Journal articles: 'Thin jet'

1

Gyulassy, M., P. Lévai, and I. Vitev. "Jet quenching in thin plasmas." Nuclear Physics A 661, no. 1-4 (December 1999): 637–40. http://dx.doi.org/10.1016/s0375-9474(99)85106-9.

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Minin, Vladilen F., Igor V. Minin, and Oleg V. Minin. "SHAPED CHARGES WITH THIN AND ULTRA-THIN FACINGS." Vestnik SSUGT (Siberian State University of Geosystems and Technologies) 26, no. 1 (2021): 133–42. http://dx.doi.org/10.33764/2411-1759-2021-26-1-133-142.

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The aim of the research is to study the formation of cumulative jets in charges with cumulative facings with a wall thickness of the order of the thickness of the jet-forming layer in classical charges. Based on mathematical modeling and experiments, it is shown that in such charges, the detonation products of explosives can play the role of an additional body that affects the axial velocity of the lin-ing throwing and leads to a collapse angle of more than 180 degrees. In this process, the mass of the jet is greater than the mass of the pestle. For the first time, corrugations were experimentally detected on the surface of the lining during its explosive compression. Corrugations may occur on the surface of the lining, leading to instability of the cumulative jet formation process. As a result of the study, it was found that the minimum wall thickness of the cladding is mainly determined by the instability of its surface (the appearance of corrugations on its surface).

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3

Weiss, Peter. "Thin Jet Flies Two for One." Science News 161, no. 9 (March 2, 2002): 133. http://dx.doi.org/10.2307/4013197.

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4

Halpern, B. L., J. J. Schmitt, J. W. Golz, Y. Di, and D. L. Johnson. "Gas jet deposition of thin films." Applied Surface Science 48-49 (January 1991): 19–26. http://dx.doi.org/10.1016/0169-4332(91)90302-z.

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5

German, Radoslav, and Roger E. Khayat. "Steady and transient thin-jet flow." Physics of Fluids 17, no. 10 (2005): 102104. http://dx.doi.org/10.1063/1.2103147.

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6

Pullin, D. I., and J. M. Simmons. "Stability of the thin-jet model of the unsteady jet flap." AIAA Journal 23, no. 7 (July 1985): 1118–20. http://dx.doi.org/10.2514/3.9046.

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7

Duchemin, Laurent. "Self-focusing of thin liquid jets." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 464, no. 2089 (October 23, 2007): 197–206. http://dx.doi.org/10.1098/rspa.2007.0068.

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The nonlinear evolution of an initially perturbed free surface perpendicularly accelerated, or of an initially flat free surface subject to a perturbed velocity profile, gives rise to the emergence of thin spikes of fluid. We are investigating the long-time evolution of a thin inviscid jet of this kind, subject or not to a body force acting in the direction of the jet itself. A fully nonlinear theory for the long-time evolution of the jet is given. In two dimensions, the curvature of the tip scales like t 3 , where t is time, and the peak undergoes an overshoot in acceleration which evolves like t −5 . In three dimensions, the jet evolves towards an axisymmetric shape, and the curvature and the overshoot in acceleration obey asymptotic laws in t 2 and t −4 , respectively. The asymptotic self-similar shape of the spike is found to be a hyperbola in two dimensions, a hyperboloid in three dimensions. Scaling laws and self-similarity are confronted with two-dimensional computations of the Richtmyer–Meshkov instability.

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8

Sasaki, Yoshi N., and Niklas Schneider. "Decadal Shifts of the Kuroshio Extension Jet: Application of Thin-Jet Theory*." Journal of Physical Oceanography 41, no. 5 (May 1, 2011): 979–93. http://dx.doi.org/10.1175/2011jpo4550.1.

