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An experimental investigation into supercavity closure mechanisms

Published online by Cambridge University Press:  19 January 2016

Ashish Karn
Affiliation:
Saint Anthony Falls Laboratory, University of Minnesota, Minneapolis, MN 55455, USA Department of Mechanical Engineering, University of Minnesota, Minneapolis, MN 55455, USA
Roger E. A. Arndt
Affiliation:
Saint Anthony Falls Laboratory, University of Minnesota, Minneapolis, MN 55455, USA Department of Civil, Environmental and Geo-Engineering, University of Minnesota, Minneapolis, MN 55455, USA
Jiarong Hong*
Affiliation:
Saint Anthony Falls Laboratory, University of Minnesota, Minneapolis, MN 55455, USA Department of Mechanical Engineering, University of Minnesota, Minneapolis, MN 55455, USA
*
Email address for correspondence: jhong@umn.edu

Abstract

Substantial discrepancy in the conditions for attainment of different closure modes of a ventilated supercavity has existed widely in the published literature. In this study, supercavity closure is investigated with an objective to understand the physical mechanisms determining closure formation and transition between different closure modes and to reconcile the observations from prior studies under various flow settings. The experiments are conducted in a closed-wall recirculating water tunnel to image ventilated supercavity closure using high speed and high-resolution photography and simultaneously measure pressure inside the cavity. The flow conditions are varied systematically to cover a broad range of water velocity, ventilation flow rate and cavitator size, which correspond to different Froude numbers, air entrainment coefficients and blockage ratios, respectively. In addition to the classical closure modes reported in the literature (e.g. re-entrant jet, twin vortex, quad vortex, etc.), the study has revealed a number of new closure modes that occur during the transition between classical modes, or under very specific flow conditions. Closure maps are constructed to depict the flow regimes, i.e. the range of Froude number and air entrainment coefficient, for various closure modes at different blockage ratios. From the closure map at each blockage ratio, a critical ventilation flow rate, below which the supercavity collapses into foamy cavity upon reduction of Froude number, is identified. The air entrainment coefficients corresponding to such critical ventilation rate are found to be independent of blockage ratio. It has been observed that in the process of generating a supercavity by increasing ventilation flow rate, the cavitation number gradually reduces to a minimum value and stays fixed upon further increments in the ventilation rate. Once a supercavity is formed, the ventilation rate can be decreased to a much lower value with no change in cavitation number while still maintaining a supercavity. This process is accompanied by a change in closure modes, which generally goes from twin vortex, to quad vortex, and then to re-entrant jet. In addition, the blockage effect is shown to play an important role in promoting the occurrence of twin-vortex closure modes. Subsequently, a physical framework governing the variation of different closure modes is proposed, and is used to explain mode transition upon the change of flow conditions, including the blockage effect. This framework is further extended to shed light on the occurrence of closure modes for ventilated supercavitation experiments across different types of flow facilities, the natural supercavity closure and the pulsating supercavity reported in the literature. Finally, in combination with a recent numerical study, our research discusses the role of the internal flow physics on the observed features during supercavity formation and closure-mode transition, paving the way for future investigations in this direction.

