Induced pressure distribution of a jet in a crossflow. by R. L. Fearn

Cover of: Induced pressure distribution of a jet in a crossflow. | R. L. Fearn

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SeriesNASA-TN-D-7916
ContributionsWeston, Robert P., National Aeronautics and Space Administration.
ID Numbers
Open LibraryOL16342588M

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Induced Surface Pressure Distribution of a Subsonic Jet in a Crossflow Article (PDF Available) January with 65 Reads How we measure 'reads'.

The scalar concentration field of the round jet in a uniform crossflow is studied for a range of jet to crossflow velocity ratios, r, with emphasis on r = 10 using planar laser-induced.

The Induced Aerodynamics of Jet and Fan Powered V/STOL Aircraft. Authors; R. “Induced Pressure Distribution of a Jet in a Crossflow,” NASA TN D, July Google Scholar [9] “A Study of Real Jet Effects on the Surface Pressure Distribution Induced by a Jet in a Crossflow,” NASA CR, March Google Scholar [25]Cited by: The model is applied to the configuration of a round jet exhausting perpendicularly through a flat plate into a uniform crossflow for a range of jet-to-crossflow velocity ratios from 3 to It is demonstrated that the model is capable of describing the measured pressure distribution on the flat plate with model parameters that are compatable Cited by: 7.

Two models of a turbulent vertical surface jet (diameters mm and mm ⁠) were designed and tested over a range of jet exit Reynolds numbers up to 10 4 ⁠. The results show that from Reynolds number – there is about a 40% increase in the entrainment coefficient, whereas from Reynolds number –10, the increase in Cited by: 6.

Good steam side flow distribution in the tubes of the high-pressure superheater/reheater is critical to properly cool the metal pressure parts. Flow distribution is a function of the flow area within the headers and the pressure loss in the tubes between the headers. Larger header diameters and/or higher tubeside pressure loss create better.

Broadband noise with a Gaussian distribution is added to this profile with an intensity of 1% of it encounters an adverse pressure gradient on the jet leeside, inducing the first boundary layer separation in the early wake region.

which is induced when the crossflow bypassing the jet blockage separates in the low-pressure region and is Cited by: 6. The jet injection angles were 90 and 60 deg. Surface pressure distribution results were obtained for jet-to-freestream velocity ratios of4, and 8. Mean flow and turbulence flowfield data were obtained for the side-by-side dual jets, mainly for the jet-to-freestream velocity ratio of more» 4.

Fig. 17 shows the St distribution comparison for the blunt body with d 0 = 2 mm and 4 mm at different jet pressure ratios. It is seen that St has an evident diminish when a counterflowing system with a 4 mm nozzle is installed on the spiked aircraft, and the falling dimension of St rises with the growth of PR, as there is a 45% decline in PR Cited by:   Hence, an experimental investigation of TF-JICF spray behaviors was performed by our group, covering the operating conditions of – atm in crossflow pressure, – in crossflow Weber number, 5–40 in momentum flux-ratio, and 0%–% in air-nozzle pressure-drop, at the crossflow temperature of °C and velocity of 75 m/ by: 5.

@article{osti_, title = {PLIF measurement of fuel concentration distribution in transient hydrogen jet flame}, author = {Tomita, Eiji and Hamamoto, Yoshisuke and Yoshiyama, Sadami and Toda, Hitoshi}, abstractNote = {To know the concentration field of fuel spray or jet is very important because the following combustion process strongly depends on it.

Study on Drag Coefficient for the Flow Past a Cylinder % ½= ¿ µ. (2) Where C H is Drag coefficient, F H is Drag Force, ρ is Air Density and U is free stream air velocity. Drag coefficient by pressure distribution Method: In this method we calculated drag coefficient.

We. The flow and flame characteristics of a 15° backward-inclined jet flame in crossflow were investigated in a wind tunnel. The flow structures, flame behaviors, and temperature fields were measured. The jet-to-crossflow momentum flux ratio was less than The flow patterns were investigated using photography and Mie-scattering : Ching Min Hsu, Dickson Bwana Mosiria, Wei Chih Jhan.