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Abstract Meridional shifts of the Kuroshio Extension (KE) jet on decadal time scales are examined using a 1960–2004 hindcast simulation of an eddy-resolving ocean general circulation model for the Earth Simulator (OFES). The leading mode of the simulated KE represents the meridional shifts of the jet on decadal time scales with the largest southward shift in the early 1980s associated with the climate regime shift in 1976/77, a result confirmed with subsurface temperature observations. The meridional shifts originate east of the date line and propagate westward along the mean jet axis, a trajectory inconsistent with the traditionally used linear long Rossby waves linearized in Cartesian coordinates, although the phase speed is comparable to that in the traditional framework. The zonal scale of these westward propagation signals is about 4000 km and much larger than their meridional scale. To understand the mechanism for the westward propagation of the KE jet shifts, the authors consider the limit of a thin jet. This dynamic framework describes the temporal evolution of the location of a sharp potential vorticity front under the assumption that variations along the jet are small compared to variations normal to the jet in natural coordinates and is well suited to the strong jet and potential vorticity gradients of the KE. For scaling appropriate to the decadal adjustments in the KE, the thin-jet model successfully reproduces the westward propagations and decadal shifts of the jet latitude simulated in OFES. These results give a physical basis for the prediction of decadal variability in the KE.

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Sasaki, Yoshi N., and Niklas Schneider. "Decadal Shifts of the Kuroshio Extension Jet: Application of Thin-Jet Theory*." Journal of Physical Oceanography 41, no. 5 (May 2011): 979–93. http://dx.doi.org/10.1175/2010jpo4550.1.

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10

Khayat, Roger E., Michael A. N. Hanyk, and Moinuddin Ahmed. "A spectral approach to thin jet flow." Applied Numerical Mathematics 62, no. 9 (September 2012): 1187–96. http://dx.doi.org/10.1016/j.apnum.2010.11.006.

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11

Sivakumar, D., and B. N. Raghunandan. "A Study on Converging Thin Annular Jets." Journal of Fluids Engineering 119, no. 4 (December 1, 1997): 923–28. http://dx.doi.org/10.1115/1.2819518.

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An interesting feature of jets from liquid-liquid coaxial swirl atomizers used in bipropellant rockets or elsewhere is that the outer jet results in a tulip shaped liquid bulb even at operating pressure levels. In this context, experiments have been performed to study the discharge and tulip characteristics of annular jets through qualitative simulation of outer jet flow conditions at which tulip bulb prevails. It is shown that the discharge coefficient increases steeply with Reynolds number, a trend which is distinct from that of circular orifices. The range of flow conditions at which tulip bulb prevails decreases with the annular gap. If a swirl component is introduced into the annular jet, it alters the discharge characteristics and the tulip range with a tendency to form multiple tulips. Variation of tulip length for different annular gaps shows a common trend when plotted against liquid flow rate. The experimental data of tulip length agree reasonably with the theoretical model reported in literature.

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12

Sasaki, Yoshi N., Shoshiro Minobe, and Niklas Schneider. "Decadal Response of the Kuroshio Extension Jet to Rossby Waves: Observation and Thin-Jet Theory*." Journal of Physical Oceanography 43, no. 2 (February 1, 2013): 442–56. http://dx.doi.org/10.1175/jpo-d-12-096.1.

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AbstractThis study examines interannual to decadal variability of the Kuroshio Extension (KE) jet using satellite altimeter observations from 1993 to 2010. The leading empirical orthogonal function (EOF) mode of sea level variability in the KE region represents the meridional shift of the KE jet, followed by its strength changes with a few month lag. This shift of the KE jet lags atmospheric fluctuations over the eastern North Pacific by about three years. Broad sea level anomalies (SLAs) emerge in the eastern North Pacific 3–4 years before the upstream KE jet shift, and propagate westward along the KE jet axis. In the course of the propagation, the meridional scale of the SLAs gradually narrows, and their amplitude increases. This westward propagation of SLAs with a speed of about 5 cm s−1 is attributed to the westward propagation of the meridional shift of the jet, consistent with the thin-jet theory, whose importance has been suggested by previous numerical studies. In addition, the westward-propagating signals tend to conserve their quasigeostrophic potential vorticity anomaly, which may explain the characteristic changes of SLAs during the propagation. After the westward-propagating signals of positive (negative) SLAs reach at the east coast of Japan, the upstream KE jet strengthens (weakens) associated with the strength changes of the northern and southern recirculation gyres. Interestingly, this strength change of the KE jet propagates eastward with a speed of about 6 cm s−1, suggesting an importance of advection by the current.