Type
Papers
Copyright
© 2016 Cambridge University Press 

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References

Ahn, B. K., Kim, J., Jun, Y., Kim, H. & Lee, C. 2013 Experimental and numerical study of natural supercavitating flows. In Proceedings of the PRADS2013, CECO, Changwon City, Korea.Google Scholar
Buyvol, V. N. 1980 Slender Cavities in Flows With Perturbations, Nauvoka Dunka; (in Russian).Google Scholar
Callenaere, M., Franc, J., Michel, J. & Riondet, M. 2001 The cavitation instability induced by the development of a re-entrant jet. J. Fluid Mech. 444, 223256.Google Scholar
Cox, R. & Clayden, W. 1956 Air entrainment at the rear of a steady cavity. In Proceedings of the Symposium on Cavitation in Hydrodynamics, London.Google Scholar
Epshtein, L. 1973 Characteristics of ventilated cavities and some scale effects. In Proceedings of the International Symposium IUTAM, Unsteady Water Flow with High Velocities, pp. 173185. Nauka.Google Scholar
Gadd, G. & Grant, S. 1965 Some experiments on cavities behind disks. J. Fluid Mech. 23 (4), 645656.Google Scholar
Gopalan, S. & Katz, J. 2000 Flow structure and modeling issues in the closure region of attached cavitation. Phys. Fluids 12 (4), 895911.CrossRefGoogle Scholar
Campbell, I. J. & Hilborne, D.V. 1958 Air entrainment behind artificially inflated cavity. In Proceedings of the Second Symposium on Naval Hydrodynamics, Washington.Google Scholar
Hrubes, J. 2001 High-speed imaging of supercavitating underwater projectiles. Exp. Fluids 30 (1), 5764.Google Scholar
Kapankin, Y. N. & Gusev, A. V. 1984 Experimental research of joint influence of fluid and lift power of cavitator on character of flow in cavity rear part and gas departure from it. Proc. CAHI 2244, 1928.Google Scholar
Karlikov, V., Reznichenko, N., Khomyakov, A. & Sholomovich, G. 1987 A possible mechanism for the emergence of auto-oscillations in developed artificial cavitation flows and immersed gas jets. Fluid Dyn. 22 (3), 392398.Google Scholar
Karlikov, V. & Sholomovich, G. 1966 Method of approximate account for the wall effect in cavitation flow around bodies in water tunnels. Fluid Dyn. 1 (4), 6164.Google Scholar
Karn, A., Arndt, R. E. A. & Hong, J. 2015a Dependence of Supercavity closure upon flow unsteadiness. Exp. Therm. Fluid Sci. 68, 493498.CrossRefGoogle Scholar
Karn, A., Monson, G., Ellis, C., Hong, J., Arndt, R. & Gulliver, J. 2015b Mass transfer studies across ventilated hydrofoils: A step towards hydroturbine aeration. Intl J. Heat Mass Transfer 87, 512520.Google Scholar
Kinzel, M. P., Lindau, J. W. & Kunz, R. F. 2009 Air entrainment mechanisms from artificial supercavities: insight based on numerical simulations. In Proceedings of the 7th International Symposium on Cavitation, CAV 2009, Ann Arbor, vol. 136.Google Scholar
Kawakami, E.2010 Investigation of the behavior of ventilated supercavities, MS Thesis, University of Minnesota, Twin cities.CrossRefGoogle Scholar
Kawakami, E. & Arndt, R. E. A. 2011 Investigation of the behavior of ventilated supercavities. J. Fluid Engng 133 (9), 091305,1–11.Google Scholar
Kshatriya, S., Patwardhan, A. & Eaglesham, A. 2007 Experimental studies of ventilated cavities in a channel. Chem. Engng Sci. 62 (4), 979989.CrossRefGoogle Scholar
Kuklinski, R., Castano, J. & Henoch, C. 2001 Experimental study of ventilated cavities on dynamic test model. In CAV 2001: Fourth International Symposium on Cavitation. Naval Undersa Weapons Center, Newport, RI.Google Scholar
Logvinovich, G. V. 1973 Hydrodynamics of Free-Boundary Flows. Halsted Press.Google Scholar
Michel, J. 1984 Some features of water flows with ventilated cavities. Trans. ASME J. Fluids Engng 106 (3), 319326.Google Scholar
Nesteruk, I. 2014 Shape of slender axisymmetric ventilated supercavities. J. Comput. Engng 2014, 501590,1–18.Google Scholar
Paryshev, E. 2003 Mathematical modelling of unsteady cavity flows. In Proceedings of Fifth International Symposium on Cavitation (CAV 2003), Osaka, Japan, pp. 118.Google Scholar
Peng, X., Wang, Z., Pan, S. & Yan, K. 2006 Generation mechanism of ventilated supercavitation in an axisymmetric body with cavitator. In Proceedings of Sixth International Symposium on Cavitation, CAV2006, Wageningen, Netherlands.Google Scholar
Pan, Z., Lu, C., Chen, Y. & Hu, S. 2010 Numerical study of periodically forced-pitching of a supercavitating vehicle. In Proceedings of Ninth International Conference on Hydrodynamics, Shanghai, China.Google Scholar
Savchenko, Y. 2001 Supercavitation-problems and perspectives. In Fourth International Symposium on Cavitation. California Institute of Technology Pasadena, California, vol. 200.Google Scholar
Semenenko, V. N. 2001a Artificial Supercavitation: Physics and Calculation. Ukrainian Academy of Sciences, Kiev Inst of Hydromechanics.Google Scholar
Semenenko, V. N. 2001b Dynamic Processes of Supercavitation and Computer Simulation. Ukrainian Academy of Sciences, Kiev Inst of Gydromechanics.Google Scholar
Shi, H., Itoh, M. & Takami, T. 2000 Optical observation of the supercavitation induced by high-speed water entry. Trans. ASME J. Fluids Engng 122 (4), 806810.Google Scholar
Silberman, E. & Song, C. S. 1961 Instability of ventilated cavities. J. Ship. Res. 5 (1), 1333.CrossRefGoogle Scholar
Skidmore, G.2013 The pulsation of ventilated supercavities, Master of Science thesis, Department of Aerospace Engineering, Pennsylvania State University.Google Scholar
Skidmore, G., Brungart, T. A., Lindau, J. W. & Moeny, M. J. 2015 Noise generated by ventilated supercavities. Noise Control Engr. J. 63 (1), 94101.Google Scholar
Song, C. S.1961 Pulsation of ventilated cavities. (No. 32 B). Saint Anthony Falls Laboratory, University of Minnesota.Google Scholar
Spurk, J. & König, B. 2002 On the gas loss from ventilated supercavities. Acta Mech. 155, 125135.Google Scholar
Stinebring, D. R., Billet, M. L., Lindau, J. W. & Kunz, R. F.2001 Developed cavitation-cavity dynamics, DTIC Document.Google Scholar
Tulin, M. P.1964 Supercavitating propellers, momentum theory. (No. TR-121-4). Hydronautics Inc. Laurel MD: DTIC Document.Google Scholar
Vlasenko, Y. D. 2003 Experimental investigation of supercavitation flow regimes at subsonic and transonic speeds. In Fifth International Symposium on Cavitation, Osaka, Japan.Google Scholar
Wu, T., Whitney, A. K. & Brennen, C. 1971 Cavity-flow wall effects and correction rules. J. Fluid Mech. 49 (2), 223256.Google Scholar
Wu, T. 1972 Cavity and wake flows. Annu. Rev. Fluid Mech. 4, 243284.Google Scholar
Zhang, X., Wei, Y., Zhang, J., Wang, C. & Yu, K. 2007 Experimental research on the shape characters of natural and ventilated supercavitation. J. Hydrodyn. B 19 (5), 564571.CrossRefGoogle Scholar
Zhou, J., Yu, K., Min, J. & Yang, M. 2010 The comparative study of ventilated super cavity shape in water tunnel and infinite flow field. J. Hydrodyn. B 22 (5), 689696.Google Scholar

