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1

Peregrine, D. H., and C. J. Chapman. "High Speed Flow." Mathematical Gazette 85, no. 504 (November 2001): 569. http://dx.doi.org/10.2307/3621821.

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2

Bryanston-Cross, P. J. "High speed flow visualisation." Progress in Aerospace Sciences 23, no. 2 (January 1986): 85–104. http://dx.doi.org/10.1016/0376-0421(86)90001-1.

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3

Wahab, Norfariza, Hiroyuki Sasahara, Shinnosuke Baba, Yuta Hirastuka, and Takashi Nakamura. "Development of High-speed Shearing Method to Obtain Flow Stress under High Strain Rate." International Journal of Modeling and Optimization 5, no. 2 (April 2015): 140–44. http://dx.doi.org/10.7763/ijmo.2015.v5.450.

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4

Schönteich, Bernward, Elisabeth Stammen, and Klaus Dilger. "High-speed Mass Flow Measurement in Highly ViscousAdhesives by Constant Temperature Anemometry." Journal of The Adhesion Society of Japan 51, s1 (2015): 269–73. http://dx.doi.org/10.11618/adhesion.51.269.

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5

OZAWA, Satoru. "Flow visualization in high speed trains." JOURNAL OF THE FLOW VISUALIZATION SOCIETY OF JAPAN 5, no. 19 (1985): 360–64. http://dx.doi.org/10.3154/jvs1981.5.360.

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6

Warren, Eric S., Julius E. Harris, and H. A. Hassan. "Transition model for high-speed flow." AIAA Journal 33, no. 8 (August 1995): 1391–97. http://dx.doi.org/10.2514/3.12687.

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7

Elsner, Markus. "High-speed imaging in a flow." Nature Biotechnology 30, no. 9 (September 2012): 841. http://dx.doi.org/10.1038/nbt.2366.

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8

Baker, Chris. "The flow around high speed trains." Journal of Wind Engineering and Industrial Aerodynamics 98, no. 6-7 (June 2010): 277–98. http://dx.doi.org/10.1016/j.jweia.2009.11.002.

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9

Singh, Narendra, and Thomas E. Schwartzentruber. "Aerothermodynamic correlations for high-speed flow." Journal of Fluid Mechanics 821 (May 25, 2017): 421–39. http://dx.doi.org/10.1017/jfm.2017.195.

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Heat flux and drag correlations are developed for high-speed flow over spherical geometries that are accurate for any Knudsen number ranging from continuum to free-molecular conditions. A stagnation point heat flux correlation is derived as a correction to the continuum (Fourier model) heat flux and also reproduces the correct heat flux in the free-molecular limit by use of a bridging function. In this manner, the correlation can be combined with existing continuum correlations based on computational fluid dynamics simulations, yet it can now be used accurately in the transitional and free-molecular regimes. The functional form of the stagnation point heat flux correlation is physics based, and was derived via the Burnett and super-Burnett equations in a recent article, Singh & Schwartzentruber (J. Fluid Mech., vol. 792, 2016, pp. 981–996). In addition, correlation parameters from the literature are used to construct simple expressions for the local heat flux around the sphere as well as the integrated drag coefficient. A large number of direct simulation Monte Carlo calculations are performed over a wide range of conditions. The computed heat flux and drag data are used to validate the correlations and also to fit the correlation parameters. Compared to existing continuum-based correlations, the new correlations will enable engineering analysis of flight conditions at higher altitudes and/or smaller geometry radii, useful for a variety of applications including blunt body planetary entry, sharp leading edges, low orbiting satellites, meteorites and space debris.
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10

Lu, Frank K., Qin Li, and Chaoqun Liu. "Microvortex generators in high-speed flow." Progress in Aerospace Sciences 53 (August 2012): 30–45. http://dx.doi.org/10.1016/j.paerosci.2012.03.003.

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11

Holyoake, Alex J., and Jim N. McElwaine. "High-speed granular chute flows." Journal of Fluid Mechanics 710 (August 31, 2012): 35–71. http://dx.doi.org/10.1017/jfm.2012.331.