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13

Li, Tsai Cheng, Rwei Ching Chang, and Y. C. Li. "Characterization of Conductive Thin Films Deposited by Ink Jet Printing." Applied Mechanics and Materials 284-287 (January 2013): 57–61. http://dx.doi.org/10.4028/www.scientific.net/amm.284-287.57.

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With the advantage of simplicity and low cost, ink jet printing has the potential to replace the traditional chemical and physical deposition technology in thin film fabrication. In this work, silver conductive thin films are deposited on glass and polyimide substrates by ink jet printing, where some major characteristics of the printed thin films are investigated and compared to those deposited by sputtering. The micro texture and residual stresses of the thin films are measured with X-ray diffractometry (XRD). Using thin film scratch tester, the adhesion of thin films deposited by both ink jet printing and sputtering is studied. Further observations on electric and optical performance by using visible wavelength photospectrometry, four-point probe, and surface profiler are also discussed. The result shows that the micro texture of the printed thin film behaves as good as the sputtered thin film. Furthermore, the micro scratch result illustrates that the adhesion of the printed thin film is even better than the sputtered thin film. It emphasizes that, after certain baking process, the ink jet printing has the possibility to replace sputtering in thin film deposition, especially for the polymer substrates.

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14

Imasaka, Totaro, Katsunori Tanaka, and Nobuhiko Ishibashi. "Thin-layer chromatography with supersonic jet fluorometric detection." Analytical Chemistry 62, no. 4 (February 15, 1990): 374–78. http://dx.doi.org/10.1021/ac00203a012.

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15

Paul, Kateri E., William S. Wong, Steven E. Ready, and Robert A. Street. "Additive jet printing of polymer thin-film transistors." Applied Physics Letters 83, no. 10 (September 8, 2003): 2070–72. http://dx.doi.org/10.1063/1.1609233.

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16

Scoutaris, Nikolaos, Martin Snowden, and Dennis Douroumis. "Taste masked thin films printed by jet dispensing." International Journal of Pharmaceutics 494, no. 2 (October 2015): 619–22. http://dx.doi.org/10.1016/j.ijpharm.2015.05.018.

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17

Li, Tsai-Cheng, Rwei-Ching Chang, and Yen-Choung Li. "INK JET PRINTED THIN FILMS ON GLASS AND POLYIMIDE SUBSTRATES." Transactions of the Canadian Society for Mechanical Engineering 37, no. 3 (September 2013): 873–83. http://dx.doi.org/10.1139/tcsme-2013-0074.

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Silver conductive thin films deposited on glass and polyimide substrates by using ink jet printing are studied in this work. Characterization of the printed thin films and comparison with sputtered films are investigated. The micro texture, residual stress, adhesion, hardness, optical reflectance, and electric resistance of the thin films are discussed. The result shows that the ink jet printing has the possibility to replace sputtering in thin film deposition, especially for the polymer substrates.

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18

Josserand, Christophe, Pascal Ray, and Stéphane Zaleski. "Droplet impact on a thin liquid film: anatomy of the splash." Journal of Fluid Mechanics 802 (August 10, 2016): 775–805. http://dx.doi.org/10.1017/jfm.2016.468.