Karn et al. supplementary movie

A side view of the re-entrant jet closure mechanism. Note how the liquid outside the cavity closure gushes into the cavity and the air is entrained out of the cavity in the form of toroidal vortices.

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Video 785.3 KB

Karn et al. supplementary movie

A bottom view of the re-entrant jet closure mechanism. Note how the liquid outside the cavity closure gushes into the cavity and the air is entrained out of the cavity in the form of toroidal vortices.

Download Karn et al. supplementary movie(Video)
Video 2.1 MB

Karn et al. supplementary movie

A side view of the twin vortex closure mechanism. The individual vortices can be seen more clearly in the bottom view.

Download Karn et al. supplementary movie(Video)
Video 110.5 KB

Karn et al. supplementary movie

A bottom view of the twin vortex closure mechanism. Note that the re-circulation of the two vortices are in the opposite direction.

Download Karn et al. supplementary movie(Video)
Video 2.6 MB

Karn et al. supplementary movie

A side view of the quad-vortex closure mechanism. The viewing angle is at an angle to the normal to show the four vortices. Both the front and rear bottom vortex have a vortex lying above it.

Download Karn et al. supplementary movie(Video)
Video 1 MB

Karn et al. supplementary movie

A side view of the hybrid quad-vortex - re-entrant jet closure mechanism. The two pairs of vortices can be seen along with the liquid gushing into the cavity. The lower pair of vortices are more stable compared to the upper pair.

Download Karn et al. supplementary movie(Video)
Video 4.7 MB

Karn et al. supplementary movie

A side view of the unstable/hybrid twin vortex - quad vortex closure mechanism. Note that in this unstable mode, one to three vortices might intermittently disappear. The lower pair of vortices are more stable compared to the upper pair.

Download Karn et al. supplementary movie(Video)
Video 7.5 MB

Karn et al. supplementary movie

A side view of the hybrid twin vortex - re-entrant jet closure mechanism. Along with the two vortices, liquid gushing into the cavity can be seen as well.

Download Karn et al. supplementary movie(Video)
Video 3.5 MB

Karn et al. supplementary movie

A side view of the interacting vortex closure mechanism. It can be clearly seen that the two vortices interact with each other to form one single thick vortex at the closure.

Download Karn et al. supplementary movie(Video)
Video 1.5 MB