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AbstractThis paper reports experimental findings on the flow of sand down a steep chute. Nearly all granular flow models have a maximum value for the friction and therefore predict that flows on steep slopes will accelerate at a constant rate until the interaction with the ambient fluid becomes important. This prediction has not been tested by previous work, which has focused on relatively low slope angles where steady, fully developed flows occur after short distances. We test this by investigating flows over a much greater range of slope angles (30–50${}^{\ensuremath{\circ} } $) and flow depths (4–130 particle diameters). We examine flows with two basal conditions, one flat and frictional, the other bumpy. The latter imposes a no-slip condition for slow, deep flows, but permits some degree of slip for high flow velocities. The data suggests that friction can be much larger than theories such as the $\ensuremath{\mu} (I)$ rheology proposed by Jop, Forterre & Pouliquen (Nature, vol. 441, 2006) suggest and that there may be constant velocity states above the angle of vanishing ${h}_{\mathit{stop}} $. Although these flows do not vary in time, all but the flows on the bumpy base at low inclinations accelerate down the slope. A recirculation mechanism sustains flows with a maximum mass flux of $20~\mathrm{kg} ~{\mathrm{s} }^{\ensuremath{-} 1} $, allowing observations to be made at multiple points for each flow for an indefinite period. Flows with Froude number in the range 0.1–25 and bulk inertial number 0.1–2.7 were observed in the dense regime, with surface velocities in the range 0.2–5.6 $\mathrm{m} ~{\mathrm{s} }^{\ensuremath{-} 1} $. Previous studies have focused on $I\lessapprox 0. 5$. We show that a numerical implementation of the $\ensuremath{\mu} (I)$ rheology does not fully capture the accelerating dynamics or the transverse velocity profile on the bumpy base. We also observe the transverse separation of the flow into a dense core flanked by dilute regions and the formation of longitudinal vortices.
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12

Solomon, John T., Rajan Kumar, and Farrukh S. Alvi. "High-Bandwidth Pulsed Microactuators for High-Speed Flow Control." AIAA Journal 48, no. 10 (October 2010): 2386–96. http://dx.doi.org/10.2514/1.j050405.

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13

McDaniel, R. D., R. P. Nance, and H. A. Hassan. "Transition Onset Prediction for High-Speed Flow." Journal of Spacecraft and Rockets 37, no. 3 (May 2000): 304–9. http://dx.doi.org/10.2514/2.3579.

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14

TANAKA, Kenichi, and Junjiro IWAMOTO. "A Study on High-Speed Pulsating Flow." Proceedings of Conference of Hokkaido Branch 2003.43 (2003): 52–53. http://dx.doi.org/10.1299/jsmehokkaido.2003.43.52.

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15

Browning, D. W. "Flow control in high-speed communication networks." IEEE Transactions on Communications 42, no. 7 (July 1994): 2480–89. http://dx.doi.org/10.1109/26.297859.

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16

Leonov, Sergey B., Dmitry A. Yarantsev, Anatoly P. Napartovich, and Igor V. Kochetov. "Plasma-Assisted Chemistry in High-Speed Flow." Plasma Science and Technology 9, no. 6 (December 2007): 760–65. http://dx.doi.org/10.1088/1009-0630/9/6/29.

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17

AMARATUNGA, S. R., O. R. TUTTY, and G. T. ROBERTS. "High-speed flow with discontinuous surface catalysis." Journal of Fluid Mechanics 420 (October 10, 2000): 325–59. http://dx.doi.org/10.1017/s0022112000001610.

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In a reacting gas flow both gas-phase chemical activity and surface catalysis can increase the rate of heat transfer from the gas to a solid surface. In particular, when there is a discontinuous change in the catalytic properties of the surface, there can be a very large increase in the local heat transfer rate. In this study numerical simulations have been performed for the laminar high-speed flow of a high-temperature, non-equilibrium reacting gas mixture over a flat plate. The surface of the plate is partly catalytic, with the leading region non-catalytic, and a discontinuous change in the catalytic properties of the surface at the catalytic junction. The surface is assumed to be isothermal, and cold relative to the free stream. The gas is assumed to be a mixture of molecular and atomic forms of a diatomic gas in an inert gas forming a thermal bath, giving a three-species mixture with dissociation and recombination of the reactive species. The calculations are performed for a gas with atomic and molecular oxygen in an argon bath, but a full range of gas-phase chemical and surface catalytic effects is considered. Kinetic schemes with frozen gas-phase chemistry, and partial or full recombination of atomic oxygen in the boundary layer are investigated. The catalytic nature of the surface material is given by a catalytic recombination rate coeffcient, which varies from zero (non-catalytic) to one (fully catalytic), and the effects on the flow and the surface heat transfer of materials which are non-, partially, or fully catalytic are considered. A self-similar thin-layer analytical model of the change in the gas composition downstream of the catalytic junction is developed. For physically realistic (O(10−2)) values of the catalytic recombination rate coeffcient, the predictions from this model of the surface values of the atomic oxygen mass fraction and the catalytic surface heat transfer rate are excellent when the only change in the composition of the gas comes from the surface catalysis, and reasonable when there is partial recombination of the gas in the boundary layer due to the gas-phase chemistry. In contrast, when the surface is fully catalytic, the streamwise diffusion terms play a significant role, and the model is not valid. These results should apply to other situations with an attached boundary layer with recombination reactions. A comparison is made between the calculated and experimental measurements of the heat transfer rate at the catalytic junction. With a kinetic scheme which allows partial recombination in the boundary layer, good agreement is found between the experimental and predicted values for surface materials which are essentially non-catalytic. For a catalytic material (platinum), the experimental and numerical heat transfer rates are matched to estimate the value of the catalytic recombination rate coeffcient. The values obtained show a considerable amount of scatter, but are consistent with those found in the literature.
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18