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We investigate the dynamics of drop impact on a thin liquid film at short times in order to identify the mechanisms of splash formation. Using numerical simulations and scaling analysis, we show that it depends both on the inertial dynamics of the liquid and the cushioning of the gas. Two asymptotic regimes are identified, characterized by a new dimensionless number $J$: when the gas cushioning is weak, the jet is formed after a sequence of bubbles are entrapped and the jet speed is mostly selected by the Reynolds number of the impact. On the other hand, when the air cushioning is important, the lubrication of the gas beneath the drop and the liquid film controls the dynamics, leading to a single bubble entrapment and a weaker jet velocity.

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19

Piferi, Cecilia, Chiara Carra, Kateryna Bazaka, Hector Eduardo Roman, Elisa Camilla Dell’Orto, Vittorio Morandi, Igor Levchenko, and Claudia Riccardi. "Controlled Deposition of Nanostructured Hierarchical TiO2 Thin Films by Low Pressure Supersonic Plasma Jets." Nanomaterials 12, no. 3 (February 3, 2022): 533. http://dx.doi.org/10.3390/nano12030533.

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Plasma-assisted supersonic jet deposition (PA-SJD) is a precise technique for the fabrication of thin films with a desired nanostructured morphology. In this work, we used quadrupole mass spectrometry of the neutral species in the jet and the extensive characterization of TiO2 films to improve our understanding of the relationship between jet chemistry and film properties. To do this, an organo–metallic precursor (titanium tetra–isopropoxide or TTIP) was first dissociated using a reactive argon–oxygen plasma in a vacuum chamber and then delivered into a second, lower pressure chamber through a nozzle. The pressure difference between the two chambers generated a supersonic jet carrying nanoparticles of TiO2 in the second chamber, and these were deposited onto the surface of a substrate located few centimeters away from the nozzle. The nucleation/aggregation of the jet nanoparticles could be accurately tuned by a suitable choice of control parameters in order to produce the required structures. We demonstrate that high-quality films of up to several µm in thickness and covering a surface area of few cm2 can be effectively produced using this PA-SJD technique.

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Li, Shuang-Liang. "A thin disk model for the high efficiency jet in powerful lobe-dominated FRII radio galaxies." Proceedings of the International Astronomical Union 12, S324 (September 2016): 196–98. http://dx.doi.org/10.1017/s1743921317001375.

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AbstractWe propose a thin accretion disk with magnetically driven winds model to investigate the high jet efficiency phenomenon in lobe-dominated luminous FRII radio galaxies, which was reported by Fernandes et al. (2011) and Punsly (2011). It was found that the temperature of a thin disk with winds was much lower comparing with that of a standard thin disk because the winds take the most of energy released in the disk away, resulting in a much smaller raditive efficiency. Therefore, the jet efficiency can be very high even for conventional jet power. Our model can explain the observations quite well.

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21

Carra, Chiara, Elisa Dell’Orto, Vittorio Morandi, and Claudia Riccardi. "ZnO Nanostructured Thin Films via Supersonic Plasma Jet Deposition." Coatings 10, no. 8 (August 13, 2020): 788. http://dx.doi.org/10.3390/coatings10080788.

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Zinc Oxide nanostructured thin films were grown by a novel plasma assisted vapour deposition method, which aims to combine the versatility of deposition processes that are mediated by plasma with the capability to control particles diffusion and nucleation. For this purpose, the proposed approach spatially separates into two different vacuum chambers the creation of zinc oxide from a metalorganic precursor from the actual film growth, thanks to the extraction of a supersonic jet of plasma seeded by the precursor fragments. The characterization of the reactor in different plasma conditions has been carried out by means of optical emission spectroscopy (OES). ZnO films with different degrees of purity, thickness uniformity, as well as different morphologies can be obtained varying the deposition parameters. The samples profiles have been collected in order to evaluate deposition rates and films uniformity. The as-prepared as well as annealed thin films were characterized by attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) to evaluate their chemical composition and purity. According to Raman analyses, the annealed samples are high-purity wurtzite-type crystalline zinc oxide films. Atomic force microscopy (AFM) and scanning electron microscopy (SEM) confirm a surface morphology characterized by columnar structures.

