[1] Savart, F., Ann. Chim. Phys., 53, 337 (1833).
[2] Rayleigh, W.S. (Lord), "On the instability of jets", Proc.London Math. Soc., 4, 10
(1879).
[3] Brenner, M.P., Lister, J., Stone, H.A., "Pinching threads,singularities and the number
0.0304...", Phys. Fluids, 8(11), 2827 (1996).
[4] Brenner, M.P., Eggers, J., Joseph, K., Nagel, S.R., Shi,X.D., "Breakdown of scaling in
droplet fission at high Reynolds number", Phys. Fluids, 9 (6), 1573 (1997).
[5] Almgren, R., Bertozzi, A., Brenner, M.P., "Stable and unstable singularities in the
unforced Hele-Shaw cell", Phys.Fluids, 8 (6), 1356 (1996).
[6] Nagi, N.M., Thomas, S.L., "Satellite formation in capillary jet breakup", Phys. Fluids,
A 2 (7). 1141 (1990).
[7] Lafrance, P., "Nonlinear breakup of a laminar liquid jet",The Phys. Fluids, 18 (4), 428
(1975).
[8] Rutland, D.F., Jameson, G.J., "Theoretical prediction of the sizes of drops formed in
the breakup of capillary jets",Chem. Eng. Sci., 25, 1689 (1970).
[9] Hirt, C.W., Nichols, B.D., Romero. N.C., "SOLA-A numerical solution algorithm for
transient fluid flows", Los Alamos Scientific Lab. Rep., LA-5852 (1975).
[10] Welch, J.E., Harlow, F.H., Shannon, J.P., Daly, B.J., "The MAC method. A computing
technique for solving viscous,incompressible, transient fluid-flow problems involving free
surfaces", Los Alamos Scientific Lab. Rep., LA-3425, Los Alamos, NM (1965).
[11] Hirt, C.W., Nichols, B.D., "Volume of fluid (VOF) method for the dynamics of free
boundaries", J. Comp. Phys., 39,201 (1981).
[12] Rudman, M., "Volume-tracking methods for interfacial flow calculations", Int. J.
Numer. Methods Fluids, 24, 671(1997).
[13] Chang, H.C., Demekhin, E. A., Kalaidin, E., "Iterated stretching of viscoelastic
jets", Phys. Fluids, 11 (7), 1717(1999).
[14] Yang, C., Mao, Z.S., "An improved level set approach to the simulation of drop and
bubble motion", Chinese J. Chem.Eng., 10 (3), 263 (2002).
[15] Zhou, L.X., Yang, M., Lian, C.Y., Fan, L.S., Lee, D.J.,"Comparison of a full second-
order moment model and an algebraic stress two-phase turbulence model for simulating
bubble-liquid flows in a bubble column", Chinese J. Chem.Eng., 10 (2), 142-148 (2002).
[16] Kothe, D.B., Mjolsness, R.C., Torrey, M.D., "RIPPLE: A computer program for
incompressible flow with free surfaces", Los Alamos National Lab Rep., LA-12007-MS (1991).
[17] Brackbill, J.U., Kothe, D.B., Zemach, C., "A continuum method for modeling surface
tension", J. Comp. Phys.,100, 335-354 (1992).
[18] Rider, W.J., Kothe, D.B., "Reconstructing volume tracking", Los Alamos National Lab.
Rep., LA-UR-96-2375(1996).
[19] Hong, R.Y., Li, H.Z., Cheng, M.Y., Zhang, J.Y., "Numerical simulation and verification
of a gas-solid jet fluidized bed", Powder Tech., 87 (1), 73 (1996).
[20] Hong, R.Y., Guo, Q.J., Luo, G.H., Zhang, J.Y., Ding, J.,"On the jet penetration height
in fiuidized beds with two vertical jets", Powder Tech., 133 (L), 68 (2003).
[21] Harlow, H.F., Amsden, A.A., "Numerical calculation of multiphase flow", J. Comp.
Phys., 17, 19 (1975).
[22] Spalding, D.B., "Developments in the IPSA procedure for numerical computation of
multi-phase-flow phenomena with interphase slip, unequal temperature, etc.", In:
Proceedings of the 2nd National Symp. on Numerical Properties and Methodologies in Heat
Transfer, Shih, T.M., Hemisphere, N. Y., Eds., New York, 421-436 (1983).
[23] van Leer, B., "Towards the ultimate conservative difference scheme", J. Comp. Phys.,
32, 101 (1979).
[24] Hirt, C.W., "Heuristic stability theory for finite-difference equation", J. Comp.
Phys., 2, 339 (1968).
[25] Youngs, D.L., "Time-dependent mlti-material flow with large fluid distortion", In:
Numerical Methods for Fluid Dynamics, Morton, K.W., Baines, M.J., Eds., Academic Press, New
York, 273-285 (1982).
[26] Fluent Inc., Fluent Version 5.5, Users’ Guide, Centerra Resource Park, 10 Cavendish
Court, Lebanon, NH 03766, USA (2001). |
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