Zhang, Chao-Xuan, and Andreas Manz. "High-Speed Free-Flow Electrophoresis on Chip." Analytical Chemistry 75, no. 21 (November 2003): 5759–66. http://dx.doi.org/10.1021/ac0345190.

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19

Johansen, Geir Anton, Uwe Hampel, and Bjørn Tore Hjertaker. "Flow imaging by high speed transmission tomography." Applied Radiation and Isotopes 68, no. 4-5 (April 2010): 518–24. http://dx.doi.org/10.1016/j.apradiso.2009.09.004.

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20

Ahmed, Diyar I., M. Z. Yusoff, Al-Falahi Amir, and S. Kasolang. "High Speed Flow Characteristics in Gun Tunnel." Procedia Engineering 41 (2012): 1787–93. http://dx.doi.org/10.1016/j.proeng.2012.07.384.

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21

Snyder, Ray, and Lambertus Hesselink. "High speed optical tomography for flow visualization." Applied Optics 24, no. 23 (December 1, 1985): 4046. http://dx.doi.org/10.1364/ao.24.004046.

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22

Maki, Kevin J., Lawrence J. Doctors, Robert F. Beck, and Armin W. Troesch. "Transom-stern flow for high-speed craft." Australian Journal of Mechanical Engineering 3, no. 2 (January 2006): 191–99. http://dx.doi.org/10.1080/14484846.2006.11464508.

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23

Lerario, Giovanni, Dario Ballarini, Antonio Fieramosca, Alessandro Cannavale, Armando Genco, Federica Mangione, Salvatore Gambino, et al. "High-speed flow of interacting organic polaritons." Light: Science & Applications 6, no. 2 (September 5, 2016): e16212-e16212. http://dx.doi.org/10.1038/lsa.2016.212.

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24

Golan, Lior, Daniella Yeheskely-Hayon, Limor Minai, and Dvir Yelin. "High-speed interferometric spectrally encoded flow cytometry." Optics Letters 37, no. 24 (December 11, 2012): 5154. http://dx.doi.org/10.1364/ol.37.005154.

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25

Nayak, Krishna S., Bob S. Hu, and Dwight G. Nishimura. "Rapid quantitation of high-speed flow jets." Magnetic Resonance in Medicine 50, no. 2 (July 17, 2003): 366–72. http://dx.doi.org/10.1002/mrm.10538.

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26

Groléat, Tristan, Sandrine Vaton, and Matthieu Arzel. "High-speed flow-based classification on FPGA." International Journal of Network Management 24, no. 4 (June 5, 2014): 253–71. http://dx.doi.org/10.1002/nem.1863.

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27

TOYODA, Kento, Yutaka ABE, Akiko KANEKO, Shun ANZAI, Tomohisa YUASA, Bunki KAWANO, and Tomoichiro TAMURA. "Droplet Flow Behavior of High-speed Spray Flow with Condensation." Proceedings of Conference of Kanto Branch 2018.24 (2018): OS0602. http://dx.doi.org/10.1299/jsmekanto.2018.24.os0602.

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28

OIKAWA, Manabu, Kento TOYODA, Tomohisa YUASA, Akihiro FUTSUTA, Akiko KANEKO, Yutaka ABE, and Bunki KAWANO. "Flow Behavior of High Speed Droplet Spray Flow with Condensation." Proceedings of Conference of Kanto Branch 2019.25 (2019): 19B19. http://dx.doi.org/10.1299/jsmekanto.2019.25.19b19.