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22

Gyulassy, M., P. Lévai, and I. Vitev. "Jet quenching in thin quark–gluon plasmas I: formalism." Nuclear Physics B 571, no. 1-2 (April 2000): 197–233. http://dx.doi.org/10.1016/s0550-3213(99)00713-0.

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23

Bai, Y., D. J. Vieira, J. M. Wouters, G. W. Butler, D. Rosenauer, K. E. G. Löbner, V. G. Lind, and D. R. Phillips. "A high-intensity thin-target He-jet production source." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 126, no. 1-4 (April 1997): 198–200. http://dx.doi.org/10.1016/s0168-583x(96)01074-9.

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24

Kwack, Young-Jin, and Woon-Seop Choi. "Electrohydrodynamic Jet Printed Indium–Zinc–Oxide Thin-Film Transistors." Journal of Display Technology 12, no. 1 (January 2016): 3–7. http://dx.doi.org/10.1109/jdt.2015.2441834.

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25

Ustin, S. A., K. A. Brown, and W. Ho. "An apparatus for supersonic jet epitaxy of thin films." Review of Scientific Instruments 71, no. 3 (March 2000): 1479–87. http://dx.doi.org/10.1063/1.1150484.

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Rebrov, Aleksei K., Rustam S. Sharafudinov, Andrey V. Shishkin, and Nikolai I. Timoshenko. "Free C2F4 Jet Deposition of Thin PTFE-like Films." Plasma Processes and Polymers 2, no. 6 (July 19, 2005): 464–71. http://dx.doi.org/10.1002/ppap.200400081.

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Beecher, P., P. Servati, A. Rozhin, A. Colli, V. Scardaci, S. Pisana, T. Hasan, et al. "Ink-jet printing of carbon nanotube thin film transistors." Journal of Applied Physics 102, no. 4 (August 15, 2007): 043710. http://dx.doi.org/10.1063/1.2770835.

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28

Yoshimori, Akira. "Horizontal Divergence Caused by Meanders of a Thin Jet." Journal of Physical Oceanography 24, no. 2 (February 1994): 345–52. http://dx.doi.org/10.1175/1520-0485(1994)024<0345:hdcbmo>2.0.co;2.

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29

INAMURA, Eijiro, Masaki ENDO, Yoko SAKAKIBARA, and Junjiro IWAMOTO. "2429 Deformation of Thin Circular Plate by Supersonic Jet." Proceedings of the JSME annual meeting 2007.1 (2007): 431–32. http://dx.doi.org/10.1299/jsmemecjo.2007.1.0_431.

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30

Kwack, Young-Jin, and Woon-Seop Choi. "Electrohydrodynamic Jet Spraying Technique for Oxide Thin-Film Transistor." IEEE Electron Device Letters 34, no. 1 (January 2013): 78–80. http://dx.doi.org/10.1109/led.2012.2226557.

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31

Ralph, E. A., and L. Pratt. "Predicting eddy detachment for an equivalent barotropic thin jet." Journal of Nonlinear Science 4, no. 1 (December 1994): 355–74. http://dx.doi.org/10.1007/bf02430638.

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32

Shutov, A. I., V. I. Potapov, and V. I. Agibalov. "Economical cooling modes in air-jet thin glass quenching." Glass and Ceramics 45, no. 12 (December 1988): 440–43. http://dx.doi.org/10.1007/bf00679764.

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33

Lawson, Nicholas J., and Malcolm R. Davidson. "Crossflow Characteristics of an Oscillating Jet in a Thin Slab Casting Mould." Journal of Fluids Engineering 121, no. 3 (September 1, 1999): 588–95. http://dx.doi.org/10.1115/1.2823509.