The effect of vortex generators in the form of tabs on the penetration and spreading of a jet in a cross‐flow has been studied experimentally. It is found that the tab has very little effect when placed on the leeward side, i.e., on the downstream edge of the jet nozzle relative to the free‐stream by: a ZZZrueger-accom _ Ecellence in Air Distribution a1AIR DISTRIBUTION ENGINEERING AIR DISTRIBUTION ENGINEERING AIR DISTRIBUTION BASICS Primary Jet Extensive studies have shown that the air jet from free round openings, grilles, perforated panels, ceiling diffusers, and other INDUCED ROOM A R GENTLE MOVEMENT GREATEST POSSIBLE SOURCE OF.

Vertical jet in flowing water is a common phenomenon in daily life. To study the flow and turbulent characteristics of different jet orifice shapes and under different velocity ratios, the realizable k-ε turbulent model was adopted to analyze the three-dimensional (3D) flow, turbulence, and vortex characteristics using circular, square, and rectangular jet orifices and velocity ratios of 2, 5.

The change in pressure distribution results in forces in the aft flow direction which is the actual drag induced by the lift. The awful diagram purports (and has done so for decades) to give a physical connection between the production of lift and the subsequent induction of drag, but it does nothing except "induce" non critical thinkers into.

American Institute of Aeronautics and Astronautics Sunrise Valley Drive, Suite Reston, VA Evaporative cooling is the process where warm water from an industrial process is pumped up to the top of the cooling tower where the water distribution system is.

The water then gets distributed by cooling tower nozzles to the wet deck. At the same time, air is being drawn through the air-inlet louvers forcing water to evaporate.

This is observed, for instance, away from walls in jet-in-crossflow scramjet combustors, where diffusion flames burn in supersonic regions enveloping the fuel jet (see Figure 6b and Section ).

Further research on these aspects is warranted, including investigations of the influences of shocklets on the production of reaction by: For example, the jet/crossflow length scale is a measure for the distance over which a pure jet will intrude into a crossflow before it gets strongly deflected (or affected).

It should be noted that the length measures are only "order of magnitude"; pre- cise coefficients have to be determined from experi- ments or from more detailed flow analysis. Pressure Indicator FI FT FR FC Flow Recorder Level Controller Pressure Transmitter Pressure Recorder Crossflow Inducted Draft Packed Tower Tubular Screen Counterflow Boom Loader Forced Draft Chimney Tower Standard P&ID Symbols Legend | Industry Standardized P&ID Symbols.

Liu X, Katz J (). Measurements of pressure distribution in a cavity flow by integrating the material acceleration. Proceedings of the ASME Heat Transfer/Fluids Engineering Summer ConferenceHT/FED 3.

Yue W, Parlange MB, Meneveau C, Zhu W, Van Hout R, Katz J (). The result is!!£- = 27r a Uc b + 27r a2 Ua b sin 11 cas e (19) where a is of the same form as for a buoyant jet in stagnant ambient (Equation 6) and a2 is the crossflow induced entrainment coefficient.

Overview of Jet Integral Models Available for Mixing Zone Analysis A large number of jet integral models for submerged single port or. This volume comprises the proceedings of the 42nd National and 5th International Conference on Fluid Mechanics and Fluid Power held at IIT Kanpur in December, The conference proceedings encapsulate the best deliberations held during the conference.

The diversity of participation in the. Liu X, Katz J (). Measurements of pressure distribution in a cavity flow by integrating the material acceleration. Proceedings of the ASME Heat Transfer/Fluids Engineering Summer ConferenceHT/FED 3. Soranna F, Chow YC, Uzol O, Katz J ().

Rotor boundary layer response to an impinging wake. These proceedings primarily focus on advances in the theory, experiments, and numerical simulations of turbulence in the contexts of flow-induced vibration and noise, as well as their control.

Fluid-related structural vibration and noise problems are often encountered in many engineering fields. Boundary layer separation is the detachment of a boundary layer from the surface into a broader wake. Boundary layer separation occurs when the portion of the boundary layer closest to the wall or leading edge reverses in flow direction.

The separation point is defined as the point between the forward and backward flow, where the shear stress.

