face angle appears to be most optimal in enhancing crossflow interaction and promoting flow-independence compared to the 60° face angle. Future research on narrower and wider face angles and the relationship between the face angle and other design parameters could further improve LJIC injection performance and flow-independence.
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