Abstract:An investigation of the possibility of controlling the evolution of jets into the far field is presented. Driven by practical concerns the study examined a highly turbulent jet flow. To enhance controllability of the flow evolution the virtues of non-circular nozzles and active flow excitation were combined. The study examined an air jet, Reae = 8ooo, average turbulence intensity 1.8% issuing into stagnant room air out of a triangular nozzle, which had piezoceramic actuators mounted on the flat sides. The evol… Show more
“…More recently, strong instabilities of a jet column were observed when a square jet was forced using azimuthal modes excitation effected via amplitude modulation, although detailed analysis about the effects of nozzle geometry on the jet dynamics was not provided (Wiltse and Glezer 1993). In later work, spatial mode excitation had been implemented on triangular jets and elliptic jets with various initial velocity profiles (Vandsburger and Ding 1995;Ding 1995). It was shown that the initial velocity profiles have significant influence on the effects of such combined excitations in terms of the flow characteristics associated with nozzle geometry.…”
Section: Mixing Control Methodsmentioning
confidence: 99%
“…(Sforza et al 1966, Trentacoste & Sforza 1967. Later studies of jets emerging from noncircular nozzles with corners showed that the introduction of sharp corners in the nozzle can increase significantly the fine-scale turbulence at the corners relative to the flat segments of the nozzle (Schadow et al 1988, Toyoda & Hussain 1989 and enhance mass entrainment (Vandsburger & Ding 1995). In some cases, the small-scale turbulence was produced by threedimensional flows, which were formed at the corner regions inside the nozzle (Su & Friedrich 1994).…”
Section: Outline Of the Thesismentioning
confidence: 99%
“…rectangular (Sfeir 1975, Husain & Hussain 1983, Quinn 1989, Austin 1992, square (Quinn 1992, Grinstein et al 1995, Vandsburger & Ding 1995, triangular (Schadow et al 1990, Mi et al 2000, lobed (Wang et al 2001, Zaman 1994 and elliptic (Dhanak & Debernardinis 1981, Ho & Gutmark 1987. Koshigoe et al (1989) conducted linear stability analysis on different initial conditions that might promote the non-uniform growth behavior underlying axis switching.…”
The present research focuses on the studies of the transitional stage of jets and plumes. It can be generally divided into two parts, namely, starting jets and starting forced plumes. The first part attempts to improve the understanding of the vortex dynamics in starting jets and to examine the differences between that of the circular jets and square jets. Based on the qualitative (via PLIF) and quantitative results obtained (via PIV), it was found that streamwise vortices generated at the corners of the square nozzle interacted with the primary vortices. The interactions had altered the downstream flow characteristics tremendously. Vortex pinch-off, leapfrogging, coalescence and axis-switching were observed in starting square jets and the mechanisms were analyzed. For starting forced plume, Boussinesq and non-Boussinesq cases had been investigated analytically and experimentally. An analytical model for the starting forced plume covering the entire range of jet-like, transitional and plume-like had been developed based on the understanding Wang & Law (2002) for forced plumes. The velocity ratio between the head vortex and the trailing buoyant jet was derived to vary from the jet-like to plume-like phases. The transitional changes for this ratio had also been quantified. Experimental results verified the analytical model. The quantative PIV results showed disorder behaviors in the near-field region for the non-Boussinesq cases (15% ∆ >). Virtual origin correction approach was utilized to compensate the non-Boussinesq effects.