This banner text can have markup. web; books; video; audio; software; images; Toggle navigation. Gruber et al. 4 9 applied NO PLIF to study the instantaneous jet plume structure when gaseous fuel was injected into a Mach 2 non reacting crossflow with the aid of pylon Flet cher et al.

60 Hartfield et al. 61 used I 2 PLIF to measure the steady, non reacting compressible flow quantities density pressure, temperature and velocity. Numerical Investigation of The Crossflow Instabilities Induced by a Periodic Programme for the SIG workshop "Laminar-Turbulent Transition Mechanisms, Prediction and Control", June 17 - 20, Tuesday, June 19 LAMINAR-TURBULENT TRANSITION MECHANISMS, PREDICTION AND CONTROL A forced draught is where the air flow comes directly from the fan to the object.

Such as an hair dryer. An induced draught is where the air flow is induced {lit lead in} by a separate flow of air. UCI Combustion Laboratory The UCI Combustion Laboratory () has evolved through 30 years of research ranging from basic science to practical UCICL is housed in the Engineering Laboratory Facility in the Mechanical and Aerospace Engineering Complex.

The jet should supress shock-induced separation and delay buffet onset to higher AoA and to higher CL values. Pressure coefficient Cp on the model surface corresponding to the different jet intensities is shown in Figure 2.

One can see that the increase of a jet stagnation pressure moves the shock wave downstream and leads to a better CpTE. The type of crossflow within multi-jet systems can typically be characterized by crossflow of a defined free stream type flow or by a flow formed by the spent air from the impinging jets.

The strength of the crossflow within the impingement array is determined by the design of the outflow and by the associated routing of the spent air. The problem of multiple turbulent jet interactions is investigated with special attention to applications in kraft recovery boilers.

The phenomena due to turbulence are simulated with the k-ε turbulence model, and a multigrid numerical technique is applied to solve the time-averaged Navier-Stokes equations governing the flows. Investigations carried out include a study on the simulation of Cited by: 1. Journal Papers Book Chapter.

Pathak, B., Basu, S. and Kumar, R. Kumar, “Numerical simulation of high-pressure gas atomization of two-phase flow: Effect of gas pressure on droplet size distribution,” Advanced Powder Technology, “Dispersion and Vaporization of Biofuels and Conventional Fuels in a Crossflow Pre-mixer.

The University of Alberta Faculty of Engineering conducts leading-edge, interdisciplinary research and is awarded more than $65 million in research funding per year. Zhang, T.Q., Liu, W.C., and Guo, S. () “Improved Model for Contaminant Intrusion Induced by Negative Pressure Events in Water Distribution Systems”, ASCE Journal of.

For Reynolds number set atthe oscillating condition at the inlet engaged the jet into flapping. The jet showed a tendency to a permanent lean towards one side of the channel, for all used frequencies.

Flapping was more one-sided which led to a shift in the average Nusselt Author: Johnny Issa, Najib Saliba, Bchara Sidnawi. The initial stage of high-pressure induced beta-lactoglobulin aggregation: The long-run simulation; The onset of turbulence in pipe flow; The particle image velocimetry method in the study of the dynamics of phase transitions induced by high pressure in triolein and oleic acid.

The jets crossflow is drawn, by ( kW) air pressure blower (A),to the plenum (D). (CD), since the pressure drop is a combination of flow contraction in the impingement jet plate and the shear force induced due to friction take places within the and Text Book on Impingement Heat Transfer: Hollworth, B.R.

and Barry, R.D. V = 1, ft/sec RPM = 8, RV = 2 D = inches. Inserting these numbers into our equation, we have: This equals inches. From this, we subtract half the inlet diameter, which is is inches in our example.

So, – gives us the final length of inches. V-8 Intake Manifolds. So far, we have looked at the relatively. An exemplary engine noise reduction system, can be provided, which can include a noise reduction fluid source, and a microjet(s) placed at an axial location downstream from a nozzle exit of an engine and configured to asymmetrically inject a noise reduction fluid from the noise reduction fluid source into a jet flow of the engine.

The engine can be a jet engine.

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