WANG Zhi-liang, S. P. Lin, ZHOU Zhe-wei. Formation of Radially Expanding Liquid Sheet by Impinging Two Round Jets[J]. Applied Mathematics and Mechanics, 2010, 31(8): 891-900. doi: 10.3879/j.issn.1000-0887.2010.08.001
Citation: WANG Zhi-liang, S. P. Lin, ZHOU Zhe-wei. Formation of Radially Expanding Liquid Sheet by Impinging Two Round Jets[J]. Applied Mathematics and Mechanics, 2010, 31(8): 891-900. doi: 10.3879/j.issn.1000-0887.2010.08.001

Formation of Radially Expanding Liquid Sheet by Impinging Two Round Jets

doi: 10.3879/j.issn.1000-0887.2010.08.001
  • Received Date: 1900-01-01
  • Rev Recd Date: 2010-06-01
  • Publish Date: 2010-08-15
  • A thin circular liquid sheet can be formed by impinging two identicalround jets against each other. The liquid sheet expands to a certain critical radial distance and breaks. The unsteady process of the formation and breakup of the liquid sheet in the ambient gas was smiulated num erically. Both liquid and gas were treated as incompressible Newtonian fluids. The flow considered was axi-symm etric. The liquid-gas interface was modeled with a level set function. A finite difference scheme was used to solve the governing Navier-Stokes equations with physical boundary conditions. The numerical results show how a thin circular sheet can be formed and broken at its circular edge, in slow motion. The sheet continues to thin as it expands radially. Hence the Weber number decreases rad ially. The Weber number is defined asu2h/, where and are respectively the liquid density and the surface tension, and u and h are, respectively, the average velocity and the half sheet thickness at a local radial location in the liquid sheet. The num erical results show that the sheet indeed terminates at a radial location where the Weber num ber reaches one as observed in experiments. The spatio-tem poral linear theory predicts that the breakup is initiated by the sinuousm ode at the critical Weber number Wec=1 be low which absolute instability occurs. The other independentmode called varicose mode grow smore slowly than the sinuousmode according to the linear theory. However our numerical results show that the varicose mode actually overtakes the sinuous mode during the non linear evolution, and is respon sible for the final breakup. The linear theory predicts the nature of disturbance waves correctly only at the onset of instability, but cannotpredict the exact consequence of the instability.
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  • [1]
    Savart F. Memoire sure le choc d’une veine liquid lancee contre un plan circulair[J]. Ann Chim Phys, 1833, 54: 56-87.
    [2]
    Savart F. Suit du memoire sur le choc dune veine liquid lancee contre un plan circulaire[J]. Ann Chim Phys, 1833, 54: 113-145.
    [3]
    Savart F. Memoire sure le choc de deux veine liquids, animees de mouvemens directement opposes[J]. Ann Chim Phys, 1833, 55: 257-310.
    [4]
    Chubb D L, Calfo F D, McConley M W, McMaster M S, Afjeh A A. Geometry of thin liquid sheet flows[J]. AIAA J, 1994, 32(6): 1325-1328. doi: 10.2514/3.12139
    [5]
    Soderberg L D, Alfredsson P H. Experimental and theoretical stability investigations of plane liquid jets[J]. Eur J Mech B/Fluids, 1998, 17(5): 689-737. doi: 10.1016/S0997-7546(98)80022-8
    [6]
    Squire H B. Investigation of the instability of a moving liquid film[J]. Br J Appl Phys, 1953, 4(6): 167-169. doi: 10.1088/0508-3443/4/6/302
    [7]
    Hagerty W W, Shea J F. A study of the stability of plane fluid sheets[J]. J Appl Mech, 1955, 22(4): 509-514.
    [8]
    Fraser R P, Eisenklam P, Dombrowski N, Hasson D. Drop formation from rapidly moving liquid sheets[J]. AIChE J, 1962, 8(5): 672-680. doi: 10.1002/aic.690080522
    [9]
    Taylor G I. The dynamics of thin sheets of fluid Ⅱ: waves on fluid sheets [J]. Proc R Soc Lond, Ser A, 1959, 253: 296-312. doi: 10.1098/rspa.1959.0195
    [10]
    Taylor G I. The dynamics of thin sheets of fluid Ⅲ: disintegration of fluid sheets[J]. Proc R Soc Lond, Ser A, 1959, 253: 313-321. doi: 10.1098/rspa.1959.0196
    [11]
    Huang J C P. The break-up of axisymmetric liquid sheets[J]. J Fluid Mech, 1970, 43(2): 305-319. doi: 10.1017/S0022112070002392
    [12]
    Clanet C, Villermaux E. Life of a smooth liquid sheet[J]. J Fluid Mech, 2002, 462: 307-340.
    [13]
    Villermaux E, Clanet C. Life of a flapping liquid sheet[J]. J Fluid Mech, 2002, 462: 341-363.
    [14]
    Crapper G D, Dombrowski N, Pyott G A D. Large amplitude Kelvin-Helmholtz waves on thin liquid sheets[J]. Proc R Soc Lond, Ser A, 1975, 342: 209-224. doi: 10.1098/rspa.1975.0021
    [15]
    Clark C J, Dombrowski N. Aerodynamic instability and disintegration of inviscid liquid sheets[J]. Proc R Soc Lond, Ser A, 1972, 329: 467-478. doi: 10.1098/rspa.1972.0124
    [16]
    Crapper G D, Dombrowski N, Jepson W P. Wave growth on thin sheets of non-Newtonian liquids[J]. Proc R Soc Lond, Ser A, 1975, 342: 225-236. doi: 10.1098/rspa.1975.0022
    [17]
    Lin S P, Jiang W Y. Absolute and convective instability of a radially expanding liquid sheet[J]. Phys Fluids, 2003, 15(6): 1745-1754. doi: 10.1063/1.1570422
    [18]
    Brackbill J U, Kothe D B, Zemach C. A continuum method for modeling surface tension[J]. J Comp Phys, 1992, 100(2): 335-354. doi: 10.1016/0021-9991(92)90240-Y
    [19]
    Osher S, Sethian J A. Fronts propagating with curvature dependent speed: algorithms based on Hamilton-Jacobi formulations[J]. J Comp Phys, 1988, 79(1): 12-49. doi: 10.1016/0021-9991(88)90002-2
    [20]
    Sethian J A. Level Set Methods and Fast Marching Methods[M]. London: Cambridge University Press, 1999.
    [21]
    Sussman M, Smereka P, Osher S. A level set approach for computing solutions to incompressible 2-phase flow[J]. J Comp Phys, 1994, 114(1): 146-159. doi: 10.1006/jcph.1994.1155
    [22]
    Chorin A J. Numerical solution of the Navier-Stokes equations[J]. Math Comp, 1968, 22(104): 745-762. doi: 10.1090/S0025-5718-1968-0242392-2
    [23]
    Temam R. On an approximate solution of the Navier-Stokes equations by the method of fractional steps, part 1[J]. Archiv Ration Mech Anal, 1969, 32(2): 135-153.
    [24]
    Fortin M, Peyret R, Temam R. Résolution numérique des équations de Navier-Stokes pour un fluide visqueux incompressible[J]. J Mech, 1971,10(3): 357 -390.
    [25]
    Li J. Cacul d’interface affine par morceaux(piecewise linear interface calculation[J]. C R Acad Sci Paris, Ser ⅡB, 1995, 320(8) : 391-396.
    [26]
    Jiang G S, Shu C W. Efficient implementation of weighted ENO schemes[J]. J Comp Phys, 1996, 126(1): 202-228. doi: 10.1006/jcph.1996.0130
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