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The application of LDA to a transient 1/3 scale (500 mm wide) water model of a mould, typical of steel thin slab casting, is presented. The characteristics of a crossflow, associated with the oscillating jet emerging from a submerged nozzle (internal diameter 33 mm), were analyzed for a range of casting rates (0–2 m/min), nozzle submergences (20–120 mm) and nozzle-mould wall gap widths (0–21 mm). The frequency of oscillation was found to be primarily dependent on the casting rate of the system, independent of nozzle submergence or gap width, whereas the RMS crossflow velocity depended on all three parameters. Additional crossflow was also observed past the jet below the nozzle exit and this allowed the jet to oscillate even with zero gap width.

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34

Akiyama, Shinsaku, Yusuke Waki, Shinya Okino, and Hideshi Hanazaki. "Unstable jets generated by a sphere descending in a very strongly stratified fluid." Journal of Fluid Mechanics 867 (March 20, 2019): 26–44. http://dx.doi.org/10.1017/jfm.2019.123.

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The flow around a sphere descending at constant speed in a very strongly stratified fluid ($Fr\lesssim 0.2$) is investigated by the shadowgraph method and particle image velocimetry. Unlike the flow under moderately strong stratification ($Fr\gtrsim 0.2$), which supports a thin cylindrical jet, the flow generates an unstable jet, which often develops into turbulence. The transition from a stable jet to an unstable jet occurs for a sufficiently low Froude number $Fr$ that satisfies $Fr/Re<1.57\times 10^{-3}$. The Froude number $Fr$ here is in the range of $0.0157<Fr<0.157$ or lower, while the Reynolds number $Re$ is in the range of $10\lesssim Re\lesssim 100$ for which the homogeneous fluid shows steady and axisymmetric flows. Since the radius of the jet can be estimated by the primitive length scale of the stratified fluid, i.e. $l_{\unicode[STIX]{x1D708}}^{\ast }=\sqrt{\unicode[STIX]{x1D708}^{\ast }/N^{\ast }}$ or $l_{\unicode[STIX]{x1D708}}^{\ast }/2a^{\ast }=\sqrt{Fr/2Re}$, this predicts that the jet becomes unstable when it becomes thinner than approximately $l_{\unicode[STIX]{x1D708}}^{\ast }/2a^{\ast }=0.028$, where $N^{\ast }$ is the Brunt–Väisälä frequency, $a^{\ast }$ the radius of the sphere and $\unicode[STIX]{x1D708}^{\ast }$ the kinematic viscosity of the fluid. The instability begins when the boundary-layer thickness becomes thin, and the disturbances generated by shear instabilities would be transferred into the jet. When the flow is marginally unstable, two unstable states, i.e. a meandering jet and a turbulent jet, can appear. The meandering jet is thin with a high vertical velocity, while the turbulent jet is broad with a much smaller velocity. The meandering jet may persist for a long time, or develop into a turbulent jet in a short time. When the instability is sufficiently strong, only the turbulent jet could be observed.

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Cheng, P. J., and H. Y. Lai. "Nonlinear Stability Analysis of Thin Film Flow from a Liquid Jet Impinging on a Circular Concentric Disk." Journal of Mechanics 22, no. 2 (June 2006): 115–24. http://dx.doi.org/10.1017/s172771910000441x.

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AbstractThe paper investigates the stability of thin film flow from a liquid jet impinging on a circular concentric disk using a long-wave perturbation method to solve for the generalized nonlinear kinematic equations of free film interface. To begin with a normal mode approach is employed to obtain the linear stability solution for the film flow. In the linear stability solutions only subcritical region can be resolved. In other words, no solution of supercritical region can be obtained in linear domain. Furthermore, the role that the forces of gravitation and surface tension play in the flow is nothing but to stabilize the system. To further investigate the realistic impinging jet flow stability conditions, the weak nonlinear dynamics of a film flow is studied by using the method of multiple scales. Various subcritical nonlinear behaviors expressed in terms of absolute stability, conditional stability and explosive instability can be characterized by solving the Ginzburg-Landau equation. It is found that the jet flow will become relatively unstable for an increasing Reynolds number, a relative smaller distance from the center of the impinging jet on the disk and a smaller diameter of the exit jet. It is also concluded that the flow will always stay in a subcritical instability region if the characteristic diameter of the potential core at nozzle exit is less than 0.01mm for the numerical conditions given in this paper. In such a case when the amplitude of external flow disturbance is smaller than the threshold amplitude a stable jet flow can be ensured.