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29

MIYABE, Masahiro. "The internal flow of high specific speed mixed-flow pump." Proceedings of Conference of Kansai Branch 2002.77 (2002): _6–45_—_6–46_. http://dx.doi.org/10.1299/jsmekansai.2002.77._6-45_.

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30

Zhang, LingQian, ZhenXing Liu, ZhiWei Ma, W. Baumjohann, M. W. Dunlop, GuangJun Wang, Xiao Wang, H. Reme, and C. Carr. "Convective high-speed flow and field-aligned high-speed flows explored by TC-1." Science Bulletin 53, no. 15 (August 2008): 2371–75. http://dx.doi.org/10.1007/s11434-008-0324-3.

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31

Azarova, Olga A. "High Speed Flows." Fluids 8, no. 4 (March 24, 2023): 109. http://dx.doi.org/10.3390/fluids8040109.

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32

PANARAS, ARGYRIS G., and DIMITRIS DRIKAKIS. "High-speed unsteady flows around spiked-blunt bodies." Journal of Fluid Mechanics 632 (July 27, 2009): 69–96. http://dx.doi.org/10.1017/s0022112009006235.

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This paper presents a detailed investigation of unsteady supersonic and hypersonic flows around spiked-blunt bodies, including the investigation of the effects of the flow field initialization on the flow results. Past experimental research has shown that if the geometry of a spiked-blunt body is such that a shock formation consisting of an oblique foreshock and a bow aftershock appears, then the flow may be unsteady. The unsteady flow is characterized by periodic radial inflation and collapse of the conical separation bubble formed around the spike (pulsation). Beyond a certain spike length the flow is ‘stable’, i.e. steady or mildly oscillating in the radial direction. Both unsteady and ‘stable’ conditions have been reported when increasing or decreasing the spike length during an experimental test and, additionally, hysteresis effects have been observed. The present study reveals that for certain geometries the numerically simulated flow depends strongly on the assumed initial flow field, including the occurrence of bifurcations due to inherent hysteresis effects and the appearance of unsteady flow modes. Computations using several different configurations reveal that the transient (initial) flow development corresponds to a nearly inviscid flow field characterized by a foreshock–aftershock interaction. When the flow is pulsating, the further flow development is not sensitive to initial conditions, whereas for an oscillating or almost ‘steady’ flow, the flow development depends strongly on the assumed initial flow field.
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33

Fořt, Ivan, Pavel Seichter, Luboš Pešl, František Rieger, and Tomáš Jirout. "BLENDING CHARACTERISTICS OF HIGH-SPEED ROTARY IMPELLERS." Chemical and Process Engineering 34, no. 4 (December 1, 2013): 427–34. http://dx.doi.org/10.2478/cpe-2013-0035.

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Abstract This paper presents a comparison of the blending efficiency of eight high-speed rotary impellers in a fully baffled cylindrical vessel under the turbulent flow regime of agitated charge. Results of carried out experiments (blending time and impeller power input) confirm that the down pumping axial flow impellers exhibit better blending efficiency than the high-speed rotary impellers with prevailing radial discharge flow. It follows from presented results that, especially for large scale industrial realisations, the axial flow impellers with profiled blades bring maximum energy savings in comparison with the standard impellers with inclined flat blades (pitched blade impellers).
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34

Sato, Kyosuke, Haiyuan Wu, and Qian Chen. "High-speed and High-accuracy Scene Flow Estimation Using Kinect." Procedia Computer Science 22 (2013): 945–53. http://dx.doi.org/10.1016/j.procs.2013.09.178.

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35

Morris, Jeffrey F. "High-speed trains: in microchannels?" Journal of Fluid Mechanics 792 (March 4, 2016): 1–4. http://dx.doi.org/10.1017/jfm.2016.51.

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Kahkeshani et al. (J. Fluid Mech., vol. 786, 2016, R3) have studied particle ordering in suspension flow in a rectangular microchannel. Experiments and numerical simulations reveal that inertial focusing and hydrodynamic interactions result in long-lived ‘trains’ of regularly spaced particles. The preferred spacing is frustrated at sufficient particle concentration, an important feature for applications.
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36

OHSHIMA, Naoya, Donghyuk KANG, Kazuhiko YOKOTA, and Kotaro SATO. "Flow Characteristics of High-Speed Swirling Flow in a Circular Pipe." Proceedings of Mechanical Engineering Congress, Japan 2016 (2016): G0500804. http://dx.doi.org/10.1299/jsmemecj.2016.g0500804.