“…More recently, strong instabilities of a jet column were observed when a square jet was forced using azimuthal modes excitation effected via amplitude modulation, although detailed analysis about the effects of nozzle geometry on the jet dynamics was not provided (Wiltse and Glezer 1993). In later work, spatial mode excitation had been implemented on triangular jets and elliptic jets with various initial velocity profiles (Vandsburger and Ding 1995;Ding 1995). It was shown that the initial velocity profiles have significant influence on the effects of such combined excitations in terms of the flow characteristics associated with nozzle geometry.…”
Section: Mixing Control Methodsmentioning
confidence: 99%
“…(Sforza et al 1966, Trentacoste & Sforza 1967. Later studies of jets emerging from noncircular nozzles with corners showed that the introduction of sharp corners in the nozzle can increase significantly the fine-scale turbulence at the corners relative to the flat segments of the nozzle (Schadow et al 1988, Toyoda & Hussain 1989 and enhance mass entrainment (Vandsburger & Ding 1995). In some cases, the small-scale turbulence was produced by threedimensional flows, which were formed at the corner regions inside the nozzle (Su & Friedrich 1994).…”
Section: Outline Of the Thesismentioning
confidence: 99%
“…rectangular (Sfeir 1975, Husain & Hussain 1983, Quinn 1989, Austin 1992, square (Quinn 1992, Grinstein et al 1995, Vandsburger & Ding 1995, triangular (Schadow et al 1990, Mi et al 2000, lobed (Wang et al 2001, Zaman 1994 and elliptic (Dhanak & Debernardinis 1981, Ho & Gutmark 1987. Koshigoe et al (1989) conducted linear stability analysis on different initial conditions that might promote the non-uniform growth behavior underlying axis switching.…”
The present research focuses on the studies of the transitional stage of jets and plumes. It can be generally divided into two parts, namely, starting jets and starting forced plumes. The first part attempts to improve the understanding of the vortex dynamics in starting jets and to examine the differences between that of the circular jets and square jets. Based on the qualitative (via PLIF) and quantitative results obtained (via PIV), it was found that streamwise vortices generated at the corners of the square nozzle interacted with the primary vortices. The interactions had altered the downstream flow characteristics tremendously. Vortex pinch-off, leapfrogging, coalescence and axis-switching were observed in starting square jets and the mechanisms were analyzed. For starting forced plume, Boussinesq and non-Boussinesq cases had been investigated analytically and experimentally. An analytical model for the starting forced plume covering the entire range of jet-like, transitional and plume-like had been developed based on the understanding Wang & Law (2002) for forced plumes. The velocity ratio between the head vortex and the trailing buoyant jet was derived to vary from the jet-like to plume-like phases. The transitional changes for this ratio had also been quantified. Experimental results verified the analytical model. The quantative PIV results showed disorder behaviors in the near-field region for the non-Boussinesq cases (15% ∆ >). Virtual origin correction approach was utilized to compensate the non-Boussinesq effects.
“…The sharp corners lead to the generation of high-frequency turbulent eddies, and the edges shed large-scale coherent structures, thus resulting in higher spread along the edge than that along vertex [9]. The small-and large-scale mixing is essential in combustion systems [10], and to improve the entrainment rate [11]. Further, the triangular jets introduce ''high-instability modes into the flow via the non-symmetric mean velocity and pressure distribution around the nozzle'' as discussed by Schadow et al [12].…”
Flow visualization studies using shadowgraph technique are carried out to investigate the shock evolution from non-circular slot jets at various under-expansion levels. The non-circular topologies considered are triangular, square and elliptic, and the circular jet is taken as the baseline case for the study. These jets are underexpanded in the pressure ratio (R) range of 2-6 corresponding to a fully expanded jet Mach number up to 1.85. Results indicate that the shock cell structures of non-circular jets strongly depend upon the initial shape of the topology. The shock structures of triangular jet have additional secondary oblique shocks that are distinct from those of other non-circular jets. Mach disk is almost absent in a shock cell structure of triangular jet, which is unlike the case of other jets used in the study. The study suggests that square jet undergoes faster diffusion process compared with the triangular jet. Axis-switching phenomenon is predicted for the elliptical jet at a distance of 3-7 equivalent diameters.
“…One point that is not fully investigated in previous studies is the e¨ect of corner radii in noncircular jets and this point is indicated to be a further research topic by Quinn [4]. The existence of sharp corners in the nozzle can increase the ¦ne-scale turbulence at the corners relative to the §at segments of the nozzle as indicated in [5,6], and enhance mass entrainment signi¦cantly in [7].…”
Experimental investigation of the turbulent §ow ¦eld of jets emanating from circular and curved-edged noncircular nozzles is conducted using hotwire anemometry. Distributions of the mean velocity vector are obtained by traversing a triple-sensor hot-wire probe at varying streamwise locations downstream of the jet exit plane in a low-speed free-jet facility. Measurements are obtained for a baseline circular nozzle (round jet) and for equilateral triangular and square nozzles. The data are used to compare the structure of the §ow ¦eld within these jets such as their mean velocity, turbulent kinetic energy, and entrainment levels. Axis rotation phenomenon is also investigated for noncircular nozzles, and it was not observed up to a streamwise location of 10d (d is the nozzle equivalent diameter, equals to 40 mm) for noncircular nozzles.
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