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Fresco, A. Y., J. A. Fernández-Ontiveros, M. A. Prieto, J. A. Acosta-Pulido, and A. Merloni. "Low optical polarization at the core of the optically thin jet of M87." Monthly Notices of the Royal Astronomical Society 496, no. 2 (June 8, 2020): 2204–12. http://dx.doi.org/10.1093/mnras/staa1566.

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ABSTRACT We study the optical linear and circular polarization in the optically thin regime of the core and jet of M87. Observations were acquired two days before the Event Horizon Telescope (EHT) campaign in early 2017 April. A high degree (∼20 per cent) of linear polarization (Plin) is detected in the bright jet knots resolved at $\sim 10\,\mathrm{ to}\,23\, \rm {arcsec}$ ($0.8{-}1.8\, \rm {kpc}$) from the centre, whereas the nucleus and inner jet show Plin ≲ 5 per cent. The position angle of the linear polarization shifts by ∼90° from each knot to the adjacent ones, with the core angle perpendicular to the first knot. The nucleus was in a low level of activity (Plin ∼ 2–3 per cent), and no emission was detected from HST-1. No circular polarization was detected either in the nucleus or the jet above a 3 σ level of Pcirc ≤ 1.5 per cent, discarding the conversion of Plin into Pcirc. A disordered magnetic field configuration or a mix of unresolved knots polarized along axes with different orientations could explain the low Plin. The latter implies a smaller size of the core knots, in line with current interferometric observations. Polarimetry with EHT can probe this scenario in the future. A steep increase of both Plin and Pcirc with increasing frequency is expected for the optically thin domain, above the turnover point. This work describes the methodology to recover the four Stokes parameters using a λ/4 waveplate polarimeter.

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TESHIMA, Koji. "Generation of a thin plate jet by a rectangular orifice." SHINKU 30, no. 5 (1987): 399–401. http://dx.doi.org/10.3131/jvsj.30.399.

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38

Narimisa, Mehrnoush, František Krčma, Yuliia Onyshchenko, Zdenka Kozáková, Rino Morent, and Nathalie De Geyter. "Atmospheric Pressure Microwave Plasma Jet for Organic Thin Film Deposition." Polymers 12, no. 2 (February 6, 2020): 354. http://dx.doi.org/10.3390/polym12020354.

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In this work, the potential of a microwave (MW)-induced atmospheric pressure plasma jet (APPJ) in film deposition of styrene and methyl methacrylate (MMA) precursors is investigated. Plasma properties during the deposition and resultant coating characteristics are studied. Optical emission spectroscopy (OES) results indicate a higher degree of monomer dissociation in the APPJ with increasing power and a carrier gas flow rate of up to 250 standard cubic centimeters per minute (sccm). Computational fluid dynamic (CFD) simulations demonstrate non-uniform monomer distribution near the substrate and the dependency of the deposition area on the monomer-containing gas flow rate. A non-homogeneous surface morphology and topography of the deposited coatings is also observed using atomic force microscopy (AFM) and SEM. Coating chemical analysis and wettability are studied by XPS and water contact angle (WCA), respectively. A lower monomer flow rate was found to result in a higher C–O/C–C ratio and a higher wettability of the deposited coatings.