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37

KANEKO, Kenji, Akio MURAOKA, and Toshiaki SETOGUCHI. "Internal Flow Visualization of a High Specific Speed Diagonal-Flow Fan." Journal of the Visualization Society of Japan 13, Supplement1 (1993): 223–26. http://dx.doi.org/10.3154/jvs.13.supplement1_223.

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38

Petrov, M. "Flow Modellium software package for calculating high-speed compressible gas flow." Журнал вычислительной математики и математической физики 58, no. 11 (November 2018): 1932–54. http://dx.doi.org/10.31857/s004446690003544-9.

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39

Kaneko, Kenji, Akio Muraoka, Norimasa Shiomi, and Toshiaki Setoguchi. "Internal Flow of High-Specific-Speed Diagonal Flow Fan in Low Flow Range." Transactions of the Japan Society of Mechanical Engineers Series B 61, no. 591 (1995): 3836–41. http://dx.doi.org/10.1299/kikaib.61.3836.

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40

MATSUDA, Keisuke, Gunki NUKUI, Jun SAWADA, Kiyoshi HATTA, and Toshiyasu KINARI. "Air Flow Analysis around High-speed Rotating Roller." Journal of Textile Engineering 64, no. 3 (June 15, 2018): 63–69. http://dx.doi.org/10.4188/jte.64.63.

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41

KASHIMURA, Hideo, Kazuyasu MATSUO, Toshiyuki AOKI, and Youichi TAKESUE. "Computer-aided visualization of the high speed flow." JOURNAL OF THE FLOW VISUALIZATION SOCIETY OF JAPAN 7, no. 26 (1987): 269–72. http://dx.doi.org/10.3154/jvs1981.7.269.

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42

Modarress, Dariush, and Medhat Azzazy. "Modern experimental techniques for high-speed flow measurements." Journal of Aircraft 26, no. 10 (October 1989): 889–99. http://dx.doi.org/10.2514/3.45858.

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43

Nakano, Hideo, Koji Matsuda, Masafumi Yohda, Teruyuki Nagamune, Isao Endo, and Tsuneo Yamane. "High Speed Polymerase Chain Reaction in Constant Flow." Bioscience, Biotechnology, and Biochemistry 58, no. 2 (January 1994): 349–52. http://dx.doi.org/10.1271/bbb.58.349.

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44

Pellizzari, M., M. Simonutti, J. Degardin, J. A. Sahel, M. Fink, M. Paques, and M. Atlan. "High speed optical holography of retinal blood flow." Optics Letters 41, no. 15 (July 25, 2016): 3503. http://dx.doi.org/10.1364/ol.41.003503.

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45

Chen, Yong, and Wei Zhang. "Dynamic model of high speed following traffic flow." Acta Physica Sinica 69, no. 6 (2020): 064501. http://dx.doi.org/10.7498/aps.69.20191251.

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46

Znamenskaya, I. A., E. Y. Koroteeva, Y. N. Shirshov, A. M. Novinskaya, and N. N. Sysoev. "High speed imaging of a supersonic waterjet flow." Quantitative InfraRed Thermography Journal 14, no. 2 (December 9, 2016): 185–92. http://dx.doi.org/10.1080/17686733.2016.1243749.

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47

Ruleva, L. B., and S. I. Solodovnikov. "Heat flow measurements on high-speed aircraft models." IOP Conference Series: Materials Science and Engineering 927 (September 26, 2020): 012083. http://dx.doi.org/10.1088/1757-899x/927/1/012083.

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48

HADJADJ, A., and A. KUDRYAVTSEV. "Computation and flow visualization in high-speed aerodynamics." Journal of Turbulence 6 (January 2005): N16. http://dx.doi.org/10.1080/14685240500209775.

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49

Hatay, F. F., S. Biringen, G. Erlebacher, and W. E. Zorumski. "Stability of high‐speed compressible rotating Couette flow." Physics of Fluids A: Fluid Dynamics 5, no. 2 (February 1993): 393–404. http://dx.doi.org/10.1063/1.858887.

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50

Kondo, H., A. Fujisato, N. Yamaoka, S. Inoue, S. Miyamoto, F. Sato, T. Iida, et al. "High speed lithium flow experiments for IFMIF target." Journal of Nuclear Materials 329-333 (August 2004): 208–12. http://dx.doi.org/10.1016/j.jnucmat.2004.04.305.

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