A thin circular liquid sheet can be formed by impinging two identical round 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 is simulated numerically. Both liquid and gas are treated as incompressible Newtonian fluids. The flow considered is axisymmetric. The liquid-gas interface is modeled with a level set function. A finite difference scheme is 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 break at its circular edge in slow motion. The sheet continues to thin as it expands radially. Hence, the Weber number decreases radially. The Weber number is defined as ρu 2 h/σ, where ρ and σ 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 numerical results show that the sheet indeed terminates at a radial location, where the Weber number reaches one as observed in experiments. The spatio-temporal linear theory predicts that the breakup is initiated by the sinuous mode at the critical Weber number We c =1, below which the absolute instability occurs. The other independent mode called the varicose mode grows more slowly than the sinuous mode according to the linear theory. However, our numerical results show that the varicose mode actually overtakes the sinuous mode during the nonlinear evolution, and is responsible for the final breakup. The linear theory predicts the nature of disturbance waves correctly only at the onset of the instability, but cannot predict the exact consequence of the instability.
By numerical simulation of basic flow,this paper extends Floquet stability analysis of interfacial flow with periodic fluctuation into large density ratio range.Stability of a liquid aluminum jet in a coaxial nitrogen stream with velocity fluctuation is investigated by Chebyshev collocation method and the Floquet theory.Parametric resonance of the jet and the influences of different physical parameters on the instability are discussed.The results show qualitative agreement with the available experimental data.
Molecular dynamics simulation is applied to study the instability and rupture process of ultra-thin water films on a solid substrate.Results show the small disturbance of the film will develop linearly due to the spinodal instability,whereas the interaction between solid and liquid has less influences on the initial growth.Then the rupture occurs and the rim recedes with a dynamic contact angle.The radius of the rim varies with time as the square root of t,which is consistent with the macroscopic theory available. Stronger interaction between solid and liquid will postpone rupture time,decline the dynamic contact angle and raise the density of water near the interface between solid and liquid.