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Flierl, Glenn R. "Thin jet and contour dynamics models of Gulf Stream meandering." Dynamics of Atmospheres and Oceans 29, no. 2-4 (July 1999): 189–215. http://dx.doi.org/10.1016/s0377-0265(99)00006-8.

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40

Park, Dong-Wha, and Jong-Sun Yun. "Structural characterization of diamond thin films prepared by plasma jet." Thin Solid Films 345, no. 1 (May 1999): 60–66. http://dx.doi.org/10.1016/s0040-6090(99)00072-3.

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41

Guilly, J., and M. Pennaneach. "Thin layers obtained by plasma jet deposition at low pressure." Applied Surface Science 36, no. 1-4 (January 1989): 170–76. http://dx.doi.org/10.1016/0169-4332(89)90911-2.

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42

Fan, Rong, Dong Chan Kim, Sung Hee Jung, Jae Ho Um, Wan In Lee, and Chee Won Chung. "Characterization of CuInS2 thin films prepared by aerosol jet deposition." Thin Solid Films 521 (October 2012): 123–27. http://dx.doi.org/10.1016/j.tsf.2012.02.038.

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Chun Huang, Wen-Tung Hsu, Chi-Hung Liu, Shin-Yi Wu, Shih-Hsien Yang, Tai-Hung Chen, and Ta-Chin Wei. "Low-Temperature Atmospheric-Pressure-Plasma Jet for Thin-Film Deposition." IEEE Transactions on Plasma Science 37, no. 7 (July 2009): 1127–28. http://dx.doi.org/10.1109/tps.2008.2011636.

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Badalov, Shai, and Christopher J. Arnusch. "Ink-jet printing assisted fabrication of thin film composite membranes." Journal of Membrane Science 515 (October 2016): 79–85. http://dx.doi.org/10.1016/j.memsci.2016.05.046.

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Bolotnova, R. Kh, and V. A. Korobchinskaya. "Boiling water jet outflow from a thin nozzle: spatial modeling." Thermophysics and Aeromechanics 24, no. 5 (September 2017): 761–71. http://dx.doi.org/10.1134/s0869864317050110.

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Kim, Dongjo, Youngmin Jeong, Chang Young Koo, Keunkyu Song, and Jooho Moon. "Thin Film Transistors with Ink-Jet Printed Amorphous Oxide Semiconductors." Japanese Journal of Applied Physics 49, no. 5 (May 20, 2010): 05EB06. http://dx.doi.org/10.1143/jjap.49.05eb06.

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Benedikt, J., V. Raballand, A. Yanguas-Gil, K. Focke, and A. von Keudell. "Thin film deposition by means of atmospheric pressure microplasma jet." Plasma Physics and Controlled Fusion 49, no. 12B (November 19, 2007): B419—B427. http://dx.doi.org/10.1088/0741-3335/49/12b/s39.

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Arias, A. C., S. E. Ready, R. Lujan, W. S. Wong, K. E. Paul, A. Salleo, M. L. Chabinyc, et al. "All jet-printed polymer thin-film transistor active-matrix backplanes." Applied Physics Letters 85, no. 15 (October 11, 2004): 3304–6. http://dx.doi.org/10.1063/1.1801673.

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Burgess, B. H. "Thin-jet scaling in large-scale shallow water quasigeostrophic flow." Geophysical & Astrophysical Fluid Dynamics 114, no. 4-5 (July 17, 2020): 481–503. http://dx.doi.org/10.1080/03091929.2020.1788013.

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ENDO, Masaki, Eijiro INAMURA, Yoko SAKAKIBARA, and Junjiro IWAMOTO. "Impingement of Underexpanded Jet on Elastic Thin Plate(Fluids Engineering)." Transactions of the Japan Society of Mechanical Engineers Series B 75, no. 757 (2009): 1774–80. http://dx.doi.org/10.1299/kikaib.75.757_1774.

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Journal articles on the topic 'Thin jet'

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